Holography: Difference between revisions
Louis Knee (talk | contribs) m Undid revision 1263755131 by Brijeshl880 (talk) Revert vandalism/advertising |
|||
Line 1: | Line 1: | ||
{{Short description|Recording to reproduce a three-dimensional light field}} |
|||
{{Other uses}} |
{{Other uses}} |
||
{{Distinguish|Pepper's ghost}} |
|||
{{For|the documentary authorship|Holograph}} |
|||
{{Use dmy dates|date=June 2020}} |
|||
[[File:Holomouse2.jpg|thumb|Two photographs of a single hologram taken from different viewpoints]] |
[[File:Holomouse2.jpg|thumb|Two photographs of a single hologram taken from different viewpoints]] |
||
'''Holography''' is a technique that enables a [[wavefront]] to be recorded and later reconstructed. It is best known as a method of generating [[three-dimensional images]], and has a wide range of other uses, including data storage, microscopy, and interferometry. In principle, it is possible to make a hologram for any type of [[Holography#Non-optical holography|wave]]. |
|||
'''Holography''' (from the [[Greek language|Greek]] ὅλος ''hólos'', "whole" + γραφή ''[[-graphy|grafē]]'', "[[writing]], [[drawing]]") is a technique that allows the [[light]] scattered from an object to be recorded and later reconstructed so that when an imaging system (a camera or an eye) is placed in the reconstructed beam, an image of the object will be seen even when the object is no longer present. The image changes as the position and orientation of the viewing system changes in exactly the same way as if the object were still present, thus making the image appear [[Three-dimensional space|three-dimensional]]. |
|||
A '''hologram''' is a recording of an [[Wave interference|interference]] pattern that can reproduce a 3D [[light field]] using [[diffraction]]. In general usage, a hologram is a recording of any type of wavefront in the form of an interference pattern. It can be created by capturing [[light]] from a real scene, or it can be generated by a computer, in which case it is known as a [[computer-generated hologram]], which can show virtual objects or scenes. Optical holography needs a [[laser]] light to record the light field. The reproduced light field can generate an image that has the depth and [[parallax]] of the original scene.<ref>{{Cite web |url=http://holocenter.org/what-is-holography |title=What is Holography? {{!}} holocenter |language=en-US |access-date=2019-09-02}}</ref> A hologram is usually unintelligible when viewed under [[Diffuse reflection|diffuse ambient light]]. When suitably lit, the interference pattern diffracts the light into an accurate reproduction of the original light field, and the objects that were in it exhibit visual [[Depth perception|depth cues]] such as [[parallax]] and [[perspective (visual)|perspective]] that change realistically with the different angles of viewing. That is, the view of the image from different angles shows the subject viewed from similar angles. |
|||
The holographic recording itself is not an image; it consists of an apparently random structure of either varying intensity, density or profile. |
|||
A hologram is traditionally generated by overlaying a second wavefront, known as the reference beam, onto a wavefront of interest. This generates an interference pattern, which is then captured on a physical medium. When the recorded interference pattern is later illuminated by the second wavefront, it is diffracted to recreate the original wavefront.<ref name=Jesacher>{{Cite journal |last1=Jesacher |first1=Alexander |last2=Ritsch-Marte |first2=Monika |date=2016-01-02 |title=Synthetic holography in microscopy: opportunities arising from advanced wavefront shaping |url=http://www.tandfonline.com/doi/full/10.1080/00107514.2015.1120007 |journal=Contemporary Physics |language=en |volume=57 |issue=1 |pages=46–59 |doi=10.1080/00107514.2015.1120007 |bibcode=2016ConPh..57...46J |issn=0010-7514}}</ref> The 3D image from a hologram can often be viewed with non-laser light. However, in common practice, major image quality compromises are made to remove the need for laser illumination to view the hologram. |
|||
==Overview and history== |
|||
The [[Magyars|Hungarian]]-[[British people|British]] physicist [[Dennis Gabor]] (Hungarian name: Gábor Dénes),<ref>[[Dennis Gabor|Gabor, Dennis]]. (1948), A new microscopic principle, ''Nature'', 161, p 777-8</ref><ref>{{Cite journal|doi = 10.1098/rspa.1949.0075|first = Dennis|last = Gabor|year = 1949|title = Microscopy by reconstructed wavefronts|journal = Proceedings of the Royal Society|location = London|volume = 197|pages = 454–487|issue = 1051|postscript = <!--None-->|bibcode = 1949RSPSA.197..454G }}</ref> was awarded the [[Nobel Prize in Physics]] in 1971 "for his invention and development of the holographic method".<ref>{{cite web|url=http://www.nobelprize.org/nobel_prizes/physics/laureates/1971/ |title=The Nobel Prize in Physics 1971 |publisher=Nobelprize.org |date= |accessdate=2012-04-21}}</ref> |
|||
His work, done in the late 1940s, built on pioneering work in the field of X-ray microscopy by other scientists including [[Mieczysław Wolfke]] in 1920 and [[William Lawrence Bragg|WL Bragg]] in 1939.<ref>Hariharan, (1996), Section 1.2, p4-5</ref> The discovery was an unexpected result of research into improving [[electron microscope]]s at the [[British Thomson-Houston]] Company in [[Rugby, Warwickshire|Rugby]], England, and the company filed a patent in December 1947 (patent GB685286). The technique as originally invented is still used in [[electron microscopy]], where it is known as [[electron holography]], but optical holography did not really advance until the development of the [[laser]] in 1960. |
|||
[[File:Portrait of Yuri Denisyuk.jpg|thumb|upright|Portrait of Yuri Denisyuk, by [[Dieter Jung (artist)|Dieter Jung]]]] |
|||
The development of the [[laser]] enabled the first practical optical holograms that recorded 3D objects to be made in 1962 by [[Yuri Denisyuk]] in the Soviet Union<ref name="denisyuk">{{Cite journal |
|||
| title = On the reflection of optical properties of an object in a wave field of light scattered by it |
|||
| last = Denisyuk |
|||
| first = Yuri N. |
|||
| authorlink = Yuri Denisyuk |
|||
| coauthors= |
|||
| journal = [[Doklady Akademii Nauk SSSR]] |
|||
| volume = 144 |
|||
| pages = 1275–1278 |
|||
| year = 1962 |
|||
| month = |
|||
| url = |
|||
| doi = |
|||
| publisher = |
|||
| issue = 6 |
|||
}}</ref> and by [[Emmett Leith]] and Juris Upatnieks at [[University of Michigan]], USA.<ref name="leith">{{Cite journal |
|||
| title = Reconstructed wavefronts and communication theory |
|||
| author = Leith, E.N. |
|||
| coauthors= Upatnieks, J. |
|||
| journal = J. Opt. Soc. Am. |
|||
| volume = 52 |
|||
| pages = 1123–1130 |
|||
| year = 1962 |
|||
| month = |
|||
| url = |
|||
| doi =10.1364/JOSA.52.001123| publisher = |
|||
| issue = 10 |
|||
}}</ref> Early holograms used [[silver halide]] photographic emulsions as the recording medium. They were not very efficient as the grating produced absorbed much of the incident light. Various methods of converting the variation in transmission to a variation in refractive index (known as "bleaching") were developed which enabled much more efficient holograms to be produced.<ref>Upatniek J & Leaonard C., (1969), "Diffraction efficiency of bleached photographically recorded intereference patterns", Applied Optics, 8, p85-89</ref><ref>Graube A, (1974), "Advances in bleaching methods for photographically recorded holograms", Applied Optics, 13, p2942-6</ref><ref>N. J. Phillips and D. Porter, (1976), "An advance in the processing of holograms," Journal of Physics E: Scientific Instruments p. 631</ref> |
|||
A computer-generated hologram is created by digitally modeling and combining two wavefronts to generate an interference pattern image. This image can then be printed onto a mask or film and illuminated with an appropriate light source to reconstruct the desired wavefront.<ref name=Jesacher /> Alternatively, the interference pattern image can be directly displayed on a dynamic holographic display.<ref>{{Cite journal |last1=Sahin |first1=Erdem |last2=Stoykova |first2=Elena |last3=Mäkinen |first3=Jani |last4=Gotchev |first4=Atanas |date=2020-03-20 |title=Computer-Generated Holograms for 3D Imaging: A Survey |url=https://trepo.tuni.fi//bitstream/handle/10024/127486/ACM_CSUR_Sahin_revised_submitted.pdf |journal=ACM Computing Surveys |volume=53 |issue=2 |pages=32:1–32:35 |doi=10.1145/3378444 |issn=0360-0300}}</ref> |
|||
Several types of holograms can be made. Transmission holograms, such as those produced by Leith and Upatnieks, are viewed by shining laser light through them and looking at the reconstructed image from the side of the hologram opposite the source.<ref>Hariharan, (2002), Section 7.1, p 60</ref> A later refinement, the [[rainbow hologram|"rainbow transmission" hologram]], allows more convenient illumination by white light rather than by lasers.<ref name = Benton>Benton S.A, (1977), "White light transmission/reflection holography" in Applications of Holography and Optical Data Processing, ed. E. Marom et al, ps 401-9, Pregamon press, Oxford</ref> Rainbow holograms are commonly seen today on credit cards as a security feature and on product packaging.<sup>[citation needed]</sup> |
|||
Holographic portraiture often resorts to a non-holographic intermediate imaging procedure, to avoid the dangerous high-powered [[Laser#Pulsed operation|pulsed lasers]] which would be needed to optically "freeze" moving subjects as perfectly as the extremely motion-intolerant holographic recording process requires. Early holography required high-power and expensive lasers. Currently, mass-produced low-cost [[laser diode]]s, such as those found on [[DVD recorder]]s and used in other common applications, can be used to make holograms. They have made holography much more accessible to low-budget researchers, artists, and dedicated hobbyists. |
|||
Another kind of common hologram, the [[#The efficiency of a hologram|reflection]] or Denisyuk hologram, can also be viewed using a white-light illumination source on the same side of the hologram as the viewer and is the type of hologram normally seen in holographic displays. They are also capable of multicolour-image reproduction.<ref>Hariharan, (2002), Section 7.2, p61</ref> |
|||
Most holograms produced are of static objects, but systems for displaying changing scenes on dynamic holographic displays are now being developed.<ref>{{cite journal |last1 = Blanche |first1 = P.-A. |year =2010 |title = Holographic three-dimensional telepresence using large-area photorefractive polymer |journal = Nature |volume = 468 |issue = 7320 |pages = 80–83 |doi=10.1038/nature09521 |last2 = Bablumian |first2 = A. |last3 = Voorakaranam |first3 = R. |last4 = Christenson |first4 = C. |last5 = Lin |first5 = W. |last6 = Gu |first6 = T. |last7 = Flores |first7 = D. |last8 = Wang |first8 = P. |last9 = Hsieh |first9 = W.-Y. |last10 = Kathaperumal |first10 = M. |last11 = Rachwal |first11 = B. |last12 = Siddiqui |first12 = O. |last13 = Thomas |first13 = J. |last14 = Norwood |first14 = R. A. |last15 = Yamamoto |first15 = M. |last16 = Peyghambarian |first16 = N. |pmid = 21048763 |bibcode = 2010Natur.468...80B |s2cid = 205222841 |display-authors = 8 }}</ref><ref>{{Cite journal |last1=Smalley |first1=D. E. |last2=Nygaard |first2=E. |last3=Squire |first3=K. |last4=Van Wagoner |first4=J. |last5=Rasmussen |first5=J. |last6=Gneiting |first6=S. |last7=Qaderi |first7=K. |last8=Goodsell |first8=J. |last9=Rogers |first9=W. |last10=Lindsey |first10=M. |last11=Costner |first11=K. |last12=Monk |first12=A. |last13=Pearson |first13=M. |last14=Haymore |first14=B. |last15=Peatross |first15=J. |date=2018-01-25 |title=A photophoretic-trap volumetric display |journal=Nature |language=en |volume=553 |issue=7689 |pages=486–490 |doi=10.1038/nature25176 |pmid=29368704 |bibcode=2018Natur.553..486S |s2cid=4451867 |issn=1476-4687|doi-access=free }}</ref> |
|||
[[Specular holography]] is a related technique for making three-dimensional images by controlling the motion of specularities on a two-dimensional surface.<ref>{{cite web|url=http://www.zintaglio.com/how.html |title=specular holography: how |publisher=Zintaglio.com |date= |accessdate=2012-04-21}}</ref> It works by reflectively or refractively manipulating bundles of light rays, whereas Gabor-style holography works by diffractively reconstructing wavefronts. |
|||
The word ''holography'' comes from the [[Greek language|Greek]] words {{lang|grc|ὅλος}} (''holos''; "whole") and {{lang|grc|γραφή}} (''[[-graphy|graphē]]''; "[[writing]]" or "[[drawing]]"). |
|||
Most holograms produced are of static objects but systems for displaying changing scenes on a holographic [[volumetric display]] are now being developed.<ref>{{cite web|url=http://www.tgdaily.com/hardware-features/53703-mit-unveils-holographic-tv-system?utm_source=feedburner&utm_medium=feed&utm_campaign=Feed%3A+tgdaily_all_sections+%28TG+Daily+-+All+News%29|title=MIT unveils holographic TV system|accessdate = 14/09/2011}}</ref><ref>See [[Zebra imaging]].</ref><ref>{{cite journal | last1 = Blanche | first1 = P.-A. | year =2010 | title = Holographic three-dimensional telepresence using large-area photorefractive polymer | url =http://www.nature.com/nature/journal/v468/n7320/full/nature09521.html | journal = Nature | volume = 468 | issue = 7320| pages = 80–83 | doi=10.1038/nature09521 | last2 = Bablumian | first2 = A. | last3 = Voorakaranam | first3 = R. | last4 = Christenson | first4 = C. | last5 = Lin | first5 = W. | last6 = Gu | first6 = T. | last7 = Flores | first7 = D. | last8 = Wang | first8 = P. | last9 = Hsieh | first9 = W.-Y. | pmid = 21048763|bibcode = 2010Natur.468...80B }}</ref> |
|||
==History== |
|||
Holograms can also be used to store, retrieve, and process information optically.<ref>Hariharan, (2002), 12.6, p107</ref> |
|||
[[File:IntroductionToHolography1972.ogv|thumb|thumbtime=40|''Introduction to Holography'' (1972 educational film)]] |
|||
The [[Magyars|Hungarian]]-[[British people|British]] physicist [[Dennis Gabor]] invented holography in 1948 while he was looking for a way to improve [[image resolution]] in [[electron microscope]]s.<ref>{{cite journal |last1 = Gabor |first1 = Dennis |author-link = Dennis Gabor |year = 1948 |title = A new microscopic principle |journal = Nature |volume = 161 |issue = 4098 |pages = 777–8 |doi=10.1038/161777a0 |bibcode = 1948Natur.161..777G |pmid=18860291 |s2cid = 4121017 |doi-access = free }}</ref><ref>{{Cite journal |doi = 10.1098/rspa.1949.0075 |first = Dennis |last = Gabor |year = 1949 |title = Microscopy by reconstructed wavefronts |journal = Proceedings of the Royal Society |volume = 197 |pages = 454–487 |issue = 1051 |bibcode = 1949RSPSA.197..454G |s2cid = 123187722 |doi-access = free}}</ref><ref name=FieldGuideHistory>{{Cite book |last=Blanche |first=Pierre-Alexandre |title=Field guide to holography |date=2014 |publisher=SPIE Press |isbn=978-0-8194-9957-8 |series=SPIE field guides |location=Bellingham, Wash|page=1}}</ref> Gabor's work was built on pioneering work in the field of [[X-ray microscopy]] by other scientists including [[Mieczysław Wolfke]] in 1920 and [[William Lawrence Bragg]] in 1939.<ref name="Hariharan 1996">{{cite book |last1=Hariharan |first1=P. |title=Optical Holography |date=1996 |publisher=Cambridge University Press |location=Cambridge |isbn=9780521433488}}</ref> The formulation of holography was an unexpected result of Gabor's research into improving electron microscopes at the [[British Thomson-Houston]] Company (BTH) in [[Rugby, Warwickshire|Rugby]], England, and the company filed a [[patent]] in December 1947 (patent GB685286). The technique as originally invented is still used in electron microscopy, where it is known as [[electron holography]]. Gabor was awarded the [[Nobel Prize in Physics]] in 1971 "for his invention and development of the holographic method".<ref>{{cite web |url=https://www.nobelprize.org/nobel_prizes/physics/laureates/1971/ |title=The Nobel Prize in Physics 1971 |publisher=Nobelprize.org |access-date=2012-04-21}}</ref> |
|||
[[File:III-BIBI BEI BOB.jpg|thumb|Horizontal symmetric text, by [[Dieter Jung (artist)|Dieter Jung]]]] |
|||
In its early days, holography required high-power expensive lasers, but nowadays, mass-produced low-cost semi-conductor or [[LED]] [[laser]]s, such as those found in millions of [[DVD recorder]]s and used in other common applications, can be used to make holograms and have made holography much more accessible to low-budget researchers, artists and dedicated hobbyists. |
|||
Optical holography did not really advance until the development of the [[laser]] in 1960. The development of the laser enabled the first practical optical holograms that recorded 3D objects to be made in 1962 by [[Yuri Denisyuk]] in the Soviet Union<ref name="denisyuk">{{Cite journal |title = On the reflection of optical properties of an object in a wave field of light scattered by it |last = Denisyuk |first = Yuri N. |author-link = Yuri Denisyuk|journal = [[Doklady Akademii Nauk SSSR]] |volume = 144|pages = 1275–1278|year = 1962|issue = 6}}</ref> and by [[Emmett Leith]] and [[Juris Upatnieks]] at the [[University of Michigan]], US.<ref name="leith">{{Cite journal |title = Reconstructed wavefronts and communication theory|author = Leith, E.N.|author2=Upatnieks, J.|journal = J. Opt. Soc. Am. |volume = 52|pages = 1123–1130|year = 1962|doi =10.1364/JOSA.52.001123| issue = 10|bibcode = 1962JOSA...52.1123L}}</ref> |
|||
Early optical holograms used [[silver halide]] photographic emulsions as the recording medium. They were not very efficient as the produced [[diffraction grating]] absorbed much of the incident light. Various methods of converting the variation in transmission to a variation in refractive index (known as "bleaching") were developed which enabled much more efficient holograms to be produced.<ref>{{cite journal |last1 = Upatnieks |first1 = J |last2 = Leonard |first2 = C |year = 1969 |title = Diffraction efficiency of bleached, photographically recorded interference patterns |journal = Applied Optics |volume = 8 |issue = 1 |pages = 85–89 |doi = 10.1364/ao.8.000085 |pmid = 20072177 |bibcode = 1969ApOpt...8...85U }}</ref><ref>{{cite journal |last1 = Graube |first1 = A |year = 1974 |title = Advances in bleaching methods for photographically recorded holograms |journal = Applied Optics |volume = 13 |issue = 12 |pages = 2942–6 |doi = 10.1364/ao.13.002942 |pmid = 20134813 |bibcode = 1974ApOpt..13.2942G }}</ref><ref>{{cite journal |last1 = Phillips |first1 = N. J. |last2 = Porter |first2 = D. |year = 1976 |title = An advance in the processing of holograms |journal = Journal of Physics E: Scientific Instruments |volume = 9 |issue = 8 |page = 631 |doi = 10.1088/0022-3735/9/8/011 |bibcode = 1976JPhE....9..631P }}</ref> |
|||
It was thought that it would be possible to use X-rays to make holograms of molecules and view them using visible light. However, X-ray holograms have not been created to date.<ref>{{cite web|url=http://hyperphysics.phy-astr.gsu.edu/Hbase/optmod/holog.html |title=Holography |publisher=Hyperphysics.phy-astr.gsu.edu |date= |accessdate=2012-04-21}}</ref> |
|||
A major advance in the field of holography was made by [[Stephen Benton]], who invented a way to create holograms that can be viewed with natural light instead of lasers. These are called [[rainbow hologram]]s.<ref name=FieldGuideHistory /> |
|||
==How holography works== |
|||
==Basics of holography== |
|||
[[File:Holograph-record.svg|thumb|400px|Recording a hologram]] |
[[File:Holograph-record.svg|thumb|400px|Recording a hologram]] |
||
[[File:Holography-reconstruct.svg|thumb|300px|Reconstructing a hologram]] |
[[File:Holography-reconstruct.svg|thumb|300px|Reconstructing a hologram]] |
||
[[File: |
[[File:Structure of a holographic recording.jpg|thumb|This is a photograph of a small part of an unbleached transmission hologram viewed through a microscope. The hologram recorded an image of a toy van and car. It is no more possible to discern the subject of the hologram from this pattern than it is to identify what music has been recorded by looking at a [[compact disc|CD]] surface. The holographic information is recorded by the [[speckle pattern]].]] |
||
Holography is a technique for recording and reconstructing light fields.<ref name="Hariharan basics">{{cite book |last1=Hariharan |first1=P |title=Basics of Holography |date=2002 |publisher=Cambridge University Press |location=Cambridge|isbn = 9780511755569}}</ref>{{rp| Section 1}} |
|||
Holography is a technique that enables a light field, which is generally the product of a light source scattered off objects, to be recorded and later reconstructed when the original light field is no longer present, due to the absence of the original objects.<ref>Hariharan, (2002), Section 1, p1</ref> Holography can be thought of as somewhat similar to [[sound recording]], whereby a sound field created by vibrating matter like [[musical instrument]]s or [[vocal cords]], is encoded in such a way that it can be reproduced later, without the presence of the original vibrating matter. |
|||
A light field is generally the result of a light source scattered off objects. Holography can be thought of as somewhat similar to [[sound recording]], whereby a sound field created by vibrating matter like [[musical instrument]]s or [[vocal cords]], is encoded in such a way that it can be reproduced later, without the presence of the original vibrating matter.<ref>{{Cite book|last=Richards|first=Keith L.|url=https://www.worldcat.org/oclc/990152205|title=Design engineer's sourcebook|date=2018|isbn=978-1-315-35052-3|location=Boca Raton|oclc=990152205}}</ref> However, it is even more similar to [[Ambisonics|Ambisonic]] sound recording in which any listening angle of a sound field can be reproduced in the reproduction. |
|||
===Laser=== |
===Laser=== |
||
In laser holography, the hologram is recorded using a source of [[laser]] light, which is very pure in its color and orderly in its composition. Various setups may be used, and several types of holograms can be made, but all involve the interaction of light coming from different directions and producing a microscopic interference pattern which a [[photographic plate|plate]], film, or other medium [[photography|photographically]] records. |
|||
Holograms are recorded using a flash of light that illuminates a scene and then imprints on a recording medium, much in the way a photograph is recorded. In addition, however, part of the light beam must be shone directly onto the recording medium - this second light beam is known as the [[reference beam]]. A hologram requires a [[laser]] as the sole light source. Lasers can be precisely controlled and have a fixed [[wavelength]], unlike sunlight or light from conventional sources, which contain many different wavelengths. To prevent external light from interfering, holograms are usually taken in darkness, or in low level light of a different colour from the laser light used in making the hologram. |
|||
In one common arrangement, the laser beam is split into two, one known as the [[signal beam|object beam]]<!-- the traditional term, despite the redirect that results --> and the other as the [[reference beam]]. The object beam is expanded by passing it through a lens and used to illuminate the subject. The recording medium is located where this light, after being reflected or scattered by the subject, will strike it. The edges of the medium will ultimately serve as a window through which the subject is seen, so its location is chosen with that in mind. The reference beam is expanded and made to shine directly on the medium, where it interacts with the light coming from the subject to create the desired interference pattern. |
|||
Holography requires a specific [[Exposure (photography)|exposure]] time (just like photography), which can be controlled using a [[Shutter (photography)|shutter]], or by electronically timing the laser. |
|||
Like conventional photography, holography requires an appropriate [[Exposure (photography)|exposure]] time to correctly affect the recording medium. Unlike conventional photography, during the exposure the light source, the optical elements, the recording medium, and the subject must all remain motionless relative to each other, to within about a quarter of the wavelength of the light, or the interference pattern will be blurred and the hologram spoiled. With living subjects and some unstable materials, that is only possible if a very intense and extremely brief pulse of laser light is used, a hazardous procedure which is rarely done outside of scientific and industrial laboratory settings. Exposures lasting several seconds to several minutes, using a much lower-powered continuously operating laser, are typical. |
|||
===Apparatus=== |
===Apparatus=== |
||
A hologram can be made by shining part of the light beam directly into the recording medium, and the other part onto the object in such a way that some of the scattered light falls onto the recording medium. A more flexible arrangement for recording a hologram requires the laser beam to be aimed through a series of elements that change it in different ways. The first element is a [[beam splitter]] that divides the beam into two identical beams, each aimed in different directions: |
|||
* One beam (known as the 'illumination' or 'object beam') is spread using [[Lens (optics)|lenses]] and directed onto the scene using [[mirror]]s. Some of the light scattered (reflected) from the scene then falls onto the recording medium. |
|||
* The second beam (known as the 'reference beam') is also spread through the use of lenses, but is directed so that it does not come in contact with the scene, and instead travels directly onto the recording medium. |
|||
Several different materials can be used as the recording medium. One of the most common is a film very similar to [[photographic film]] ([[silver halide]] [[photographic emulsion]]), but with much smaller light-reactive grains (preferably with diameters less than 20 nm), making it capable of the much higher [[Optical resolution|resolution]] that holograms require. A layer of this recording medium (e.g., silver halide) is attached to a transparent substrate, which is commonly glass, but may also be plastic. |
|||
A hologram can be made by shining part of the light beam directly onto the recording medium, and the other part onto the object in such a way that some of the scattered light falls onto the recording medium. |
|||
A more flexible arrangement for recording a hologram requires the laser beam to be aimed through a series of elements that change it in different ways. The first element is a [[beam splitter]] that divides the beam into two identical beams, each aimed in different directions: |
|||
*One beam (known as the ''illumination'' or ''object beam'') is spread using [[Lens (optics)|lens]]es and directed onto the scene using [[mirror]]s. Some of the light scattered (reflected) from the scene then falls onto the recording medium. |
|||
*The second beam (known as the ''reference beam'') is also spread through the use of lenses, but is directed so that it doesn't come in contact with the scene, and instead travels directly onto the recording medium. |
|||
Several different materials can be used as the recording medium. One of the most common is a film very similar to [[photographic film]] ([[silver halide]] [[photographic emulsion]]), but with a much higher concentration of light-reactive grains, making it capable of the much higher [[Optical resolution|resolution]] that holograms require. A layer of this recording medium (film, etc.) is attached to a transparent substrate, which is commonly glass, but may also be plastic. |
|||
===Process=== |
===Process=== |
||
When the two laser beams reach the recording medium, their light waves intersect and [[Interference (wave propagation)|interfere]] with each other. It is this interference pattern that is imprinted on the recording medium. The pattern itself is seemingly random, as it represents the way in which the scene's light ''interfered'' with the original light source |
When the two laser beams reach the recording medium, their light waves intersect and [[Interference (wave propagation)|interfere]] with each other. It is this interference pattern that is imprinted on the recording medium. The pattern itself is seemingly random, as it represents the way in which the scene's light ''interfered'' with the original light source – but not the original light source itself. The interference pattern can be considered an [[encoded]] version of the scene, requiring a particular key – the original light source – in order to view its contents. |
||
This missing key is provided later by shining a laser, identical to the one used to record the hologram, onto the developed film. When this beam illuminates the hologram, it is |
This missing key is provided later by shining a laser, identical to the one used to record the hologram, onto the developed film. When this beam illuminates the hologram, it is diffracted by the hologram's surface pattern. This produces a light field identical to the one originally produced by the scene and scattered onto the hologram. |
||
===Holography vs. photography=== |
|||
Holography may be better understood via an examination of its differences from ordinary photography: |
|||
===Comparison with photography=== |
|||
Holography may be better understood via an examination of its differences from ordinary [[photography]]: |
|||
* A hologram represents a recording of information regarding the light that came from the original scene as scattered in a range of directions rather than from only one direction, as in a photograph. This allows the scene to be viewed from a range of different angles, as if it were still present. |
* A hologram represents a recording of information regarding the light that came from the original scene as scattered in a range of directions rather than from only one direction, as in a photograph. This allows the scene to be viewed from a range of different angles, as if it were still present. |
||
* A photograph can be recorded using normal light sources (sunlight or electric lighting) whereas a laser is required to record a hologram. |
|||
*A lens is required in photography to record the image, whereas in holography, the light from the object is scattered directly onto the recording medium. |
|||
*A |
* A lens is required in photography to record the image, whereas in holography, the light from the object is scattered directly onto the recording medium. |
||
* A holographic recording requires a second light beam (the reference beam) to be directed onto the recording medium. |
|||
* When a photograph is cut in half, each piece shows half of the scene. When a hologram is cut in half, the whole scene can still be seen in each piece. This is because, whereas each point in a [[photograph]] only represents light scattered from a single point in the scene, ''each point'' on a holographic recording includes information about light scattered from ''every point'' in the scene. Think of viewing a street outside your house through a 4 ft x 4 ft window, and then through a 2 ft x 2 ft window. You can see all of the same things through the smaller window (by moving your head to change your viewing angle), but you can see more ''at once'' through the 4 ft window. |
|||
* Whereas a photograph is a two-dimensional representation that can only reproduce a rudimentary three-dimensional effect, the reproduced viewing range of a hologram adds many more [[Depth perception|depth perception cues]] that were present in the original scene. These cues are recognized by the [[human brain]] and translated into the same perception of a three-dimensional image as when the original scene might have been viewed. |
|||
* A photograph clearly maps out the light field of the original scene. The developed hologram's surface consists of a very fine, seemingly random pattern, which appears to bear no relationship to the scene it recorded. |
|||
* A photograph can be viewed in a wide range of lighting conditions, whereas holograms can only be viewed with very specific forms of illumination. |
* A photograph can be viewed in a wide range of lighting conditions, whereas holograms can only be viewed with very specific forms of illumination. |
||
* When a photograph is cut in half, each piece shows half of the scene. When a hologram is cut in half, the whole scene can still be seen in each piece. This is because, whereas each point in a [[photograph]] only represents light scattered from a single point in the scene, ''each point'' on a holographic recording includes information about light scattered from ''every point'' in the scene. It can be thought of as viewing a street outside a house through a large window, then through a smaller window. One can see all of the same things through the smaller window (by moving the head to change the viewing angle), but the viewer can see more ''at once'' through the large window. |
|||
* A photographic [[Stereoscopy|stereogram]] is a two-dimensional representation that can produce a three-dimensional effect but only from one point of view, whereas the reproduced viewing range of a hologram adds many more [[Depth perception|depth perception cues]] that were present in the original scene. These cues are recognized by the [[human brain]] and translated into the same perception of a three-dimensional image as when the original scene might have been viewed. |
|||
* A photograph clearly maps out the light field of the original scene. The developed hologram's surface consists of a very fine, seemingly random pattern, which appears to bear no relationship to the scene it recorded. |
|||
==Physics of holography== |
==Physics of holography== |
||
{{Main|Physics of optical holography}} |
|||
For a better understanding of the process, it is necessary to understand [[interference (optics)|interference]] and [[diffraction]]. Interference occurs when one or more [[wavefronts]] are superimposed. [[Diffraction]] occurs whenever a wavefront encounters an object. The process of producing a holographic reconstruction is explained below purely in terms of interference and diffraction. It is somewhat simplified but is accurate enough to provide an understanding of how the holographic process works. |
|||
For a better understanding of the process, it is necessary to understand [[Interference (optics)|interference]] and diffraction. Interference occurs when one or more [[wavefronts]] are superimposed. Diffraction occurs when a wavefront encounters an object. The process of producing a holographic reconstruction is explained below purely in terms of interference and diffraction. It is somewhat simplified but is accurate enough to give an understanding of how the holographic process works. |
|||
For those unfamiliar with these concepts, it is worthwhile to read |
For those unfamiliar with these concepts, it is worthwhile to read those articles before reading further in this article. |
||
===Plane wavefronts=== |
===Plane wavefronts=== |
||
A [[diffraction grating]] is a structure with a repeating pattern. A simple example is a metal plate with slits cut at regular intervals. A light wave incident on a grating is split into several waves; the direction of these diffracted waves is determined by the grating spacing and the wavelength of the light. |
A [[diffraction grating]] is a structure with a repeating pattern. A simple example is a metal plate with slits cut at regular intervals. A light wave that is incident on a grating is split into several waves; the direction of these diffracted waves is determined by the grating spacing and the wavelength of the light. |
||
A simple hologram can be made by superimposing two [[plane wave]]s from the same light source on a holographic recording medium. The two waves interfere giving a [[Interference (optics)#Between two plane waves|straight |
A simple hologram can be made by superimposing two [[plane wave]]s from the same light source on a holographic recording medium. The two waves interfere, giving a [[Interference (optics)#Between two plane waves|straight-line fringe pattern]] whose intensity varies sinusoidally across the medium. The spacing of the fringe pattern is determined by the angle between the two waves, and by the wavelength of the light. |
||
The recorded light pattern is a diffraction grating. When it is illuminated by only one of the waves used to create it, it can be shown that one of the diffracted waves emerges at the same angle |
The recorded light pattern is a diffraction grating. When it is illuminated by only one of the waves used to create it, it can be shown that one of the diffracted waves emerges at the same angle at which the second wave was originally incident, so that the second wave has been 'reconstructed'. Thus, the recorded light pattern is a holographic recording as defined above. |
||
===Point sources=== |
===Point sources=== |
||
[[File:Zonenplatte Cosinus.png|upright|thumb|Sinusoidal zone plate]] |
[[File:Zonenplatte Cosinus.png|upright|thumb|Sinusoidal zone plate]] |
||
If the recording medium is illuminated with a point source and a normally incident plane wave, the resulting pattern is a [[Zone plate|sinusoidal zone plate]] which acts as a negative [[Fresnel lens]] whose focal length is equal to the separation of the point source and the recording plane. |
|||
If the recording medium is illuminated with a point source and a normally incident plane wave, the resulting pattern is a [[Zone plate|sinusoidal zone plate]], which acts as a negative [[Fresnel lens]] whose focal length is equal to the separation of the point source and the recording plane. |
|||
When a plane wavefront illuminates a negative lens, it is expanded into a wave which appears to diverge from the focal point of the lens. Thus, when the recorded pattern is illuminated with the original plane wave, some of the light is diffracted into a diverging beam equivalent to the original plane wave; a holographic recording of the point source has been created. |
|||
When a plane wave-front illuminates a negative lens, it is expanded into a wave that appears to diverge from the focal point of the lens. Thus, when the recorded pattern is illuminated with the original plane wave, some of the light is diffracted into a diverging beam equivalent to the original spherical wave; a holographic recording of the point source has been created. |
|||
When the plane wave is incident at a non-normal angle, the pattern formed is more complex but still acts as a negative lens provided it is illuminated at the original angle. |
|||
When the plane wave is incident at a non-normal angle at the time of recording, the pattern formed is more complex, but still acts as a negative lens if it is illuminated at the original angle. |
|||
===Complex objects=== |
===Complex objects=== |
||
To record a hologram of a complex object, a laser beam is first split into two |
To record a hologram of a complex object, a laser beam is first split into two beams of light. One beam illuminates the object, which then scatters light onto the recording medium. According to diffraction theory, each point in the object acts as a point source of light so the recording medium can be considered to be illuminated by a set of point sources located at varying distances from the medium. |
||
The second (reference) beam illuminates the recording medium directly. Each point source wave interferes with the reference beam, giving rise to its own sinusoidal zone plate in the recording medium. The resulting pattern is the sum of all these 'zone plates' which combine to produce a random ([[speckle]]) pattern as in the photograph above. |
The second (reference) beam illuminates the recording medium directly. Each point source wave interferes with the reference beam, giving rise to its own sinusoidal zone plate in the recording medium. The resulting pattern is the sum of all these 'zone plates', which combine to produce a random ([[Speckle pattern|speckle]]) pattern as in the photograph above. |
||
When the hologram is illuminated by the original reference beam, each of the individual zone plates reconstructs the object wave |
When the hologram is illuminated by the original reference beam, each of the individual zone plates reconstructs the object wave that produced it, and these individual wavefronts are combined to reconstruct the whole of the object beam. The viewer perceives a wavefront that is identical with the wavefront scattered from the object onto the recording medium, so that it appears that the object is still in place even if it has been removed. |
||
==Applications== |
|||
===Mathematical model=== |
|||
A single-frequency light wave can be modelled by a [[complex number]] '''U''', which represents the [[electric]] or [[magnetic field]] of the [[electromagnetic radiation#Properties|light wave]]. The [[amplitude]] and [[Phase (waves)|phase]] of the light are represented by the [[Polar form|absolute value]] and [[Polar form|angle]] of the complex number. The object and reference waves at any point in the holographic system are given by '''U'''<sub>O</sub> and '''U'''<sub>R</sub>. The combined beam is given by '''U'''<sub>O</sub> + '''U'''<sub>R</sub>. The energy of the combined beams is proportional to the square of magnitude of the combined waves as: |
|||
<math>|U_O + U_R|^2=U_O U_R^*+|U_R|^2+|U_O|^2+ U_O^*U_R</math> |
|||
If a photographic plate is exposed to the two beams and then developed, its transmittance, '''T''', is proportional to the light energy that was incident on the plate and is given by |
|||
<math>T=kU_O U_R^*+k|U_R|^2+k|U_O|^2+ kU_O^*U_R</math> |
|||
where ''k'' is a constant. |
|||
When the developed plate is illuminated by the reference beam, the light transmitted through the plate, '''U'''<sub>H</sub> is equal to the transmittance '''T''' multiplied by the reference beam amplitude '''U'''<sub>R</sub>, giving |
|||
<math>U_H=TU_R=kU_O|U_R|^2+k|U_R|^2U_R+k|U_O|^2U_R+ kU_O^*U_R^2</math> |
|||
It can be seen that '''U'''<sub>H</sub> has four terms, each representing a light beam emerging from the hologram. The first of these is proportional to '''U'''<sub>O</sub>. This is the reconstructed object beam which enables a viewer to 'see' the original object even when it is no longer present in the field of view. |
|||
The second and third beams are modified versions of the reference beam. The fourth term is known as the "conjugate object beam". It has the reverse curvature to the object beam itself and forms a [[real image]] of the object in the space beyond the holographic plate. |
|||
When the reference and object beams are incident on the holographic recording medium at significantly different angles, the virtual, real and reference wavefronts all emerge at different angles, enabling the reconstructed object to be seen clearly. |
|||
==Recording a hologram== |
|||
===Items required=== |
|||
[[File:Holography setup.jpeg|thumb|An optical table being used to make a hologram]] |
|||
To make a hologram, the following are required: |
|||
* a suitable object or set of objects |
|||
* a suitable laser beam |
|||
* part of the laser beam to be directed so that it illuminates the object (the object beam) and another part so that it illuminates the recording medium directly (the reference beam), enabling the reference beam and the light which is scattered from the object onto the recording medium to form an intereference pattern |
|||
* a recording medium which converts this interference pattern into an optical element which modifies either the amplitude or the phase of an incident light beam according to the intensity of the interference pattern. |
|||
* an environment which provides sufficient mechanical and thermal stability that the interference pattern is stable during the time in which the interference pattern is recorded<ref>Hariharan, (2002), Section 7,1. p60</ref> |
|||
These requirements are inter-related, and it is essential to understand the nature of optical interference to see this. [[Interference (optics)|Interference]] is the variation in [[intensity (physics)|intensity]] which can occur when two [[light waves]] are superimposed. The intensity of the maxima exceeds the sum of the individual intensities of the two beams, and the intensity at the minima is less than this and may be zero. The interference pattern maps the relative phase between the two waves, and any change in the relative phases causes the interference pattern to move across the field of view. If the relative phase of the two waves changes by one cycle, then the pattern drifts by one whole fringe. One phase cycle corresponds to a change in the relative distances travelled by the two beams of one wavelength. Since the wavelength of light is of the order of 0.5μm, it can be seen that very small changes in the optical paths travelled by either of the beams in the holographic recording system lead to movement of the interference pattern which is the holographic recording. Such changes can be caused by relative movements of any of the optical components or the object itself, and also by local changes in air-temperature. It is essential that any such changes are significantly less than the wavelength of light if a clear well-defined recording of the interference is to be created. |
|||
The exposure time required to record the hologram depends on the laser power available, on the particular medium used and on the size and nature of the object(s) to be recorded, just as in conventional photography. This determines the stability requirements. Exposure times of several minutes are typical when using quite powerful gas lasers and silver halide emulsions. All the elements within the optical system have to be stable to fractions of a μm over that period. It is possible to make holograms of much less stable objects by using a [[Laser pulse|pulsed laser]] which produces a large amount of energy in a very short time (μs or less).<ref>Martinez-Hurtado et al. {{doi|10.1021/la102693m}}</ref> These systems have been used to produce holograms of live people. A holographic portrait of Dennis Gabor was produced in 1971 using a pulsed ruby laser.<ref>Hariharan, (2002), Figure 4.5, p44</ref><ref>{{cite web|url=http://webmuseum.mit.edu/browser.php?m=objects&kv=67243&i=14558|title = Photograph of Dennis Gabor standing beside his holographic portrait |publisher=MIT|accessdate= 16/09/2011}}</ref> |
|||
Thus, the laser power, recording medium sensitivity, recording time and mechanical and thermal stability requirements are all interlinked. Generally, the smaller the object, the more compact the optical layout, so that the stability requirements are significantly less than when making holograms of large objects. |
|||
Another very important laser parameter is its [[Coherence (physics)#Temporal coherence|coherence]].<ref>Hariharan, (2002), Section 4.2, p40</ref> This be envisaged by considering a laser to produce a sine wave whose frequency drifts over time; the coherence length can then be considered to be the distance over which it maintains a single frequency. This is important because two waves of different frequencies do not produce a stable interference pattern. The coherence length of the laser determines the depth of field which can be recorded in the scene. A good holography laser will typically have a coherence length of several meters, ample for a deep hologram. |
|||
The objects that form the scene must, in general, have optically rough surfaces so that they scatter light over a wide range of angles. A specularly reflecting (or shiny) surface reflects the light in only one direction at each point on its surface, so in general, most of the light will not be incident on the recording medium. Holograms of flat shiny objects have been made by locating it very close to the recording plate.<ref>Hariharan, (2002), Figure 7.2, p62</ref> |
|||
===Hologram classifications=== |
|||
There are three important properties of a hologram which are defined in this section. A given hologram will have one or other of each of these three properties, e.g. we can have an amplitude modulated thin transmission hologram, or a phase modulated, volume reflection hologram. it is made up of virtual systems. |
|||
====Amplitude and phase modulation holograms==== |
|||
An amplitude modulation hologram is one where the amplitude of light diffracted by the hologram is proportional to the intensity of the recorded light. A straightforward example of this is [[photographic emulsion]] on a transparent substrate. The emulsion is exposed to the interference pattern, and is subsequently developed giving a transmittance which varies with the intensity of the pattern - the more light that fell on the plate at a given point, the darker the developed plate at that point. |
|||
A phase hologram is made by changing either the thickness or the [[refractive index]] of the material in proportion to the intensity of the holographic interference pattern. This is a [[Grating equation|phase grating]] and it can be shown that when such a plate is illuminated by the original reference beam, it reconstructs the original object wavefront. The efficiency (i.e. the fraction of the illuminated beam which is converted to reconstructed object beam) is greater for phase than for amplitude modulated holograms. |
|||
====Thin holograms and thick (volume) holograms==== |
|||
A thin hologram is one where the thickness of the recording medium is much less than the spacing of the interference fringes which make up the holographic recording. |
|||
A thick or [[volume hologram]] is one where the thickness of the recording medium is greater than the spacing of the interference pattern. The recorded hologram is now a three dimensional structure, and it can be shown that incident light is diffracted by the grating only at a particular angle, known as the [[Bragg's law|Bragg angle]].<ref>Lipson, (2011), Seection12.5.4, p443</ref> If the hologram is illuminated with a light source incident at the original reference beam angle but a broad spectrum of wavelengths, reconstruction occurs only at the wavelength of the original laser used. If the angle of illumination is changed, reconstruction will occur at a different wavelength and the colour of the re-consturcted scene changes. A volume hologram effectively acts as a colour filter. |
|||
====Transmission and reflection holograms==== |
|||
A transmission hologram is one where the object and reference beams are incident on the recording medium from the same side. In practice, several more mirrors may be used to direct the beams in the required directions. |
|||
Normally, transmission holograms can only be reconstructed using a laser or a quasi-monochromatic source, but a particular type of transmission hologram, known as a rainbow hologram, can be viewed with white light. |
|||
In a reflection hologram, the object and reference beams are incident on the plate from opposite sides of the plate. The reconstructed object is then viewed from the same side of the plate as that at which the re-constructing beam is incident. |
|||
Only volume holograms can be used to make reflection holograms, as only a very low intensity diffracted beam would be reflected by a thin hologram. |
|||
===Holographic recording media=== |
|||
The recording medium has to convert the original interference pattern into an optical element that modifies either the [[amplitude]] or the [[phase (waves)|phase]] of an incident light beam in proportion to the intensity of the original light field. |
|||
The recording medium should be able to resolve fully all the fringes arising from interference between object and reference beam. These fringe spacings can range from tens of microns to less than one micron, i.e. spatial frequencies ranging from a few hundred to several thousand cycles/mm, and ideally, the recording medium should have a response which is flat over this range. If the response of the medium to these spatial frequencies is low, the diffraction efficiency of the hologram will be poor, and a dim image will be obtained. It should be noted that standard photographic film has a very low, or even zero, response at the frequencies involved and cannot be used to make a hologram - see, for example, Kodak's professional black and white film<ref>{{cite web|url=http://www.kodak.com/eknec/documents/59/0900688a80300559/EpubBW400CN4036.pdf|title=Kodak black and white professional film||accessdate = 14/09/2011}}</ref> whose resolution starts falling off at 20 lines/mm and it is unlikely than any reconstructed beam would be obtained using this film. |
|||
If the response is not flat over the range of spatial frequencies in the interference pattern, then the resolution of the reconstructed image may also be degraded.<ref>Hariharan, (1996), Section 6.4, p88</ref><ref>Kozma A & Zelenka JS, (1970), Effect of film resolution and size in holography, Journal of the Optical Society of America, 60, 34–43</ref> |
|||
The table below shows the principal materials used for holographic recording. Note that these do not include the materials used in the [[Holography#Mass replication of holograms|mass replication]] of an existing hologram which are discussed in the next section. The resolution limit given in the table indicates the maximal number of interference lines/mm of the gratings. The required exposure is for a long exposure. Short exposure times (less than 1/1000 of a second, such as with a pulsed laser) require a higher exposure due to [[reciprocity failure]]. |
|||
{| class="wikitable" |
|||
|+General properties of recording materials for holography. Source:<ref>Hariharan, (2002), Table 6.1, p50</ref> |
|||
|- |
|||
! Material !! Reusable !! Processing !! Type of hologram !! Theoretical maximum efficiency !! Required exposure [mJ/cm<sup>2</sup>] !! Resolution limit [mm<sup>−1</sup>] |
|||
|- |
|||
| rowspan=2| [[Photographic paper|Photographic emulsions]] |
|||
| rowspan=2| No |
|||
| rowspan=2| Wet || Amplitude || 6% |
|||
| rowspan=2| 1.5 |
|||
| rowspan=2| 5000 |
|||
|- |
|||
| Phase (bleached) || 60% |
|||
|- |
|||
| Dichromated gelatin || No || Wet || Phase || 100% || 100 || 10,000 |
|||
|- |
|||
| [[Photoresist]]s || No || Wet || Phase || 30% || 100 || 3,000 |
|||
|- |
|||
| Photothermoplastics || Yes || Charge and heat || Phase || 33% || 0.1 || 500–1,200 |
|||
|- |
|||
| [[Photopolymer]]s || No || Post exposure || Phase || 100% || 10000 || 5,000 |
|||
|-|- |
|||
| [[Photorefractive effect|Photorefractives]] || Yes || None || Phase || 100% || 10 || 10,000 |
|||
|} |
|||
---- |
|||
===Embossing and mass production=== |
|||
An existing hologram can be replicated, either optically, similar to holographic recording or in the case of surface relief holograms, by [[Embossing (manufacturing)|embossing]].<ref>Iwata F & Tsujiiuchi J (1974), "Characteristics oof a photoresisit hologram and its replica", Applied Optics, 13, p1327-36</ref> Surface relief holograms are recorded in photoresists or photothermoplastics and allow cheap mass reproduction. Such embossed holograms are now widely used, for instance, as security features on credit cards or quality merchandise. The [[Royal Canadian Mint]] even produces holographic gold and silver coinage through a complex stamping process.<ref>{{cite web|url=http://www.mint.ca/store/coin/150-lunar-hologram-coin-year-of-the-rabbit-2011-prod990012|title = Lunar Holographic Coins|accessdate = 14/09/2011}}</ref> The first book to feature a hologram on the front cover was ''The Skook'' (Warner Books, 1984) by [[JP Miller]], featuring an illustration by Miller. That same year, "Telstar" by [[Ad Infinitum (band)|Ad Infinitum]] became the first record with a hologram cover and ''[[National Geographic (magazine)|National Geographic]]'' published the first magazine with a hologram cover.<ref>{{cite web|last=Freitas |first=Frank De |url=http://holographica.blogspot.com/2008/07/national-geographic-hologram-1984.html |title=Antiquarian Holographica blog |publisher=Holographica.blogspot.com |date=2008-07-30 |accessdate=2012-04-21}}</ref> |
|||
The first step in the embossing process is to make a stamper by [[Electrophoretic deposition|electrodeposition]] of [[nickel]] on the relief image recorded on the photoresist or photothermoplastic. When the nickel layer is thick enough, it is separated from the master hologram and mounted on a metal backing plate. The material used to make embossed copies consists of a [[polyester]] base film, a resin separation layer and a [[thermoplastic]] film constituting the holographic layer. |
|||
The embossing process can be carried out with a simple heated press. The bottom layer of the duplicating film (the thermoplastic layer) is heated above its softening point and pressed against the stamper, so that it takes up its shape. This shape is retained when the film is cooled and removed from the press. In order to permit the viewing of embossed holograms in reflection, an additional reflecting layer of aluminum is usually added on the hologram recording layer. Embossed holograms are used widely on credit cards, banknotes, and high value products.<ref>Hariharan, (2002), Section 9.2, p80</ref> |
|||
It is possible to print holograms directly into steel using a sheet explosive charge to create the required surface relief.<ref>{{cite web|url=http://www.physorg.com/news124039000.html |title=Holograms with explosive power |publisher=Physorg.com |date= |accessdate=2012-04-21}}</ref> |
|||
==Reconstructing and viewing the holographic image== |
|||
When the hologram plate is illuminated by a laser beam identical to the reference beam which was used to record the hologram, an exact reconstruction of the original object wavefront is obtained. An imaging system (an eye or a camera) located in the reconstructed beam 'sees' exactly the same scene as it would have done when viewing the original. When the lens is moved, the image changes in the same way as it would have done when the object was in place. If several objects were present when the hologram was recorded, the reconstructed objects move relative to one another, i.e. exhibit [[parallax]], in the same way as the original objects would have done. It was very common in the early days of holography to use a chess board as the object and then take photographs at several different angles using the reconstructed light to show how the relative positions of the chess pieces appeared to change. |
|||
A holographic image can also be obtained using a different laser beam configuration to the original recording object beam, but the reconstructed image will not match the original exactly.<ref>Hariharan, (2002), Section 2.3, p17</ref> When a laser is used to reconstruct the hologram, the image is [[speckle pattern|speckled]] just as the original image will have been. This can be a major drawback in viewing a hologram. |
|||
White light consists of light of a wide range of wavelengths. Normally, if a hologram is illuminated by a white light source, each wavelength can be considered to generate its own holographic reconstruction, and these will vary in size, angle, and distance. These will be superimposed, and the summed image will wipe out any information about the original scene, just as if you superimposed a set of photographs of the same object of different sizes and orientations. However, a holographic image can be obtained using [[white light]] in specific circumstances, e.g. with volume holograms and rainbow holograms. The white light source used to view these holograms should always approximate to a point source, i.e. a spot light or the sun. An extended source (e.g. a fluorescent lamp) will not reconstruct a hologram since it light is incident at each point at a wide range of angles, giving multiple reconstructions which will "wipe" one another out. |
|||
White light reconstructions do not contain speckles. |
|||
===Volume holograms=== |
|||
{{main|Volume hologram}} |
|||
A volume hologram can give a reconstructed beam using white light, as the hologram structure effectively filters out colours other than those equal to or very close to the colour of the laser used to make the hologram so that the reconstructed image will appear to be approximately the same colour as the laser light used to create the holographic recording. |
|||
===Rainbow holograms=== |
|||
{{main|Rainbow hologram}} |
|||
[[File:Rainbow hologram.jpeg|thumb|Rainbow hologram showing the change in colour in the vertical direction]] |
|||
In this method, parallax in the vertical plane is sacrificed to allow a bright well-defined single colour re-constructed image to be obtained using white light. The rainbow holography recording process uses a horizontal slit to eliminate vertical [[parallax]] in the output image. The viewer is then effectively viewing the holographic image through a narrow horizontal slit. Horizontal parallax information is preserved but movement in the vertical direction produces colour rather than different vertical perspectives.<ref>Hariharan, (2002), Section 7.4, p63</ref> [[Stereopsis]] and horizontal motion parallax, two relatively powerful cues to depth, are preserved. |
|||
The holograms found on [[credit cards]] are examples of rainbow holograms. These are technically transmission holograms mounted onto a reflective surface like a [[PET film (biaxially oriented)|metalized polyethylene terephthalate]] substrate commonly known as [[polyethylene terephthalate|PET]]. |
|||
===Fidelity of the reconstructed beam=== |
|||
[[File:broken hologram.jpg|thumb|Reconstructions from two parts of a broken hologram. Note the different viewpoints required to see the whole object]] |
|||
To replicate the original object beam exactly, the reconstructing reference beam must be identical to the original reference beam and the recording medium must be able to fully resolve the interference pattern formed between the object and reference beams. Exact reconstruction is required in [[holographic interferometry]], where the holographically reconstructed wavefront [[Interference (wave propagation)|interferes]] with the wavefront coming from the actual object, giving a null fringe if there has been no movement of the object and mapping out the displacement if the object has moved. This requires very precise relocation of the developed holographic plate. |
|||
Any change in the shape, orientation or wavelength of the reference beam gives rise to aberrations in the reconstructed image. For instance, the reconstructed image is magnified if the laser used to reconstruct the hologram has a shorter wavelength than the original laser. Nonetheless, good reconstruction is obtained using a laser of a different wavelength, quasi-monochromatic light or white light, in the right circumstances. |
|||
Since each point in the object illuminates all of the hologram, the whole object can be reconstructed from a small part of the hologram. Thus, a hologram can be broken up into small pieces and each one will enable the whole of the original object to be imaged. One does, however, lose information and the [[optical resolution|spatial resolution]] gets worse as the size of the hologram is decreased — the image becomes "fuzzier". The field of view is also reduced, and the viewer will have to change position to see different parts of the scene. |
|||
==Applications== |
|||
===Art=== |
===Art=== |
||
Early on, artists saw the potential of holography as a medium and gained access to science laboratories to create their work. Holographic art is often the result of collaborations between scientists and artists, although some holographers would regard themselves as both an artist and a scientist. |
Early on, artists saw the potential of holography as a medium and gained access to science laboratories to create their work. Holographic art is often the result of collaborations between scientists and artists, although some holographers would regard themselves as both an artist and a scientist. |
||
[[Salvador Dalí]] claimed to have been the first to employ holography artistically. He was certainly the first and best-known surrealist to do so, but the 1972 New York exhibit of Dalí holograms had been preceded by the holographic art exhibition that was held at the [[Cranbrook Academy of Art]] in Michigan in 1968 and by the one at the Finch College gallery in New York in 1970, which attracted national media attention.<ref>{{cite web|url=http://holophile.com/history.htm |title=The History and Development of Holography|publisher=Holophile.com |date |
[[Salvador Dalí]] claimed to have been the first to employ holography artistically. He was certainly the first and best-known surrealist to do so, but the 1972 New York exhibit of Dalí holograms had been preceded by the holographic art exhibition that was held at the [[Cranbrook Academy of Art]] in Michigan in 1968 and by the one at the Finch College gallery in New York in 1970, which attracted national media attention.<ref>{{cite web|url=http://holophile.com/history.htm |title=The History and Development of Holography|publisher=Holophile.com |access-date=2012-04-21}}</ref> In Great Britain, [[Margaret Benyon]] began using holography as an artistic medium in the late 1960s and had a solo exhibition at the [[University of Nottingham]] art gallery in 1969.<ref name=Coyle>{{Cite book| publisher = John Libbey and Company| isbn = 978-0-86196-266-2| pages = 65–88|editor-first1= Philip |editor-last1= Hayward | last = Coyle| first = Rebecca| title = Culture, Technology & Creativity in the Late Twentieth Century| chapter = Holography – Art in the space of technology| location = London, England| date = 1990| chapter-url = https://books.google.com/books?id=yLq3rM2at3cC&pg=PA67}}</ref> This was followed in 1970 by a solo show at the [[Lisson Gallery]] in London, which was billed as the "first London expo of holograms and stereoscopic paintings".<ref name="poster">{{cite web|title=Margaret Benyon Holography|url=http://www.lissongallery.com/exhibitions/margaret-benyon|website=Lisson Gallery|access-date=4 February 2016}}</ref> |
||
During the 1970s, a number of art studios and schools were established, each with their particular approach to holography. Notably, there was the San Francisco School of Holography established by [[Lloyd Cross]], The Museum of Holography in New York founded by Rosemary ( |
During the 1970s, a number of art studios and schools were established, each with their particular approach to holography. Notably, there was the San Francisco School of Holography established by [[Lloyd Cross]], The Museum of Holography in New York founded by Rosemary (Posy) H. Jackson, the Royal College of Art in London and the [[Lake Forest College]] Symposiums organised by [[Tung Jeong]].<ref>{{cite web|author=Integraf |url=http://www.integraf.com/tung_jeong.htm |title=Dr. Tung J. Jeong Biography |publisher=Integraf.com |access-date=2012-04-21}}</ref> None of these studios still exist; however, there is the Center for the Holographic Arts in New York<ref>{{cite web|url=http://www.holocenter.org |title=holocenter |publisher=holocenter |access-date=2012-04-21}}</ref> and the HOLOcenter in Seoul, which offers artists a place to create and exhibit work. |
||
During the 1980s, many artists who worked with holography helped the diffusion of this so-called "new medium" in the art world, such as Harriet Casdin-Silver of the |
During the 1980s, many artists who worked with holography helped the diffusion of this so-called "new medium" in the art world, such as Harriet Casdin-Silver of the United States, [[Dieter Jung (artist)|Dieter Jung]] of [[Germany]], and [[Moysés Baumstein]] of [[Brazil]], each one searching for a proper "language" to use with the three-dimensional work, avoiding the simple holographic reproduction of a sculpture or object. For instance, in Brazil, many concrete poets (Augusto de Campos, Décio Pignatari, Julio Plaza and José Wagner Garcia, associated with [[Moysés Baumstein]]) found in holography a way to express themselves and to renew [[Concrete Poetry]]. |
||
A small but active group of artists still |
A small but active group of artists still integrate holographic elements into their work.<ref>{{cite web |url=http://www.universal-hologram.com/ |title=The Universal Hologram |website=Cherry Optical Holography}}</ref> Some are associated with novel holographic techniques; for example, artist Matt Brand<ref>Holographic metalwork http://www.zintaglio.com</ref> employed computational mirror design to eliminate image distortion from [[specular holography]]. |
||
The MIT Museum<ref>{{cite web|url=http://web.mit.edu/museum/collections/holography.html |title=MIT Museum: Collections |
The MIT Museum<ref>{{cite web|url=http://web.mit.edu/museum/collections/holography.html |title=MIT Museum: Collections – Holography |publisher=Web.mit.edu |access-date=2012-04-21}}</ref> and Jonathan Ross<ref>{{cite web|url=http://www.jrholocollection.com/ |title=The Jonathan Ross Hologram Collection |publisher=Jrholocollection.com |access-date=2012-04-21}}</ref> both have extensive collections of holography and on-line catalogues of art holograms. |
||
===Data storage=== |
===Data storage=== |
||
{{Main|Holographic |
{{Main|Holographic data storage}} |
||
Holographic data storage is a technique that can store information at high density inside crystals or photopolymers. The ability to store large amounts of information in some kind of medium is of great importance, as many electronic products incorporate storage devices. As current storage techniques such as [[Blu-ray Disc]] reach the limit of possible data density (due to the diffraction-limited size of the writing beams), holographic storage has the potential to become the next generation of popular storage media. The advantage of this type of data storage is that the volume of the recording media is used instead of just the surface. |
|||
Currently available [[spatial light modulator|SLMs]] can produce about 1000 different images a second at 1024×1024-bit resolution which would result in about one-[[gigabit per second|gigabit-per-second]] writing speed.<ref>{{Cite journal |last1=Lang |first1=M. |last2=Eschler |first2=H. |date=1974-10-01 |title=Gigabyte capacities for holographic memories |url=https://dx.doi.org/10.1016/0030-3992%2874%2990061-9 |journal=Optics & Laser Technology |language=en |volume=6 |issue=5 |pages=219–224 |doi=10.1016/0030-3992(74)90061-9 |bibcode=1974OptLT...6..219L |issn=0030-3992}}</ref> |
|||
In 2005, companies such as Optware and [[Maxell]] produced a 120 mm disc that uses a holographic layer to store data to a potential 3.9 [[terabyte|TB]], a format called [[Holographic Versatile Disc]]. As of September 2014, no commercial product has been released. |
|||
Holography can be put to a variety of uses other than recording images. [[Holographic data storage]] is a technique that can store information at high density inside crystals or photopolymers. The ability to store large amounts of information in some kind of media is of great importance, as many electronic products incorporate storage devices. As current storage techniques such as [[Blu-ray Disc]] reach the limit of possible data density (due to the [[diffraction]]-limited size of the writing beams), holographic storage has the potential to become the next generation of popular storage media. The advantage of this type of data storage is that the volume of the recording media is used instead of just the surface. |
|||
Currently available [[spatial light modulator|SLMs]] can produce about 1000 different images a second at 1024×1024-bit resolution. With the right type of media (probably polymers rather than something like [[lithium niobate|LiNbO<sub>3</sub>]]), this would result in about one-[[gigabit per second|gigabit-per-second]] writing speed. Read speeds can surpass this, and experts believe one-[[terabit per second|terabit-per-second]] readout is possible. |
|||
Another company, [[InPhase Technologies]], was developing a competing format, but went bankrupt in 2011 and all its assets were sold to Akonia Holographics, LLC. |
|||
While many holographic data storage models have used "page-based" storage, where each recorded hologram holds a large amount of data, more recent research into using submicrometre-sized "microholograms" has resulted in several potential [[3D optical data storage]] solutions. While this approach to data storage can not attain the high data rates of page-based storage, the tolerances, technological hurdles, and cost of producing a commercial product are significantly lower. |
|||
===Dynamic holography=== |
===Dynamic holography=== |
||
Line 296: | Line 137: | ||
[[File:Contest3.jpg|thumb|''Peace Within Reach'', a Denisyuk DCG hologram by amateur Dave Battin]] |
[[File:Contest3.jpg|thumb|''Peace Within Reach'', a Denisyuk DCG hologram by amateur Dave Battin]] |
||
Since the beginning of holography, many holographers have explored its uses and displayed them to the public. |
|||
Since the beginning of holography, experimenters have explored its uses. Starting in 1971, [[Lloyd Cross]] started the San Francisco School of Holography and started to teach amateurs the methods of making holograms with inexpensive equipment. This method relied on the use of a large table of deep sand to hold the [[optics]] rigid and damp [[vibration]]s that would destroy the image. |
|||
In 1971, [[Lloyd Cross]] opened the San Francisco School of Holography and taught amateurs how to make holograms using only a small (typically 5 mW) [[helium-neon laser]] and inexpensive home-made equipment. Holography had been supposed to require a very expensive metal [[optical table]] set-up to lock all the involved elements down in place and damp any vibrations that could blur the interference fringes and ruin the hologram. Cross's home-brew alternative was a [[sandpit|sandbox]] made of a [[cinder block]] retaining wall on a plywood base, supported on stacks of old tires to isolate it from ground vibrations, and filled with sand that had been washed to remove dust. The laser was securely mounted atop the cinder block wall. The mirrors and simple lenses needed for directing, splitting and expanding the laser beam were affixed to short lengths of PVC pipe, which were stuck into the sand at the desired locations. The subject and the [[photographic plate]] holder were similarly supported within the sandbox. The holographer turned off the room light, blocked the laser beam near its source using a small [[relay]]-controlled shutter, loaded a plate into the holder in the dark, left the room, waited a few minutes to let everything settle, then made the exposure by remotely operating the laser shutter. |
|||
Many of these holographers would go on to produce art holograms. In 1983, Fred Unterseher published the ''Holography Handbook'', a remarkably easy-to-read description of making holograms at home. This brought in a new wave of holographers and gave simple methods to use the then-available AGFA [[silver halide]] recording materials. |
|||
In 1979, [[Jason Sapan]] opened the [[Holographic Studios]] in [[New York City]]. Since then, they have been involved in the production of many holographs for many artists as well as companies.<ref>{{cite news | url=https://www.thedailybeast.com/new-yorks-hologram-king-is-also-the-citys-last-pro-holographer | title=New York's Hologram King is Also the City's Last Pro Holographer | newspaper=The Daily Beast | date=27 May 2014 | last1=Strochlic | first1=Nina }}</ref> Sapan has been described as the "last professional holographer of New York". |
|||
In 2000, [[Frank DeFreitas]] published the ''Shoebox Holography Book'' and introduced the use of inexpensive [[laser pointer]]s to countless [[hobby]]ists. This was a very important development for amateurs, as the cost for a 5 mW laser dropped from $1200 to $5 as semiconductor laser diodes reached mass market. Now, there are hundreds to thousands of amateur holographers worldwide. |
|||
Many of these holographers would go on to produce art holograms. In 1983, Fred Unterseher, a co-founder of the San Francisco School of Holography and a well-known holographic artist, published the ''Holography Handbook'', an easy-to-read guide to making holograms at home. This brought in a new wave of holographers and provided simple methods for using the then-available AGFA [[silver halide]] recording materials. |
|||
In 2006, a large number of surplus Holography Quality Green Lasers (Coherent C315) became available and put Dichromated Gelatin (DCG) within the reach of the amateur holographer. The holography community was surprised at the amazing sensitivity of DCG to green [[light]]. It had been assumed that the sensitivity would be non-existent. Jeff Blyth responded with the G307 formulation of DCG to increase the speed and sensitivity to these new lasers.<ref>{{cite web|url=http://www.holowiki.com/index.php/G307_DCG_Formula |title=A Holography FAQ |publisher=HoloWiki |date=2011-02-15 |accessdate=2012-04-21}}</ref> |
|||
In 2000, [[Frank DeFreitas]] published the ''Shoebox Holography Book'' and introduced the use of inexpensive [[laser pointer]]s to countless [[hobby]]ists. For many years, it had been assumed that certain characteristics of semiconductor [[laser diodes]] made them virtually useless for creating holograms, but when they were eventually put to the test of practical experiment, it was found that not only was this untrue, but that some actually provided a [[coherence length]] much greater than that of traditional helium-neon gas lasers. This was a very important development for amateurs, as the price of red laser diodes had dropped from hundreds of dollars in the early 1980s to about $5 after they entered the mass market as a component pulled from [[Compact disc|CD]], or later, [[DVD]] players from the mid 1980s onwards. Now, there are thousands of amateur holographers worldwide. |
|||
Many film suppliers have come and gone from the silver-halide market. While more film manufactures have filled in the voids, many amateurs are now making their own film. The favorite formulations are Dichromated Gelatin, Methylene Blue Sensitised Dichromated Gelatin and Diffusion Method Silver Halide preparations. Jeff Blyth has published very accurate methods for making film in a small lab or garage.<ref>{{cite web|url=http://www.holowiki.com/index.php/Special:Search?search=Blyth&go=Go |title=Many methods are here |publisher=Holowiki.com |date= |accessdate=2012-04-21}}</ref> |
|||
By late 2000, holography kits with inexpensive laser pointer diodes entered the mainstream consumer market. These kits enabled students, teachers, and hobbyists to make several kinds of holograms without specialized equipment, and became popular gift items by 2005.<ref name="IEEE">Stephen Cass: ''[https://spectrum.ieee.org/holiday-gifts-2005 Holiday Gifts 2005 Gifts and gadgets for technophiles of all ages: Do-It Yourself-3-D]''. In ''IEEE Spectrum'', November 2005</ref> The introduction of holography kits with self-developing [[photographic plate|plates]] in 2003 made it possible for hobbyists to create holograms without the bother of wet chemical processing.<ref name="physicsteacher">Chiaverina, Chris: ''[http://www.litiholo.com/Hologram%20Kit%20article%20Physics%20Teacher%20Nov%202010.pdf Litiholo holography – So easy even a caveman could have done it (apparatus review)] {{webarchive|url=https://web.archive.org/web/20120208030253/http://www.litiholo.com/Hologram%20Kit%20article%20Physics%20Teacher%20Nov%202010.pdf |date=8 February 2012 }}''. In ''The Physics Teacher'', vol. 48, November 2010, pp. 551–552.</ref> |
|||
A small group of amateurs are even constructing their own pulsed lasers to make holograms of moving objects.<ref>{{cite web|url=http://cabd0.tripod.com/holograms/index.html |title=Jeff Blyth's Film Formulations |publisher=Cabd0.tripod.com |date= |accessdate=2012-04-21}}</ref> |
|||
In 2006, a large number of surplus holography-quality green lasers (Coherent C315) became available and put dichromated gelatin (DCG) holography within the reach of the amateur holographer. The holography community was surprised at the amazing sensitivity of DCG to green light. It had been assumed that this sensitivity would be uselessly slight or non-existent. Jeff Blyth responded with the G307 formulation of DCG to increase the speed and sensitivity to these new lasers.<ref>{{cite web |url=http://www.holowiki.com/index.php/G307_DCG_Formula |title=A Holography FAQ |publisher=HoloWiki |date=2011-02-15 |access-date=2012-04-21 |url-status=dead |archive-url=https://web.archive.org/web/20101106135632/http://www.holowiki.com/index.php/G307_DCG_Formula |archive-date=6 November 2010}}</ref> |
|||
Holography kits with self-developing film plates have now entered the consumer market. The kits make holographs and have been found to be fairly error tolerant,<ref name="physicsteacher">http://www.litiholo.com/Hologram%20Kit%20article%20Physics%20Teacher%20Nov%202010.pdf</ref> and enable holograms to be made without any other specialized equipment. |
|||
Kodak and Agfa, the former major suppliers of holography-quality silver halide plates and films, are no longer in the market. While other manufacturers have helped fill the void, many amateurs are now making their own materials. The favorite formulations are dichromated gelatin, Methylene-Blue-sensitised dichromated gelatin, and diffusion method silver halide preparations. Jeff Blyth has published very accurate methods for making these in a small lab or garage.<ref>{{cite web |url=http://www.holowiki.com/index.php/Special:Search?search=Blyth&go=Go |title=Many methods are here |publisher=Holowiki.com |access-date=2012-04-21 |url-status=dead |archive-url=https://web.archive.org/web/20120307232834/http://www.holowiki.com/index.php/Special%3ASearch?search=Blyth&go=Go |archive-date=7 March 2012}}</ref> |
|||
A small group of amateurs are even constructing their own pulsed lasers to make holograms of living subjects and other unsteady or moving objects.<ref>{{cite web|url=http://cabd0.tripod.com/holograms/index.html |title=Jeff Blyth's Film Formulations |publisher=Cabd0.tripod.com |access-date=2012-04-21}}</ref> |
|||
===Holographic interferometry=== |
===Holographic interferometry=== |
||
{{Main|holographic interferometry}} |
{{Main|holographic interferometry}} |
||
Holographic interferometry (HI) is a technique that enables static and dynamic displacements of objects with optically rough surfaces to be measured to optical interferometric precision (i.e. to fractions of a wavelength of light).<ref>Powell RL |
Holographic interferometry (HI) is a technique that enables static and dynamic displacements of objects with optically rough surfaces to be measured to optical interferometric precision (i.e. to fractions of a wavelength of light).<ref>{{cite journal | last1 = Powell | first1 = RL | last2 = Stetson | first2 = KA | year = 1965 | title = Interferometric Vibration Analysis by Wavefront Reconstruction| journal = J. Opt. Soc. Am. | volume = 55 | issue = 12 | pages = 1593–8 | doi = 10.1364/josa.55.001593 | bibcode = 1965JOSA...55.1593P }}</ref><ref>{{cite book |last1=Jones |first1=Robert |last2=Wykes |first2=Catherine |title=Holographic and Speckle Interferometry |date=1989 |publisher=Cambridge University Press |location=Cambridge |isbn=0-521-34417-4}}</ref> It can also be used to detect optical-path-length variations in transparent media, which enables, for example, fluid flow to be visualized and analyzed. It can also be used to generate contours representing the form of the surface or the isodose regions in radiation dosimetry.<ref>{{cite journal|last1=Beigzadeh |first1=A.M. |last2=Vaziri |first2=M.R. Rashidian |last3=Ziaie |first3=F. |title=Modelling of a holographic interferometry based calorimeter for radiation dosimetry|journal=Nuclear Instruments and Methods in Physics Research A|date=2017|volume=864|pages=40–49|doi=10.1016/j.nima.2017.05.019|bibcode=2017NIMPA.864...40B}}</ref> |
||
It has been widely used to measure stress, strain, and vibration in engineering structures. |
It has been widely used to measure stress, strain, and vibration in engineering structures. |
||
Line 320: | Line 165: | ||
{{Main|Interferometric microscopy}} |
{{Main|Interferometric microscopy}} |
||
The hologram keeps the information on the amplitude and phase of the field. Several holograms may keep information about the same distribution of light, emitted to various directions. The numerical analysis of such holograms allows one to emulate large [[numerical aperture]], which, in turn, enables enhancement of the resolution of [[optical microscopy]]. |
The hologram keeps the information on the amplitude and phase of the field. Several holograms may keep information about the same distribution of light, emitted to various directions. The numerical analysis of such holograms allows one to emulate large [[numerical aperture]], which, in turn, enables enhancement of the resolution of [[optical microscopy]]. The corresponding technique is called [[interferometric microscopy]]. Recent achievements of interferometric microscopy allow one to approach the quarter-wavelength limit of resolution.<ref name="U1">{{Cite journal |
||
The corresponding technique is called [[interferometric microscopy]]. Recent achievements of interferometric microscopy allow one to approach the quarter-wavelength limit of resolution.<ref name="U1">{{Cite journal |
|||
|url=http://www.opticsexpress.org/abstract.cfm?id=134719 |
|||
| author=Y.Kuznetsova |
| author=Y.Kuznetsova |
||
| |
|author2=A.Neumann, S.R.Brueck |
||
| title=Imaging interferometric microscopy–approaching the linear systems limits of |
| title=Imaging interferometric microscopy–approaching the linear systems limits of optical resolution |
||
| journal=[[Optics Express]] |
| journal=[[Optics Express]] |
||
| volume=15 |
| volume=15 |
||
Line 333: | Line 176: | ||
|bibcode = 2007OExpr..15.6651K |
|bibcode = 2007OExpr..15.6651K |
||
| pmid=19546975 |
| pmid=19546975 |
||
|issue=11 |
|issue=11| doi-access=free |
||
}}</ref> |
|||
===Sensors or biosensors=== |
===Sensors or biosensors=== |
||
{{Main|Holographic sensor}} |
{{Main|Holographic sensor}} |
||
The hologram is made with a modified material that interacts with certain molecules generating a change in the fringe periodicity or refractive index, therefore, the color of the holographic reflection.<ref>{{cite journal |first1=AK |last1=Yetisen |first2=H |last2=Butt |first3=F |last3=da Cruz Vasconcellos |first4=Y |last4=Montelongo |first5=CAB |last5=Davidson |first6=J |last6=Blyth |first7=JB |last7=Carmody |first8=S |last8=Vignolini |first9=U |last9=Steiner |first10=JJ |last10=Baumberg |first11=TD |last11=Wilkinson |first12=CR |last12=Lowe |title=Light-Directed Writing of Chemically Tunable Narrow-Band Holographic Sensors |journal= Advanced Optical Materials |volume=2 |issue=3 |pages=250–254 |year=2013 |doi= 10.1002/adom.201300375 |s2cid=96257175 |url=https://www.repository.cam.ac.uk/handle/1810/293246 }}</ref><ref>{{Cite journal | last1 = MartíNez-Hurtado | first1 = J. L. | last2 = Davidson | first2 = C. A. B. | last3 = Blyth | first3 = J. | last4 = Lowe | first4 = C. R. | title = Holographic Detection of Hydrocarbon Gases and Other Volatile Organic Compounds | doi = 10.1021/la102693m | journal = Langmuir | volume = 26 | issue = 19 | pages = 15694–15699 | year = 2010 | pmid = 20836549}}</ref> |
|||
The hologram is made with a modified material that interacts with certain molecules generating a change in the fringe periodicity or refractive index, therefore, the color of the holographic reflection.<ref>Martinez-Hurtado et al 2010; http://pubs.acs.org/doi/abs/10.1021/la102693m</ref> |
|||
===Security=== |
===Security=== |
||
{{Main|Security hologram}} |
{{Main|Security hologram}} |
||
[[File:Hologramm.JPG|thumb|left|''Identigram'' as a security element in a German identity card]] |
[[File:Hologramm.JPG|thumb|left|''Identigram'' as a security element in a German identity card]] |
||
[[File:Visa Dove Hologram Rainbow.jpg|thumb|Dove hologram used on some [[credit card]]s]] |
|||
Security holograms are very difficult to forge, because they are [[holography#Mass replication of holograms|replicated]] from a master hologram that requires expensive, specialized and technologically advanced equipment. They are used widely in many [[currencies]], such as the [[Brazilian real]] 20 note, [[Pound sterling|British pound]] 5/10/20 notes, [[Estonian kroon]] 25/50/100/500 notes, [[American dollar]] 5/10/20/50/100 notes, [[Euro]] 5/10/20/50/100/200/500 notes, [[South Korean won]] 5000/10000/50000 notes, and [[Japanese yen]] 5000/10000 notes. They are also used in credit and bank cards as well as [[passport]]s, ID cards, [[book]]s, [[DVD]]s, and [[sports equipment]]. |
|||
Holograms are commonly used for security, as they are [[#Copying and mass production|replicated]] from a master hologram that requires expensive, specialized and technologically advanced equipment, and are thus difficult to forge. They are used widely in many [[currency|currencies]], such as the [[Brazilian real|Brazilian]] 20, 50, and 100-reais notes; [[Pound sterling|British]] 5, 10, 20 and 50-pound notes; [[South Korean won|South Korean]] 5000, 10,000, and 50,000-won notes; [[Japanese yen|Japanese]] 5000 and 10,000 yen notes, [[Indian rupee|Indian]] 50, 100, 500, and 2000 rupee notes; and all the currently-circulating banknotes of the [[Canadian dollar]], [[Croatian kuna]], [[Danish krone]], and [[Euro]]. They can also be found in [[credit card|credit]] and [[bank card]]s as well as [[passport]]s, ID cards, [[book]]s, food packaging, [[DVD]]s, and sports equipment. Such holograms come in a variety of forms, from adhesive strips that are laminated on packaging for [[fast-moving consumer goods]] to holographic tags on [[Consumer electronics|electronic products]]. They often contain textual or pictorial elements to protect identities and separate genuine articles from [[counterfeit]]s. |
|||
===Other applications=== |
|||
Holographic scanners are in use in post offices, larger shipping firms, and automated conveyor systems to determine the three-dimensional size of a package. They are often used in tandem with [[checkweigher]]s to allow automated pre-packing of given volumes, such as a truck or pallet for bulk shipment of goods. |
Holographic scanners are in use in post offices, larger shipping firms, and automated conveyor systems to determine the three-dimensional size of a package. They are often used in tandem with [[checkweigher]]s to allow automated pre-packing of given volumes, such as a truck or pallet for bulk shipment of goods. |
||
Holograms produced in elastomers can be used as stress-strain reporters due to its elasticity and compressibility, the pressure and force applied are correlated to the reflected wavelength, therefore its color.<ref>'Elastic hologram' pages 113–117, Proc. of the IGC 2010, ISBN |
Holograms produced in elastomers can be used as stress-strain reporters due to its elasticity and compressibility, the pressure and force applied are correlated to the reflected wavelength, therefore its color.<ref>'Elastic hologram' pages 113–117, Proc. of the IGC 2010, {{ISBN|978-0-9566139-1-2}} here: http://www.dspace.cam.ac.uk/handle/1810/225960</ref> Holography technique can also be effectively used for radiation dosimetry.<ref>{{cite journal |last1=Beigzadeh |first1=A.M. |title=Modelling of a holographic interferometry based calorimeter for radiation dosimetry |journal=Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment |volume=864 |pages=40–49 |doi=10.1016/j.nima.2017.05.019 |year=2017 |bibcode=2017NIMPA.864...40B }}</ref><ref>{{cite journal |last1=Beigzadeh |first1=A.M. |title=Double-exposure holographic interferometry for radiation dosimetry: A new developed model |journal=Radiation Measurements |date=2018 |volume=119 |pages=132–139 |doi=10.1016/j.radmeas.2018.10.010 |bibcode=2018RadM..119..132B |s2cid=105842469 }}</ref> |
||
==== High security registration plates ==== |
|||
==Non-optical holography== |
|||
High-security holograms can be used on license plates for vehicles such as cars and motorcycles. As of April 2019, holographic license plates are required on vehicles in parts of India to aid in identification and security, especially in cases of car theft. Such number plates hold electronic data of vehicles, and have a unique ID number and a sticker to indicate authenticity.<ref>{{cite web |title=Why has the government made high security registration plates mandatory |url=https://economictimes.indiatimes.com/industry/auto/auto-news/why-has-the-government-made-high-security-registration-plates-mandatory/what-is-hsrp/slideshow/79936271.cms |website=The Economic Times |publisher=ET Online |access-date=18 July 2021}}</ref> |
|||
==Holography using other types of waves== |
|||
In principle, it is possible to make a hologram for any [[wave]]. |
In principle, it is possible to make a hologram for any [[wave]]. |
||
[[Electron holography]] is the application of holography techniques to electron waves rather than light waves. Electron holography was invented by Dennis Gabor to improve the resolution and avoid the aberrations of the [[transmission electron microscope]]. Today it is commonly used to study electric and magnetic fields in thin films, as magnetic and electric fields can shift the phase of the interfering wave passing through the sample.<ref>R. E. Dunin-Borkowski et al., Micros. Res. and Tech. vol. 64, pp. 390–402 (2004)</ref> The principle of electron holography can also be applied to [[interference lithography]].<ref> |
[[Electron holography]] is the application of holography techniques to electron waves rather than light waves. Electron holography was invented by Dennis Gabor to improve the resolution and avoid the aberrations of the [[transmission electron microscope]]. Today it is commonly used to study electric and magnetic fields in thin films, as magnetic and electric fields can shift the phase of the interfering wave passing through the sample.<ref>R. E. Dunin-Borkowski et al., Micros. Res. and Tech. vol. 64, pp. 390–402 (2004)</ref> The principle of electron holography can also be applied to [[interference lithography]].<ref>{{cite journal | last1 = Ogai | first1 = K. | display-authors = etal | year = 1993 | title = An Approach for Nanolithography Using Electron Holography| journal = Jpn. J. Appl. Phys. | volume = 32 | issue = 12S | pages = 5988–5992 | doi = 10.1143/jjap.32.5988 | bibcode = 1993JaJAP..32.5988O | s2cid = 123606284 }}</ref> |
||
[[Acoustic holography]] enables sound maps of an object to be generated. Measurements of the acoustic field are made at many points close to the object. These measurements are digitally processed to produce the "images" of the object.<ref>{{cite web |title=Acoustic Holography |url=https://www.bksv.com/en/knowledge/applications/noise-source-identification/acoustic-holography |website=Bruel and Kjaer |access-date=3 September 2022}}</ref> |
|||
[[Acoustic holography]] is a method used to estimate the sound field near a source by measuring acoustic parameters away from the source via an array of pressure and/or particle velocity transducers. Measuring techniques included within acoustic holography are becoming increasingly popular in various fields, most notably those of transportation, vehicle and aircraft design, and NVH. The general idea of acoustic holography has led to different versions such as near-field acoustic holography (NAH) and statistically optimal near-field acoustic holography (SONAH). For audio rendition, the wave field synthesis is the most related procedure. |
|||
Atomic holography has evolved out of the development of the basic elements of [[atom optics]]. With the Fresnel diffraction lens and [[atomic mirror (physics)|atomic mirrors]] atomic holography follows a natural step in the development of the physics (and applications) of atomic beams. Recent developments including [[atomic mirror (physics)|atomic mirrors]] and especially [[ridged mirror]]s have provided the tools necessary for the creation of atomic holograms,<ref name="holo">{{Cite journal| title = Reflection-Type Hologram for Atoms | author = F. Shimizu |author2=J.Fujita |date=March 2002 |journal=[[Physical Review Letters]] |volume=88 | issue = 12 |page=123201 | doi = 10.1103/PhysRevLett.88.123201 | pmid=11909457 | bibcode=2002PhRvL..88l3201S}}</ref> although such holograms have not yet been commercialized. |
|||
[[Neutron]] beam holography has been used to see the inside of solid objects.<ref>{{Cite news|url=https://www.nist.gov/news-events/news/2016/10/move-over-lasers-scientists-can-now-create-holograms-neutrons-too|title=Move Over, Lasers: Scientists Can Now Create Holograms from Neutrons, Too|last=Swenson|first=Gayle|date=2016-10-20|work=NIST|access-date=2017-04-04|language=en}}</ref> |
|||
==Things often confused with holograms== |
|||
Effects produced by [[lenticular printing]], the [[Pepper's Ghost]] illusion (or modern variants such as the [[Musion Eyeliner]]), and [[volumetric displays]] are often confused with holograms.<ref>{{cite web|url=http://www.bbc.co.uk/news/business-12328160 |title=Holographic announcers at Luton airport |publisher=Bbc.co.uk |date=2011-01-31 |accessdate=2012-04-21}}</ref><ref>{{cite web|last=Farivar |first=Cyrus |url=http://arstechnica.com/science/news/2012/04/tupac-hologram-merely-pretty-cool-optical-illusion.ars |title=Tupac "hologram" merely pretty cool optical illusion |publisher=Arstechnica.com |date=2012-04-16 |accessdate=2012-04-21}}</ref> |
|||
Holograms with x-rays are generated by using [[synchrotron]]s or x-ray [[free-electron laser]]s as radiation sources and pixelated detectors such as [[Charge-coupled device|CCDs]] as recording medium.<ref>{{cite journal | last1 = Eisebitt | first1 = S. | display-authors = etal | year = 2004 | title = Lensless imaging of magnetic nanostructures by X-ray spectro-holography | url = https://zenodo.org/record/1233277| journal = Nature | volume = 432 | issue = 7019| pages = 885–888 | doi = 10.1038/nature03139 |bibcode = 2004Natur.432..885E | pmid=15602557| s2cid = 4423853 }}</ref> The reconstruction is then retrieved via computation. Due to the shorter wavelength of [[x-ray]]s compared to visible light, this approach allows imaging objects with higher spatial resolution.<ref>{{cite journal | last1 = Pfau | first1 = B. | display-authors = etal | year = 2014 | title =Influence of stray fields on the switching-field distribution for bit-patterned media based on pre-patterned substrates | url =https://hal.archives-ouvertes.fr/hal-01282859/file/Pfau_APL_2014.pdf | journal = Applied Physics Letters | volume = 105 | issue = 13| page = 132407 | doi = 10.1063/1.4896982 |bibcode = 2014ApPhL.105m2407P | s2cid = 121512138 }}</ref> As [[free-electron laser]]s can provide ultrashort and x-ray pulses in the range of [[femtosecond]]s which are intense and coherent, x-ray holography has been used to capture ultrafast dynamic processes.<ref>{{cite journal | last1 = Chapman | first1 = H. N. | display-authors = etal | year = 2007 | title = Femtosecond time-delay X-ray holography | url = http://bib-pubdb1.desy.de//record/83807/files/Nature-merged.pdf| journal = Nature | volume = 448 | issue = 7154| pages = 676–679 | doi = 10.1038/nature06049 |bibcode = 2007Natur.448..676C | pmid=17687320| s2cid = 4406541 }}</ref><ref>{{cite journal | last1 = Günther | first1 = C.M. | display-authors = etal | year = 2011 | title = Sequential femtosecond X-ray imaging | journal = Nature Photonics | volume = 5 | issue = 2| pages = 99–102 | doi = 10.1038/nphoton.2010.287 |bibcode = 2011NaPho...5...99G }}</ref><ref>{{cite journal | last1 = von Korff | first1 = Schmising | year = 2014 | title = Imaging Ultrafast Demagnetization Dynamics after a Spatially Localized Optical Excitation | url = http://bib-pubdb1.desy.de/record/169124/files/DESY-2014-02806.pdf |display-authors=et al. | journal = Physical Review Letters | volume = 112 | issue = 21| page = 217203 | doi = 10.1103/PhysRevLett.112.217203 | bibcode=2014PhRvL.112u7203V |url-status=live |archive-url= https://web.archive.org/web/20231207161245/https://bib-pubdb1.desy.de/record/169124/files/DESY-2014-02806.pdf |archive-date= Dec 7, 2023 }}</ref> |
|||
The Pepper's ghost technique, being the easiest to implement of these methods, is most prevalent in 3D displays that claim to be (or are referred to as) "holographic". While the original illusion, used in theater, recurred to actual physical objects and persons, located offstage, modern variants replace the source object with a digital screen, which displays imagery generated with [[3D computer graphics]] to provide the necessary [[depth perception|depth cues]]. The reflection, which seems to float mid-air, is still flat, however, thus less realistic than if an actual 3D object was being reflected. |
|||
==False holograms== |
|||
Examples of this digital version of Pepper's ghost illusion include the [[Gorillaz]] performances in the [[2005 MTV Europe Music Awards#Performances|2005 MTV Europe Music Awards]] and the [[48th Grammy Awards#Performances|48th Grammy Awards]]; and [[Tupac Shakur]]'s virtual performance at [[Coachella Valley Music and Arts Festival]] in 2012, rapping alongside Snoop Dogg during the latter's set with Dr. Dre.<ref>{{cite web|url=http://marquee.blogs.cnn.com/2012/04/16/tupac-returns-as-a-hologram-at-coachella/ |title=Tupac returns as a hologram at Coachella |work=The Marquee Blog - CNN.com Blogs |publisher=CNN |date= |accessdate=2012-04-21}}</ref> |
|||
[[File:Pyramid_holographic_3D_holographic_projection_phone_projector_3D_holographic_projection_3D_mobile_phone_naked_eye_3D_pyramid.jpg|thumb|A [[Pepper's ghost]] illusion made from a clear plastic [[frustum]]]] |
|||
[[File:Hatsune Miku - Tell Your World (Live @ Anime Friends 2017).webm|thumb|Shows making using of projected images are erroneously marketed as "holographic"]] |
|||
There are many optical effects that are falsely confused with holography, such as the effects produced by [[lenticular printing]], the [[Pepper's ghost]] illusion (or modern variants such as the [[Musion Eyeliner]]), [[tomography]] and [[volumetric displays]].<ref>{{cite news|url=https://www.bbc.co.uk/news/business-12328160 |title=Holographic announcers at Luton airport |publisher=BBC News |date=2011-01-31 |access-date=2012-04-21}}</ref><ref>{{cite web|last=Farivar |first=Cyrus |url=https://arstechnica.com/science/news/2012/04/tupac-hologram-merely-pretty-cool-optical-illusion.ars |title=Tupac "hologram" merely pretty cool optical illusion |publisher=Ars Technica |date=2012-04-16 |access-date=2012-04-21}}</ref> Such illusions have been called "fauxlography".<ref>{{cite web |url=https://light2015blog.org/2015/09/28/holographic-3d-technology-from-sci-fi-fantasy-to-engineering-reality/ |title=Holographic 3D Technology: From Sci-fi Fantasy to Engineering Reality |date=2015-09-28 |website=International Year of Light Blog |archive-url=https://web.archive.org/web/20171030003249/https://light2015blog.org/2015/09/28/holographic-3d-technology-from-sci-fi-fantasy-to-engineering-reality/ |archive-date=2017-10-30}}</ref><ref>{{cite thesis |type=MFA |last=Gordon |first=Marcus A. |date=2017 |title=Habitat 44º |publisher=OCAD University |doi-access=free |doi=10.13140/RG.2.2.30421.88802}}</ref> |
|||
The Pepper's ghost technique, being the easiest to implement of these methods, is most prevalent in 3D displays that claim to be (or are referred to as) "holographic". While the original illusion, used in theater, involved actual physical objects and persons, located offstage, modern variants replace the source object with a digital screen, which displays imagery generated with [[3D computer graphics]] to provide the necessary [[depth perception|depth cues]]. The reflection, which seems to float mid-air, is still flat however, thus less realistic than if an actual 3D object was being reflected. |
|||
Examples of this digital version of Pepper's ghost illusion include the [[Gorillaz]] performances in the [[2005 MTV Europe Music Awards#Performances|2005 MTV Europe Music Awards]] and the [[48th Grammy Awards#Performances|48th Grammy Awards]]; and [[Tupac Shakur]]'s virtual performance at [[Coachella Valley Music and Arts Festival]] in 2012, rapping alongside [[Snoop Dogg]] during his set with [[Dr. Dre]].<ref>{{cite news|url=http://marquee.blogs.cnn.com/2012/04/16/tupac-returns-as-a-hologram-at-coachella/ |title=Tupac returns as a hologram at Coachella |work=The Marquee Blog |publisher=CNN Blogs |first1=Carolyn |last1=Sung |first2=Topher |last2=Gauk-Roger |first3=Denise |last3=Quan |first4=Jessica |last4=Iavazzi |date= 16 April 2012|access-date=2012-04-21 |url-status=dead |archive-url=https://web.archive.org/web/20120504172454/http://marquee.blogs.cnn.com/2012/04/16/tupac-returns-as-a-hologram-at-coachella/ |archive-date= May 4, 2012 }}</ref> Digital avatars of the Swedish supergroup [[ABBA]] were displayed on stage in May 2022.<ref>{{cite news |last1=Brause |last2=Mills |title=Super Trouper: ABBA returns to stage as virtual avatars for London gigs |url=https://www.reuters.com/lifestyle/super-trouper-abba-returns-stage-virtual-avatars-london-gigs-2022-05-26/ |date=27 May 2022 |work=Reuters |access-date=4 June 2022}}</ref> The ABBA performance used technology that was an updated version of Pepper's Ghost created by [[Industrial Light & Magic]].<ref>{{cite web |title=ABBA's mysterious "Abbatars" revealed |url=https://www.graphicnews.com/en/pages/38425/entertainment-abbas-mysterious-abbatars-revealed-1 |first1=Ninian |last1=Carter |date=November 27, 2018 |website=Graphic News |access-date=4 June 2022}}</ref> American rock group [[Kiss (band)|KISS]] unveiled similar digital avatars in December 2023 to tour in their place at the conclusion of the [[End of the Road World Tour]] using the same Pepper's Ghost technology as the ABBA avatars.<ref>{{cite news |last1=Amorosi |first1=A. D. |title=KISS Says Farewell at Madison Square Garden, Before Passing the Torch to Band's Avatar Successors: Concert Review |url=https://variety.com/2023/music/concert-reviews/kiss-final-concert-review-madison-square-garden-avatars-1235819744/ |access-date=3 December 2023 |work=[[Variety (magazine)|Variety]] |date=3 December 2023}}</ref> |
|||
An even simpler illusion can be created by [[Video projector|rear-projecting]] realistic images into semi-transparent screens. The rear projection is necessary because otherwise the semi-transparency of the screen would allow the background to be illuminated by the projection, which would break the illusion. |
An even simpler illusion can be created by [[Video projector|rear-projecting]] realistic images into semi-transparent screens. The rear projection is necessary because otherwise the semi-transparency of the screen would allow the background to be illuminated by the projection, which would break the illusion. |
||
[[Crypton Future Media]], a music software company that produced [[Hatsune Miku]],<ref>{{cite web|url=http://www.crypton.co.jp/mp/pages/prod/vocaloid/ |title=クリプトン |
[[Crypton Future Media]], a music software company that produced [[Hatsune Miku]],<ref>{{cite web|url=http://www.crypton.co.jp/mp/pages/prod/vocaloid/ |script-title=ja:クリプトン |title=Crypton |publisher=Crypton.co.jp |language=ja |access-date=2012-04-21}}</ref> one of many [[Vocaloid]] singing synthesizer applications, has produced concerts that have Miku, along with other Crypton Vocaloids, performing on stage as "holographic" characters. These concerts use rear projection onto a semi-transparent DILAD screen<ref>{{cite web |last = G. |first = Adrian |title = LA's Anime Expo hosting Hatsune Miku's first US live performance on 2 July |url = http://www.kawaiikakkoiisugoi.com/2011/06/16/las-anime-expo-hosting-hatsune-mikus-first-us-live-performance-on-july-2nd/ |access-date = 20 April 2012 |archive-date = 18 October 2012 |archive-url = https://web.archive.org/web/20121018154249/http://www.kawaiikakkoiisugoi.com/2011/06/16/las-anime-expo-hosting-hatsune-mikus-first-us-live-performance-on-july-2nd/ |url-status = dead }}</ref><ref>{{cite web|url=https://www.youtube.com/watch?v=ZCYJu7KSqQM | archive-url=https://ghostarchive.org/varchive/youtube/20211030/ZCYJu7KSqQM| archive-date=2021-10-30|title="We can invite Hatsune Miku in my room!", Part 2 (video) |publisher=Youtube.com |date=2011-09-07 |access-date=2012-04-21}}{{cbignore}}</ref> to achieve its "holographic" effect.<ref>{{cite web |title = Technically incorrect: Tomorrow's Miley Cyrus? A hologram live in concert! |url = http://news.cnet.com/8301-17852_3-20022743-71.html |access-date = 29 April 2011 }}</ref><ref>{{cite web |title = Hatsune Miku – World is Mine Live in HD |website = [[YouTube]]|url = https://www.youtube.com/watch?v=DTXO7KGHtjI |access-date = 29 April 2011 }}</ref> |
||
In 2011, in Beijing, apparel company [[Burberry]] produced the "Burberry Prorsum Autumn/Winter 2011 Hologram Runway Show", which included life size 2-D projections of models. The company's own video<ref>{{cite web|url=https://www.youtube.com/watch?v=9t5dCIuz2wY | archive-url=https://web.archive.org/web/20111004055249/http://www.youtube.com/watch?v=9t5dCIuz2wY&gl=US&hl=en&has_verified=1| archive-date=2011-10-04|title=Burberry Beijing – Full Show |publisher=Youtube.com |access-date=2012-04-21}}</ref> shows several centered and off-center shots of the main 2-dimensional projection screen, the latter revealing the flatness of the virtual models. The claim that holography was used was reported as fact in the trade media.<ref>{{cite web |url = http://www.vogue.it/en/shows/fashion-events/2011/04/burberry-in-china |title = Burberry lands in China |access-date = 14 June 2011 }}</ref> |
|||
In [[Madrid]], on 10 April 2015, a public visual presentation called "Hologramas por la Libertad" (Holograms for Liberty), featuring a ghostly virtual crowd of demonstrators, was used to protest a new Spanish law that prohibits citizens from demonstrating in public places. Although widely called a "hologram protest" in news reports,<ref>{{cite web |url=http://revolution-news.com/first-hologram-protest-in-history-held-against-spains-gag-law/ |title=First Hologram Protest in History Held Against Spain's Gag Law |publisher=revolution-news.com |access-date=2015-04-13 |url-status=dead |archive-url=https://web.archive.org/web/20150413044945/http://revolution-news.com/first-hologram-protest-in-history-held-against-spains-gag-law/ |archive-date=13 April 2015}}</ref> no actual holography was involved – it was yet another technologically updated variant of the Pepper's ghost illusion. |
|||
Holography is distinct from [[specular holography]] which is a technique for making three-dimensional images by controlling the motion of specularities on a two-dimensional surface.<ref>{{cite web |url=http://www.zintaglio.com/how.html |title=specular holography: how |publisher=Zintaglio.com |access-date=2012-04-21}}</ref> It works by reflectively or refractively manipulating bundles of light rays, not by using interference and diffraction. |
|||
In 2011, in Beijing, apparel company [[Burberry]] produced the "Burberry Prorsum Autumn/Winter 2011 Hologram Runway Show", which included life size 2-D projections of models. The company's own video<ref>{{cite web|author=|url=http://www.youtube.com/watch?v=9t5dCIuz2wY |title=Burberry Beijing - Full Show |publisher=Youtube.com |date= |accessdate=2012-04-21}}</ref> shows several centered and off-center shots of the main 2-dimensional projection screen, the latter revealing the flatness of the virtual models. The claim that holography was used was reported as fact in the trade media.<ref>{{cite web |url = http://www.vogue.it/en/shows/fashion-events/2011/04/burberry-in-china |title = Burberry lands in China |accessdate = June 14, 2011 }}</ref> |
|||
==Tactile holograms== |
|||
==Holography in fiction== |
|||
{{See also|Solid light|Slow light|label 2 = Stopping light}} |
|||
{{Dubious|reason=not appropriate Talk or relevant - see Talk page|date=August 2011}} |
|||
{{See also|Category:Holography in fiction}} |
|||
==In fiction== |
|||
Holograms are often used as [[plot device]]s in [[science fiction]]. |
|||
{{Main|Holography in fiction}} |
|||
Holography has been widely referred to in movies, novels, and TV, usually in [[science fiction]], starting in the late 1970s.<ref name=":0">{{Cite book|title=Holographic Visions: a History of New Science.|url=https://archive.org/details/holographicvisio00john_090|url-access=limited|last=Johnston|first=Sean|date=2006|publisher=Oxford University Press, UK|isbn=978-0191513886|location=Oxford|pages=[https://archive.org/details/holographicvisio00john_090/page/n427 405]–408|chapter=The Hologram and Popular Culture|oclc=437109030}}</ref> Science fiction writers absorbed the [[urban legend]]s surrounding holography that had been spread by overly-enthusiastic scientists and entrepreneurs trying to market the idea.<ref name=":0" /> This had the effect of giving the public overly high expectations of the capability of holography, due to the unrealistic depictions of it in most fiction, where they are fully [[Volumetric display|three-dimensional computer projections]] that are sometimes tactile through the use of [[Force field (fiction)|force fields]].<ref name=":0" /> Examples of this type of depiction include the hologram of [[Princess Leia]] in [[Star Wars (film)|''Star Wars'']], [[Arnold Rimmer]] from ''[[Red Dwarf]]'', who was later converted to "hard light" to make him solid, and the [[Holodeck]] and [[The Doctor (Star Trek: Voyager)|Emergency Medical Hologram]] from ''[[Star Trek]]''.<ref name=":0" /> |
|||
<!-- List arranged by release date --> |
|||
* ''The [[Carpathian Castle]]'' (1893 novel by ''[[Jules Verne]]'') the plot revolves around prima donna La Stilla, represented at the times of the events as a projected image. |
|||
Holography has served as an inspiration for many video games with science fiction elements. In many titles, fictional holographic technology has been used to reflect real life misrepresentations of potential military use of holograms, such as the "mirage tanks" in ''[[Command & Conquer: Red Alert 2]]'' that can disguise themselves as trees.<ref name=":12">{{Cite book|title=Holograms: A Cultural History|last=Johnston|first=Sean F.|publisher=Oxford University Press|year=2015|isbn=978-0191021381|chapter=11 - Channeling Dreams}}</ref> [[Player character]]s are able to use holographic decoys in games such as ''[[Halo: Reach]]'' and ''[[Crysis 2]]'' to confuse and distract the enemy.<ref name=":12" /> ''[[StarCraft|Starcraft]]'' ghost agent Nova has access to "holo decoy" as one of her three primary abilities in ''[[Heroes of the Storm]].<ref>{{Cite web|url=http://us.battle.net/heroes/en/heroes/nova/|title=Nova - Heroes of the Storm|website=us.battle.net|language=en-us|access-date=2019-10-20}}</ref>'' |
|||
* ''[[The Jetsons]]'' (1962-3 television series) uses holograms as entertainment devices, replacing the television in many episodes |
|||
* ''Star Trek: The Animated Series'' (1974 television series) episode "[[The Practical Joker]]", the [[holodeck]] is introduced |
|||
Fictional depictions of holograms have, however, inspired technological advances in other fields, such as [[augmented reality]], that promise to fulfill the fictional depictions of holograms by other means.<ref>{{Cite book|title=The Hologram: Principles and Techniques|last=Richardson|first=Martin|others=Wiltshire, John D.|isbn=978-1119088905|location=Hoboken, NJ|oclc=1000385946|date = 2017-11-13}}</ref> |
|||
* ''[[Star Wars]]'' (1977 film), use of the hologram in the movies and video games of the series to display people remotely communicating with each another |
|||
* ''[[Hello America]]'' (1981 book by ''[[J.G. Ballard]]''), holographic technology is used by president ''Charles Manson'' to scare nomad peoples along the ''United States of America'', showing images of American pop culture icons such as Gary Cooper, Mickey Mouse, or the Enterprise space ship. |
|||
* ''[[Star Trek: The Next Generation]]'' (1987 television series), uses the holodeck extensively; beginning with this series, various episodes and films throughout the ''Star Trek'' series feature holographic characters and ships |
|||
* ''[[Red Dwarf]]'' (1988 television series), after a catastrophic radiation leak inside the Jupiter mining vessel called 'Red Dwarf', crew member Second Technician [[Arnold Rimmer]] is resurrected as a hologram and walks about the ship and planets they encounter. Because he is a "soft-light hologram," he cannot touch anything as objects just pass right through him. However, later in the series he meets 'Legion,' a gestalt entity with advanced technology, who upgrades Rimmer's light bee – the object that projects his hologram by hovering around – changing his projection to what is called in the show "hard-light," thus allowing him to once again touch objects other than computer-generated. |
|||
* ''[[Back to the Future Part II]]'' (1989 film), a giant projection hologram is used as an advertisement for the (fictional) 2015 film ''[[Jaws (franchise)|Jaws]] 19'' |
|||
* ''[[Total Recall]]'' (1990 film), the main character uses a device, similar to a wrist watch, to produce a hologram of himself and deceive his foes |
|||
* ''[[Star Trek: Voyager]]'' (1995–2001 television series) introduced the [[Emergency Medical Hologram]] (EMH) doctor |
|||
* ''[[Yu-Gi-Oh!]]'' (1996–present manga,film,television series,video games), use of holographic technology used in order to make a game called [[Duel Monsters]] appear to be more life like, [[Duel Monsters]] is a game where players using a wrist mounted [[Duel Disk]] summon monsters and cast spells and traps in order to bring a players life points to 0 or diminish all the cards in a players deck. Used throughout the entire series |
|||
* ''[[Stargate: SG-1]]'' (1997–2007 television series), various characters appear as holograms in various episodes: [[Asgard (Stargate)|The Asgard]] masquerade themselves holographically as Norse gods to the primitive peoples under their protection, [[Morgan le Fay (Stargate)|Morgan le Fay]] in "The Pegasus Project" and [[Myrddin (Stargate)|Myrddin]] as a Merlin in "Avalon" and "Camelot" as a [[Ancient technology in Stargate#Holographic sentry|holographic sentry]]; [[Ancient technology in Stargate#Other|Heliopolis "Book"]]; the [[puddle jumper]] starship has a holographic [[heads-up display|HUD]]. After the Goa'uld leader [[Anubis_(Stargate)#Anubis|Anubis]] probed the mind of Asgard leader Thor, he was able to acquire their hologram technology and he used it frequently. |
|||
* ''[[Half-Life (video game)|Half-Life]]'' (1998 video game), the scientific research company Black Mesa is known to use holograms as recorded messages in their facility. |
|||
* ''[[Lost in Space (film)|Lost in Space]]'' (1998 film), [[June Lockhart]] (Maureen Robinson) appeared as Will's school principal "Cartwright" in a hologram |
|||
* ''[[Power Rangers Time Force]]'' (2001 series), their chrono morphers use holographic communication. |
|||
* ''[[Halo (series)]]'' (2001 video game) uses "holotanks" to display the avatar of an artificial intelligence construct. In Halo: Reach, an Armor Ability called the hologram allows the user to create an identical decoy. |
|||
* ''[[The First $20 Million Is Always the Hardest]]'' (2002 film) Computer geeks develop a $99 computer using a holographic projector as both the display and user interface. |
|||
* ''[[Treasure Planet]]'' (2002 film) Jim as a little boy reads from a 3D hologram book the story about Captain Flint and Treasure Planet. Later Jim as a teenager finds a sphere map and uses it to look at the galaxy map to Treasure Planet. |
|||
* ''[[Pinocchio 3000]]'' (2004 film) Mayor Scamboli owns a 3-D hologram map on his table. Cabby and Roto change channels on it. Later at Scamboland, Mayor Scamboli welcomes kids as a giant 3-D hologram version for Scamboland carnival opening. |
|||
* ''[[Stargate: Atlantis]]'' (2004–2009 television series), the [[Atlantis (Stargate)#Areas|Atlantis]] city-starship features a hologram room that allows access to the Ancient database in the form of holograms; an [[Ancient technology in Stargate#Control Chair|Ancient Control Chair]] contains holographic projectors; in the episode "Rising", Melia (a member of the Atlantean High Council during the first siege of Atlantis some ten millennia ago) is first seen as a hologram describing the history of the Ancients in the Pegasus Galaxy; [[Aurora-class battleship]] can project holograms remotely for communication purposes |
|||
* ''[[The Island (2005 film)|The Island]]'' (2005 film), a holographic projector surrounded the military compound where clones were kept to give the illusion of a tropical environment; holographic displays are present on various terminals, including the MSN information terminal in Los Angeles |
|||
* ''[[Meet the Robinsons]]'' (2007 film), Bowler Hat Michael Goob Yagoobian has a discussion with the Bowler Hat Robot about getting revenge and Bowler Hat robot shows him a 3-D hologram image of a flying car-plane time machine. |
|||
* ''[[Dead Space (video game)|Dead Space]]'' (2008 video game), to replace the player's HUD, a holographic display shows up in front of the player's character |
|||
* ''[[Avatar (2009 film)|Avatar]]'' (2009 film), holographic displays are used extensively on terminals and HUDs |
|||
* ''[[G.I. Joe: The Rise of Cobra]]'' a 2009 live-action movie |
|||
* ''[[Iron Man (film)|Iron Man]]'' and ''[[Iron Man 2]]'', in the 2008 and 2010 films, holographic displays appear in the titular character's suit. |
|||
* ''[[Enthiran]]'' (2010 film), Chitti, the robot, can be telecommunicated with using a "virtual calling" where each caller can be seen as a holographic projection in front of the robot during the call |
|||
* Computer GUIs in [[Mass Effect (series)|Mass Effect]] are explained in the codex to consist of a projected holographic display, combined with the use of '[[Haptic technology|force feedback]]' gloves that allow the user to experience simulated tactile sensations when manipulating them. |
|||
==See also== |
==See also== |
||
{{ |
{{cols|colwidth=21em}} |
||
* [[List of file formats#3D graphics|3D file formats]] |
|||
* [[Computer-generated holography]] |
|||
* [[Holographic display]] |
|||
* [[Augmented reality]] |
|||
* [[Australian Holographics]] |
* [[Australian Holographics]] |
||
* [[Autostereoscopy]] |
* [[Autostereoscopy]] |
||
* [[Computer-generated holography]] |
|||
* [[Digital holography]] |
* [[Digital holography]] |
||
* [[Digital holographic microscopy]] |
|||
* [[Digital planar holography]] |
* [[Digital planar holography]] |
||
* [[Fog display]] |
|||
* [[Holographic principle]] |
* [[Holographic principle]] |
||
* [[Holonomic brain theory]] |
* [[Holonomic brain theory]] |
||
* [[Hogel Processing Unit]] |
|||
* [[Integral imaging]] |
* [[Integral imaging]] |
||
* [[List of emerging technologies]] |
* [[List of emerging technologies]] |
||
* [[Phase-coherent holography]] |
* [[Phase-coherent holography]] |
||
* [[Plasmon#Possible applications|Plasmon |
* [[Plasmon#Possible applications|Plasmon – possible applications]] (full color holography) |
||
* [[Tomography]] |
* [[Tomography]] |
||
* [[Volumetric display]] |
|||
{{div col end}} |
|||
* [[Volumetric printing]] |
|||
{{colend}} |
|||
==References== |
==References== |
||
{{Reflist|30em}} |
{{Reflist|30em}} |
||
==Bibliography== |
|||
==Reference sources== |
|||
{{Refbegin}} |
{{Refbegin}} |
||
*Hariharan P, 1996, Optical Holography, Cambridge University Press, ISBN |
* Hariharan P, 1996, Optical Holography, Cambridge University Press, {{ISBN|0-521-43965-5}} |
||
*Hariharan P, 2002, Basics of Holography, Cambridge University Press, ISBN |
* Hariharan P, 2002, Basics of Holography, Cambridge University Press, {{ISBN|0-521-00200-1}} |
||
*Lipson A., Lipson SG, Lipson H, Optical Physics, 2011, Cambridge University Press, ISBN |
* Lipson A., Lipson SG, Lipson H, Optical Physics, 2011, Cambridge University Press, {{ISBN|978-0-521-49345-1}} |
||
{{Refend}} |
{{Refend}} |
||
==Further reading== |
==Further reading== |
||
{{Refbegin|30em}} |
{{Refbegin|30em}} |
||
* ''Lasers and holography: an introduction to coherent optics'' W. E. Kock, Dover Publications (1981), ISBN |
* ''Lasers and holography: an introduction to coherent optics'' W. E. Kock, Dover Publications (1981), {{ISBN|978-0-486-24041-1}} |
||
* ''Principles of holography'' H. M. Smith, Wiley (1976), ISBN |
* ''Principles of holography'' H. M. Smith, Wiley (1976), {{ISBN|978-0-471-80341-6}} |
||
* G. Berger et al., ''Digital Data Storage in a phase-encoded |
* G. Berger et al., ''Digital Data Storage in a phase-encoded holographic memory system: data quality and security'', Proceedings of SPIE, Vol. 4988, pp. 104–111 (2003) |
||
* ''Holographic Visions: A History of New Science'' Sean F. Johnston, Oxford University Press (2006), ISBN |
* ''Holographic Visions: A History of New Science'' Sean F. Johnston, Oxford University Press (2006), {{ISBN|0-19-857122-4}} |
||
* {{Cite book|title = Practical Holography, Third Edition|last = Saxby|first = Graham|year = 2003|publisher = Taylor and Francis|isbn = 978-0-7503-0912-7}} |
* {{Cite book|title = Practical Holography, Third Edition|last = Saxby|first = Graham|year = 2003|publisher = Taylor and Francis|isbn = 978-0-7503-0912-7}} |
||
* ''Three-Dimensional Imaging Techniques'' Takanori Okoshi, Atara Press (2011), ISBN |
* ''Three-Dimensional Imaging Techniques'' Takanori Okoshi, Atara Press (2011), {{ISBN|978-0-9822251-4-1}} |
||
* ''Holographic Microscopy of Phase Microscopic Objects: Theory and Practice'' Tatyana Tishko, Tishko Dmitry, Titar Vladimir, World Scientific (2010), ISBN |
* ''Holographic Microscopy of Phase Microscopic Objects: Theory and Practice'' Tatyana Tishko, Tishko Dmitry, Titar Vladimir, World Scientific (2010), {{ISBN|978-981-4289-54-2}} |
||
* {{cite book|title=The Hologram: Principles and Techniques|editor-first1=Martin J. |editor-last1=Richardson |editor-first2=John D.|editor-last2=Wiltshire|publisher=Wiley|year=2017|isbn=9781119088905|oclc=1000385946|doi=10.1002/9781119088929|last1=Richardson|first1=Martin J.|last2=Wiltshire|first2=John D.|bibcode=2017hpt..book.....R }} |
|||
{{Refend}} |
{{Refend}} |
||
Line 447: | Line 291: | ||
==External links== |
==External links== |
||
{{Commons category|Holography}} |
{{Commons category|Holography}} |
||
* "[https://web.archive.org/web/20041204092005/http://nobelprize.org/physics/laureates/1971/gabor-autobio.html Dennis Gabor – Autobiography]", 30 September 2004, Nobelprize.org |
|||
* [http://www.ihma.org International Hologram Manufacturers Association] |
|||
* |
**"[https://www.nobelprize.org/uploads/2018/06/gabor-lecture.pdf Holography, 1948-1971 Nobel Lecture]", 11 December 1971, by Dennis Gabor |
||
* "[http://science.howstuffworks.com/hologram.htm How Holograms Work]", How Stuff Works, by Tracy V. Wilson, 30 August 2023 |
|||
* [http://www.media.mit.edu/spi/ MIT's Spatial Imaging Group with papers about holographic theory and Holographic video] |
|||
* "[http://qed.wikina.org/holography/ Holography]" by The Strange Theory of Light, QED |
|||
* [http://www.integraf.com/a-holography_medical_applications.htm Medical Applications of Holograms] |
|||
* "[https://youtube.com/watch?v=aTB2ryoWIFU&t=459 Making Real Holograms!!!!!!]" at [[YouTube]] by The Thought Emporium, 19 November 2020 |
|||
* [http://science.howstuffworks.com/hologram.htm How Stuff Works – holograms] |
|||
* Walker, John. (1992) [http://www.artdesigncafe.com/holographic-art-1992 "Holographic Art"]. ''Glossary of Art, Architecture & Design since 1945'', 3rd. ed. |
|||
* [http://holocenter.org Center for the Holographic Arts, New York – a non-profit organisation promoting holography] |
|||
* [http://www.zintaglio.com Specular holography art site] |
|||
* [http://news.bbc.co.uk/2/hi/technology/7230258.stm Faster way to produce holographic tiles] |
|||
* [http://amasci.com/amateur/holo1.html Abrasion, hand-drawn holograms] |
|||
* [http://holoforum.org/forum Holoforum – A place to discuss holography] |
|||
* [http://qed.wikina.org/holography/ Animations demonstrating holography] by QED |
|||
* {{US patent|3506327}} — "''Wavefront reconstruction using a coherent reference beam''" — E. N. Leith et al. |
|||
{{Display technology}} |
{{Display technology}} |
||
{{photography subject}} |
{{photography subject}} |
||
{{ |
{{emerging technologies|displays=yes}} |
||
{{Stereoscopy}} |
{{Stereoscopy}} |
||
{{Use dmy dates|date=May 2011}} |
|||
{{Authority control}} |
|||
[[Category:Holography| ]] |
[[Category:Holography| ]] |
||
[[Category:British inventions]] |
[[Category:British inventions]] |
||
[[Category:Emerging technologies]] |
|||
[[Category:Hungarian inventions]] |
[[Category:Hungarian inventions]] |
||
[[Category:Laser image generation]] |
[[Category:Laser image generation]] |
||
[[Category:Photographic techniques]] |
[[Category:Photographic techniques]] |
||
[[Category:3D imaging]] |
[[Category:3D imaging]] |
||
[[Category:Articles containing video clips]] |
|||
[[af:Holografie]] |
|||
[[als:Holografie]] |
|||
[[ar:تصوير تجسيمي]] |
|||
[[bg:Холография]] |
|||
[[bs:Holografija]] |
|||
[[ca:Holografia]] |
|||
[[cs:Holografie]] |
|||
[[de:Holografie]] |
|||
[[es:Holografía]] |
|||
[[eo:Holografio]] |
|||
[[eu:Holografia]] |
|||
[[fa:تمامنگاری]] |
|||
[[fr:Holographie]] |
|||
[[gl:Holografía]] |
|||
[[ko:홀로그래피]] |
|||
[[hi:होलोग्राफी]] |
|||
[[hr:Holografija]] |
|||
[[id:Holografi]] |
|||
[[it:Olografia]] |
|||
[[he:הולוגרפיה]] |
|||
[[kn:ಪ್ರಕಾಶ ವಿಜ್ಞಾನ]] |
|||
[[kk:Голоографиялық акпараттық жүйе]] |
|||
[[lv:Hologrāfija]] |
|||
[[lt:Holografija]] |
|||
[[hu:Holográfia]] |
|||
[[mk:Холографија]] |
|||
[[ml:ഹോളോഗ്രഫി]] |
|||
[[nl:Holografie]] |
|||
[[ja:ホログラフィー]] |
|||
[[no:Holografi]] |
|||
[[pl:Holografia]] |
|||
[[pt:Holografia]] |
|||
[[ro:Holografie]] |
|||
[[ru:Голография]] |
|||
[[simple:Holography]] |
|||
[[sk:Holografia]] |
|||
[[sl:Holografija]] |
|||
[[sr:Холографија]] |
|||
[[fi:Holografia]] |
|||
[[sv:Holografi]] |
|||
[[ta:முப்பரிமாண ஒளிப்படவியல்]] |
|||
[[th:ฮอโลกราฟี]] |
|||
[[tr:Holografi]] |
|||
[[uk:Голографія]] |
|||
[[war:Holograpiya]] |
|||
[[zh:全息摄影]] |
Latest revision as of 16:05, 22 December 2024
Holography is a technique that enables a wavefront to be recorded and later reconstructed. It is best known as a method of generating three-dimensional images, and has a wide range of other uses, including data storage, microscopy, and interferometry. In principle, it is possible to make a hologram for any type of wave.
A hologram is a recording of an interference pattern that can reproduce a 3D light field using diffraction. In general usage, a hologram is a recording of any type of wavefront in the form of an interference pattern. It can be created by capturing light from a real scene, or it can be generated by a computer, in which case it is known as a computer-generated hologram, which can show virtual objects or scenes. Optical holography needs a laser light to record the light field. The reproduced light field can generate an image that has the depth and parallax of the original scene.[1] A hologram is usually unintelligible when viewed under diffuse ambient light. When suitably lit, the interference pattern diffracts the light into an accurate reproduction of the original light field, and the objects that were in it exhibit visual depth cues such as parallax and perspective that change realistically with the different angles of viewing. That is, the view of the image from different angles shows the subject viewed from similar angles.
A hologram is traditionally generated by overlaying a second wavefront, known as the reference beam, onto a wavefront of interest. This generates an interference pattern, which is then captured on a physical medium. When the recorded interference pattern is later illuminated by the second wavefront, it is diffracted to recreate the original wavefront.[2] The 3D image from a hologram can often be viewed with non-laser light. However, in common practice, major image quality compromises are made to remove the need for laser illumination to view the hologram.
A computer-generated hologram is created by digitally modeling and combining two wavefronts to generate an interference pattern image. This image can then be printed onto a mask or film and illuminated with an appropriate light source to reconstruct the desired wavefront.[2] Alternatively, the interference pattern image can be directly displayed on a dynamic holographic display.[3]
Holographic portraiture often resorts to a non-holographic intermediate imaging procedure, to avoid the dangerous high-powered pulsed lasers which would be needed to optically "freeze" moving subjects as perfectly as the extremely motion-intolerant holographic recording process requires. Early holography required high-power and expensive lasers. Currently, mass-produced low-cost laser diodes, such as those found on DVD recorders and used in other common applications, can be used to make holograms. They have made holography much more accessible to low-budget researchers, artists, and dedicated hobbyists.
Most holograms produced are of static objects, but systems for displaying changing scenes on dynamic holographic displays are now being developed.[4][5]
The word holography comes from the Greek words ὅλος (holos; "whole") and γραφή (graphē; "writing" or "drawing").
History
[edit]The Hungarian-British physicist Dennis Gabor invented holography in 1948 while he was looking for a way to improve image resolution in electron microscopes.[6][7][8] Gabor's work was built on pioneering work in the field of X-ray microscopy by other scientists including Mieczysław Wolfke in 1920 and William Lawrence Bragg in 1939.[9] The formulation of holography was an unexpected result of Gabor's research into improving electron microscopes at the British Thomson-Houston Company (BTH) in Rugby, England, and the company filed a patent in December 1947 (patent GB685286). The technique as originally invented is still used in electron microscopy, where it is known as electron holography. Gabor was awarded the Nobel Prize in Physics in 1971 "for his invention and development of the holographic method".[10]
Optical holography did not really advance until the development of the laser in 1960. The development of the laser enabled the first practical optical holograms that recorded 3D objects to be made in 1962 by Yuri Denisyuk in the Soviet Union[11] and by Emmett Leith and Juris Upatnieks at the University of Michigan, US.[12]
Early optical holograms used silver halide photographic emulsions as the recording medium. They were not very efficient as the produced diffraction grating absorbed much of the incident light. Various methods of converting the variation in transmission to a variation in refractive index (known as "bleaching") were developed which enabled much more efficient holograms to be produced.[13][14][15]
A major advance in the field of holography was made by Stephen Benton, who invented a way to create holograms that can be viewed with natural light instead of lasers. These are called rainbow holograms.[8]
Basics of holography
[edit]Holography is a technique for recording and reconstructing light fields.[16]: Section 1 A light field is generally the result of a light source scattered off objects. Holography can be thought of as somewhat similar to sound recording, whereby a sound field created by vibrating matter like musical instruments or vocal cords, is encoded in such a way that it can be reproduced later, without the presence of the original vibrating matter.[17] However, it is even more similar to Ambisonic sound recording in which any listening angle of a sound field can be reproduced in the reproduction.
Laser
[edit]In laser holography, the hologram is recorded using a source of laser light, which is very pure in its color and orderly in its composition. Various setups may be used, and several types of holograms can be made, but all involve the interaction of light coming from different directions and producing a microscopic interference pattern which a plate, film, or other medium photographically records.
In one common arrangement, the laser beam is split into two, one known as the object beam and the other as the reference beam. The object beam is expanded by passing it through a lens and used to illuminate the subject. The recording medium is located where this light, after being reflected or scattered by the subject, will strike it. The edges of the medium will ultimately serve as a window through which the subject is seen, so its location is chosen with that in mind. The reference beam is expanded and made to shine directly on the medium, where it interacts with the light coming from the subject to create the desired interference pattern.
Like conventional photography, holography requires an appropriate exposure time to correctly affect the recording medium. Unlike conventional photography, during the exposure the light source, the optical elements, the recording medium, and the subject must all remain motionless relative to each other, to within about a quarter of the wavelength of the light, or the interference pattern will be blurred and the hologram spoiled. With living subjects and some unstable materials, that is only possible if a very intense and extremely brief pulse of laser light is used, a hazardous procedure which is rarely done outside of scientific and industrial laboratory settings. Exposures lasting several seconds to several minutes, using a much lower-powered continuously operating laser, are typical.
Apparatus
[edit]A hologram can be made by shining part of the light beam directly into the recording medium, and the other part onto the object in such a way that some of the scattered light falls onto the recording medium. A more flexible arrangement for recording a hologram requires the laser beam to be aimed through a series of elements that change it in different ways. The first element is a beam splitter that divides the beam into two identical beams, each aimed in different directions:
- One beam (known as the 'illumination' or 'object beam') is spread using lenses and directed onto the scene using mirrors. Some of the light scattered (reflected) from the scene then falls onto the recording medium.
- The second beam (known as the 'reference beam') is also spread through the use of lenses, but is directed so that it does not come in contact with the scene, and instead travels directly onto the recording medium.
Several different materials can be used as the recording medium. One of the most common is a film very similar to photographic film (silver halide photographic emulsion), but with much smaller light-reactive grains (preferably with diameters less than 20 nm), making it capable of the much higher resolution that holograms require. A layer of this recording medium (e.g., silver halide) is attached to a transparent substrate, which is commonly glass, but may also be plastic.
Process
[edit]When the two laser beams reach the recording medium, their light waves intersect and interfere with each other. It is this interference pattern that is imprinted on the recording medium. The pattern itself is seemingly random, as it represents the way in which the scene's light interfered with the original light source – but not the original light source itself. The interference pattern can be considered an encoded version of the scene, requiring a particular key – the original light source – in order to view its contents.
This missing key is provided later by shining a laser, identical to the one used to record the hologram, onto the developed film. When this beam illuminates the hologram, it is diffracted by the hologram's surface pattern. This produces a light field identical to the one originally produced by the scene and scattered onto the hologram.
Comparison with photography
[edit]Holography may be better understood via an examination of its differences from ordinary photography:
- A hologram represents a recording of information regarding the light that came from the original scene as scattered in a range of directions rather than from only one direction, as in a photograph. This allows the scene to be viewed from a range of different angles, as if it were still present.
- A photograph can be recorded using normal light sources (sunlight or electric lighting) whereas a laser is required to record a hologram.
- A lens is required in photography to record the image, whereas in holography, the light from the object is scattered directly onto the recording medium.
- A holographic recording requires a second light beam (the reference beam) to be directed onto the recording medium.
- A photograph can be viewed in a wide range of lighting conditions, whereas holograms can only be viewed with very specific forms of illumination.
- When a photograph is cut in half, each piece shows half of the scene. When a hologram is cut in half, the whole scene can still be seen in each piece. This is because, whereas each point in a photograph only represents light scattered from a single point in the scene, each point on a holographic recording includes information about light scattered from every point in the scene. It can be thought of as viewing a street outside a house through a large window, then through a smaller window. One can see all of the same things through the smaller window (by moving the head to change the viewing angle), but the viewer can see more at once through the large window.
- A photographic stereogram is a two-dimensional representation that can produce a three-dimensional effect but only from one point of view, whereas the reproduced viewing range of a hologram adds many more depth perception cues that were present in the original scene. These cues are recognized by the human brain and translated into the same perception of a three-dimensional image as when the original scene might have been viewed.
- A photograph clearly maps out the light field of the original scene. The developed hologram's surface consists of a very fine, seemingly random pattern, which appears to bear no relationship to the scene it recorded.
Physics of holography
[edit]For a better understanding of the process, it is necessary to understand interference and diffraction. Interference occurs when one or more wavefronts are superimposed. Diffraction occurs when a wavefront encounters an object. The process of producing a holographic reconstruction is explained below purely in terms of interference and diffraction. It is somewhat simplified but is accurate enough to give an understanding of how the holographic process works.
For those unfamiliar with these concepts, it is worthwhile to read those articles before reading further in this article.
Plane wavefronts
[edit]A diffraction grating is a structure with a repeating pattern. A simple example is a metal plate with slits cut at regular intervals. A light wave that is incident on a grating is split into several waves; the direction of these diffracted waves is determined by the grating spacing and the wavelength of the light.
A simple hologram can be made by superimposing two plane waves from the same light source on a holographic recording medium. The two waves interfere, giving a straight-line fringe pattern whose intensity varies sinusoidally across the medium. The spacing of the fringe pattern is determined by the angle between the two waves, and by the wavelength of the light.
The recorded light pattern is a diffraction grating. When it is illuminated by only one of the waves used to create it, it can be shown that one of the diffracted waves emerges at the same angle at which the second wave was originally incident, so that the second wave has been 'reconstructed'. Thus, the recorded light pattern is a holographic recording as defined above.
Point sources
[edit]If the recording medium is illuminated with a point source and a normally incident plane wave, the resulting pattern is a sinusoidal zone plate, which acts as a negative Fresnel lens whose focal length is equal to the separation of the point source and the recording plane.
When a plane wave-front illuminates a negative lens, it is expanded into a wave that appears to diverge from the focal point of the lens. Thus, when the recorded pattern is illuminated with the original plane wave, some of the light is diffracted into a diverging beam equivalent to the original spherical wave; a holographic recording of the point source has been created.
When the plane wave is incident at a non-normal angle at the time of recording, the pattern formed is more complex, but still acts as a negative lens if it is illuminated at the original angle.
Complex objects
[edit]To record a hologram of a complex object, a laser beam is first split into two beams of light. One beam illuminates the object, which then scatters light onto the recording medium. According to diffraction theory, each point in the object acts as a point source of light so the recording medium can be considered to be illuminated by a set of point sources located at varying distances from the medium.
The second (reference) beam illuminates the recording medium directly. Each point source wave interferes with the reference beam, giving rise to its own sinusoidal zone plate in the recording medium. The resulting pattern is the sum of all these 'zone plates', which combine to produce a random (speckle) pattern as in the photograph above.
When the hologram is illuminated by the original reference beam, each of the individual zone plates reconstructs the object wave that produced it, and these individual wavefronts are combined to reconstruct the whole of the object beam. The viewer perceives a wavefront that is identical with the wavefront scattered from the object onto the recording medium, so that it appears that the object is still in place even if it has been removed.
Applications
[edit]Art
[edit]Early on, artists saw the potential of holography as a medium and gained access to science laboratories to create their work. Holographic art is often the result of collaborations between scientists and artists, although some holographers would regard themselves as both an artist and a scientist.
Salvador Dalí claimed to have been the first to employ holography artistically. He was certainly the first and best-known surrealist to do so, but the 1972 New York exhibit of Dalí holograms had been preceded by the holographic art exhibition that was held at the Cranbrook Academy of Art in Michigan in 1968 and by the one at the Finch College gallery in New York in 1970, which attracted national media attention.[18] In Great Britain, Margaret Benyon began using holography as an artistic medium in the late 1960s and had a solo exhibition at the University of Nottingham art gallery in 1969.[19] This was followed in 1970 by a solo show at the Lisson Gallery in London, which was billed as the "first London expo of holograms and stereoscopic paintings".[20]
During the 1970s, a number of art studios and schools were established, each with their particular approach to holography. Notably, there was the San Francisco School of Holography established by Lloyd Cross, The Museum of Holography in New York founded by Rosemary (Posy) H. Jackson, the Royal College of Art in London and the Lake Forest College Symposiums organised by Tung Jeong.[21] None of these studios still exist; however, there is the Center for the Holographic Arts in New York[22] and the HOLOcenter in Seoul, which offers artists a place to create and exhibit work.
During the 1980s, many artists who worked with holography helped the diffusion of this so-called "new medium" in the art world, such as Harriet Casdin-Silver of the United States, Dieter Jung of Germany, and Moysés Baumstein of Brazil, each one searching for a proper "language" to use with the three-dimensional work, avoiding the simple holographic reproduction of a sculpture or object. For instance, in Brazil, many concrete poets (Augusto de Campos, Décio Pignatari, Julio Plaza and José Wagner Garcia, associated with Moysés Baumstein) found in holography a way to express themselves and to renew Concrete Poetry.
A small but active group of artists still integrate holographic elements into their work.[23] Some are associated with novel holographic techniques; for example, artist Matt Brand[24] employed computational mirror design to eliminate image distortion from specular holography.
The MIT Museum[25] and Jonathan Ross[26] both have extensive collections of holography and on-line catalogues of art holograms.
Data storage
[edit]Holographic data storage is a technique that can store information at high density inside crystals or photopolymers. The ability to store large amounts of information in some kind of medium is of great importance, as many electronic products incorporate storage devices. As current storage techniques such as Blu-ray Disc reach the limit of possible data density (due to the diffraction-limited size of the writing beams), holographic storage has the potential to become the next generation of popular storage media. The advantage of this type of data storage is that the volume of the recording media is used instead of just the surface. Currently available SLMs can produce about 1000 different images a second at 1024×1024-bit resolution which would result in about one-gigabit-per-second writing speed.[27]
In 2005, companies such as Optware and Maxell produced a 120 mm disc that uses a holographic layer to store data to a potential 3.9 TB, a format called Holographic Versatile Disc. As of September 2014, no commercial product has been released.
Another company, InPhase Technologies, was developing a competing format, but went bankrupt in 2011 and all its assets were sold to Akonia Holographics, LLC.
While many holographic data storage models have used "page-based" storage, where each recorded hologram holds a large amount of data, more recent research into using submicrometre-sized "microholograms" has resulted in several potential 3D optical data storage solutions. While this approach to data storage can not attain the high data rates of page-based storage, the tolerances, technological hurdles, and cost of producing a commercial product are significantly lower.
Dynamic holography
[edit]In static holography, recording, developing and reconstructing occur sequentially, and a permanent hologram is produced.
There also exist holographic materials that do not need the developing process and can record a hologram in a very short time. This allows one to use holography to perform some simple operations in an all-optical way. Examples of applications of such real-time holograms include phase-conjugate mirrors ("time-reversal" of light), optical cache memories, image processing (pattern recognition of time-varying images), and optical computing.
The amount of processed information can be very high (terabits/s), since the operation is performed in parallel on a whole image. This compensates for the fact that the recording time, which is in the order of a microsecond, is still very long compared to the processing time of an electronic computer. The optical processing performed by a dynamic hologram is also much less flexible than electronic processing. On one side, one has to perform the operation always on the whole image, and on the other side, the operation a hologram can perform is basically either a multiplication or a phase conjugation. In optics, addition and Fourier transform are already easily performed in linear materials, the latter simply by a lens. This enables some applications, such as a device that compares images in an optical way.[28]
The search for novel nonlinear optical materials for dynamic holography is an active area of research. The most common materials are photorefractive crystals, but in semiconductors or semiconductor heterostructures (such as quantum wells), atomic vapors and gases, plasmas and even liquids, it was possible to generate holograms.
A particularly promising application is optical phase conjugation. It allows the removal of the wavefront distortions a light beam receives when passing through an aberrating medium, by sending it back through the same aberrating medium with a conjugated phase. This is useful, for example, in free-space optical communications to compensate for atmospheric turbulence (the phenomenon that gives rise to the twinkling of starlight).
Hobbyist use
[edit]Since the beginning of holography, many holographers have explored its uses and displayed them to the public.
In 1971, Lloyd Cross opened the San Francisco School of Holography and taught amateurs how to make holograms using only a small (typically 5 mW) helium-neon laser and inexpensive home-made equipment. Holography had been supposed to require a very expensive metal optical table set-up to lock all the involved elements down in place and damp any vibrations that could blur the interference fringes and ruin the hologram. Cross's home-brew alternative was a sandbox made of a cinder block retaining wall on a plywood base, supported on stacks of old tires to isolate it from ground vibrations, and filled with sand that had been washed to remove dust. The laser was securely mounted atop the cinder block wall. The mirrors and simple lenses needed for directing, splitting and expanding the laser beam were affixed to short lengths of PVC pipe, which were stuck into the sand at the desired locations. The subject and the photographic plate holder were similarly supported within the sandbox. The holographer turned off the room light, blocked the laser beam near its source using a small relay-controlled shutter, loaded a plate into the holder in the dark, left the room, waited a few minutes to let everything settle, then made the exposure by remotely operating the laser shutter.
In 1979, Jason Sapan opened the Holographic Studios in New York City. Since then, they have been involved in the production of many holographs for many artists as well as companies.[29] Sapan has been described as the "last professional holographer of New York".
Many of these holographers would go on to produce art holograms. In 1983, Fred Unterseher, a co-founder of the San Francisco School of Holography and a well-known holographic artist, published the Holography Handbook, an easy-to-read guide to making holograms at home. This brought in a new wave of holographers and provided simple methods for using the then-available AGFA silver halide recording materials.
In 2000, Frank DeFreitas published the Shoebox Holography Book and introduced the use of inexpensive laser pointers to countless hobbyists. For many years, it had been assumed that certain characteristics of semiconductor laser diodes made them virtually useless for creating holograms, but when they were eventually put to the test of practical experiment, it was found that not only was this untrue, but that some actually provided a coherence length much greater than that of traditional helium-neon gas lasers. This was a very important development for amateurs, as the price of red laser diodes had dropped from hundreds of dollars in the early 1980s to about $5 after they entered the mass market as a component pulled from CD, or later, DVD players from the mid 1980s onwards. Now, there are thousands of amateur holographers worldwide.
By late 2000, holography kits with inexpensive laser pointer diodes entered the mainstream consumer market. These kits enabled students, teachers, and hobbyists to make several kinds of holograms without specialized equipment, and became popular gift items by 2005.[30] The introduction of holography kits with self-developing plates in 2003 made it possible for hobbyists to create holograms without the bother of wet chemical processing.[31]
In 2006, a large number of surplus holography-quality green lasers (Coherent C315) became available and put dichromated gelatin (DCG) holography within the reach of the amateur holographer. The holography community was surprised at the amazing sensitivity of DCG to green light. It had been assumed that this sensitivity would be uselessly slight or non-existent. Jeff Blyth responded with the G307 formulation of DCG to increase the speed and sensitivity to these new lasers.[32]
Kodak and Agfa, the former major suppliers of holography-quality silver halide plates and films, are no longer in the market. While other manufacturers have helped fill the void, many amateurs are now making their own materials. The favorite formulations are dichromated gelatin, Methylene-Blue-sensitised dichromated gelatin, and diffusion method silver halide preparations. Jeff Blyth has published very accurate methods for making these in a small lab or garage.[33]
A small group of amateurs are even constructing their own pulsed lasers to make holograms of living subjects and other unsteady or moving objects.[34]
Holographic interferometry
[edit]Holographic interferometry (HI) is a technique that enables static and dynamic displacements of objects with optically rough surfaces to be measured to optical interferometric precision (i.e. to fractions of a wavelength of light).[35][36] It can also be used to detect optical-path-length variations in transparent media, which enables, for example, fluid flow to be visualized and analyzed. It can also be used to generate contours representing the form of the surface or the isodose regions in radiation dosimetry.[37]
It has been widely used to measure stress, strain, and vibration in engineering structures.
Interferometric microscopy
[edit]The hologram keeps the information on the amplitude and phase of the field. Several holograms may keep information about the same distribution of light, emitted to various directions. The numerical analysis of such holograms allows one to emulate large numerical aperture, which, in turn, enables enhancement of the resolution of optical microscopy. The corresponding technique is called interferometric microscopy. Recent achievements of interferometric microscopy allow one to approach the quarter-wavelength limit of resolution.[38]
Sensors or biosensors
[edit]The hologram is made with a modified material that interacts with certain molecules generating a change in the fringe periodicity or refractive index, therefore, the color of the holographic reflection.[39][40]
Security
[edit]Holograms are commonly used for security, as they are replicated from a master hologram that requires expensive, specialized and technologically advanced equipment, and are thus difficult to forge. They are used widely in many currencies, such as the Brazilian 20, 50, and 100-reais notes; British 5, 10, 20 and 50-pound notes; South Korean 5000, 10,000, and 50,000-won notes; Japanese 5000 and 10,000 yen notes, Indian 50, 100, 500, and 2000 rupee notes; and all the currently-circulating banknotes of the Canadian dollar, Croatian kuna, Danish krone, and Euro. They can also be found in credit and bank cards as well as passports, ID cards, books, food packaging, DVDs, and sports equipment. Such holograms come in a variety of forms, from adhesive strips that are laminated on packaging for fast-moving consumer goods to holographic tags on electronic products. They often contain textual or pictorial elements to protect identities and separate genuine articles from counterfeits.
Holographic scanners are in use in post offices, larger shipping firms, and automated conveyor systems to determine the three-dimensional size of a package. They are often used in tandem with checkweighers to allow automated pre-packing of given volumes, such as a truck or pallet for bulk shipment of goods. Holograms produced in elastomers can be used as stress-strain reporters due to its elasticity and compressibility, the pressure and force applied are correlated to the reflected wavelength, therefore its color.[41] Holography technique can also be effectively used for radiation dosimetry.[42][43]
High security registration plates
[edit]High-security holograms can be used on license plates for vehicles such as cars and motorcycles. As of April 2019, holographic license plates are required on vehicles in parts of India to aid in identification and security, especially in cases of car theft. Such number plates hold electronic data of vehicles, and have a unique ID number and a sticker to indicate authenticity.[44]
Holography using other types of waves
[edit]In principle, it is possible to make a hologram for any wave.
Electron holography is the application of holography techniques to electron waves rather than light waves. Electron holography was invented by Dennis Gabor to improve the resolution and avoid the aberrations of the transmission electron microscope. Today it is commonly used to study electric and magnetic fields in thin films, as magnetic and electric fields can shift the phase of the interfering wave passing through the sample.[45] The principle of electron holography can also be applied to interference lithography.[46]
Acoustic holography enables sound maps of an object to be generated. Measurements of the acoustic field are made at many points close to the object. These measurements are digitally processed to produce the "images" of the object.[47]
Atomic holography has evolved out of the development of the basic elements of atom optics. With the Fresnel diffraction lens and atomic mirrors atomic holography follows a natural step in the development of the physics (and applications) of atomic beams. Recent developments including atomic mirrors and especially ridged mirrors have provided the tools necessary for the creation of atomic holograms,[48] although such holograms have not yet been commercialized.
Neutron beam holography has been used to see the inside of solid objects.[49]
Holograms with x-rays are generated by using synchrotrons or x-ray free-electron lasers as radiation sources and pixelated detectors such as CCDs as recording medium.[50] The reconstruction is then retrieved via computation. Due to the shorter wavelength of x-rays compared to visible light, this approach allows imaging objects with higher spatial resolution.[51] As free-electron lasers can provide ultrashort and x-ray pulses in the range of femtoseconds which are intense and coherent, x-ray holography has been used to capture ultrafast dynamic processes.[52][53][54]
False holograms
[edit]There are many optical effects that are falsely confused with holography, such as the effects produced by lenticular printing, the Pepper's ghost illusion (or modern variants such as the Musion Eyeliner), tomography and volumetric displays.[55][56] Such illusions have been called "fauxlography".[57][58]
The Pepper's ghost technique, being the easiest to implement of these methods, is most prevalent in 3D displays that claim to be (or are referred to as) "holographic". While the original illusion, used in theater, involved actual physical objects and persons, located offstage, modern variants replace the source object with a digital screen, which displays imagery generated with 3D computer graphics to provide the necessary depth cues. The reflection, which seems to float mid-air, is still flat however, thus less realistic than if an actual 3D object was being reflected.
Examples of this digital version of Pepper's ghost illusion include the Gorillaz performances in the 2005 MTV Europe Music Awards and the 48th Grammy Awards; and Tupac Shakur's virtual performance at Coachella Valley Music and Arts Festival in 2012, rapping alongside Snoop Dogg during his set with Dr. Dre.[59] Digital avatars of the Swedish supergroup ABBA were displayed on stage in May 2022.[60] The ABBA performance used technology that was an updated version of Pepper's Ghost created by Industrial Light & Magic.[61] American rock group KISS unveiled similar digital avatars in December 2023 to tour in their place at the conclusion of the End of the Road World Tour using the same Pepper's Ghost technology as the ABBA avatars.[62]
An even simpler illusion can be created by rear-projecting realistic images into semi-transparent screens. The rear projection is necessary because otherwise the semi-transparency of the screen would allow the background to be illuminated by the projection, which would break the illusion.
Crypton Future Media, a music software company that produced Hatsune Miku,[63] one of many Vocaloid singing synthesizer applications, has produced concerts that have Miku, along with other Crypton Vocaloids, performing on stage as "holographic" characters. These concerts use rear projection onto a semi-transparent DILAD screen[64][65] to achieve its "holographic" effect.[66][67]
In 2011, in Beijing, apparel company Burberry produced the "Burberry Prorsum Autumn/Winter 2011 Hologram Runway Show", which included life size 2-D projections of models. The company's own video[68] shows several centered and off-center shots of the main 2-dimensional projection screen, the latter revealing the flatness of the virtual models. The claim that holography was used was reported as fact in the trade media.[69]
In Madrid, on 10 April 2015, a public visual presentation called "Hologramas por la Libertad" (Holograms for Liberty), featuring a ghostly virtual crowd of demonstrators, was used to protest a new Spanish law that prohibits citizens from demonstrating in public places. Although widely called a "hologram protest" in news reports,[70] no actual holography was involved – it was yet another technologically updated variant of the Pepper's ghost illusion.
Holography is distinct from specular holography which is a technique for making three-dimensional images by controlling the motion of specularities on a two-dimensional surface.[71] It works by reflectively or refractively manipulating bundles of light rays, not by using interference and diffraction.
Tactile holograms
[edit]In fiction
[edit]Holography has been widely referred to in movies, novels, and TV, usually in science fiction, starting in the late 1970s.[72] Science fiction writers absorbed the urban legends surrounding holography that had been spread by overly-enthusiastic scientists and entrepreneurs trying to market the idea.[72] This had the effect of giving the public overly high expectations of the capability of holography, due to the unrealistic depictions of it in most fiction, where they are fully three-dimensional computer projections that are sometimes tactile through the use of force fields.[72] Examples of this type of depiction include the hologram of Princess Leia in Star Wars, Arnold Rimmer from Red Dwarf, who was later converted to "hard light" to make him solid, and the Holodeck and Emergency Medical Hologram from Star Trek.[72]
Holography has served as an inspiration for many video games with science fiction elements. In many titles, fictional holographic technology has been used to reflect real life misrepresentations of potential military use of holograms, such as the "mirage tanks" in Command & Conquer: Red Alert 2 that can disguise themselves as trees.[73] Player characters are able to use holographic decoys in games such as Halo: Reach and Crysis 2 to confuse and distract the enemy.[73] Starcraft ghost agent Nova has access to "holo decoy" as one of her three primary abilities in Heroes of the Storm.[74]
Fictional depictions of holograms have, however, inspired technological advances in other fields, such as augmented reality, that promise to fulfill the fictional depictions of holograms by other means.[75]
See also
[edit]- 3D file formats
- Computer-generated holography
- Holographic display
- Augmented reality
- Australian Holographics
- Autostereoscopy
- Digital holography
- Digital holographic microscopy
- Digital planar holography
- Fog display
- Holographic principle
- Holonomic brain theory
- Hogel Processing Unit
- Integral imaging
- List of emerging technologies
- Phase-coherent holography
- Plasmon – possible applications (full color holography)
- Tomography
- Volumetric display
- Volumetric printing
References
[edit]- ^ "What is Holography? | holocenter". Retrieved 2 September 2019.
- ^ a b Jesacher, Alexander; Ritsch-Marte, Monika (2 January 2016). "Synthetic holography in microscopy: opportunities arising from advanced wavefront shaping". Contemporary Physics. 57 (1): 46–59. Bibcode:2016ConPh..57...46J. doi:10.1080/00107514.2015.1120007. ISSN 0010-7514.
- ^ Sahin, Erdem; Stoykova, Elena; Mäkinen, Jani; Gotchev, Atanas (20 March 2020). "Computer-Generated Holograms for 3D Imaging: A Survey" (PDF). ACM Computing Surveys. 53 (2): 32:1–32:35. doi:10.1145/3378444. ISSN 0360-0300.
- ^ Blanche, P.-A.; Bablumian, A.; Voorakaranam, R.; Christenson, C.; Lin, W.; Gu, T.; Flores, D.; Wang, P.; et al. (2010). "Holographic three-dimensional telepresence using large-area photorefractive polymer". Nature. 468 (7320): 80–83. Bibcode:2010Natur.468...80B. doi:10.1038/nature09521. PMID 21048763. S2CID 205222841.
- ^ Smalley, D. E.; Nygaard, E.; Squire, K.; Van Wagoner, J.; Rasmussen, J.; Gneiting, S.; Qaderi, K.; Goodsell, J.; Rogers, W.; Lindsey, M.; Costner, K.; Monk, A.; Pearson, M.; Haymore, B.; Peatross, J. (25 January 2018). "A photophoretic-trap volumetric display". Nature. 553 (7689): 486–490. Bibcode:2018Natur.553..486S. doi:10.1038/nature25176. ISSN 1476-4687. PMID 29368704. S2CID 4451867.
- ^ Gabor, Dennis (1948). "A new microscopic principle". Nature. 161 (4098): 777–8. Bibcode:1948Natur.161..777G. doi:10.1038/161777a0. PMID 18860291. S2CID 4121017.
- ^ Gabor, Dennis (1949). "Microscopy by reconstructed wavefronts". Proceedings of the Royal Society. 197 (1051): 454–487. Bibcode:1949RSPSA.197..454G. doi:10.1098/rspa.1949.0075. S2CID 123187722.
- ^ a b Blanche, Pierre-Alexandre (2014). Field guide to holography. SPIE field guides. Bellingham, Wash: SPIE Press. p. 1. ISBN 978-0-8194-9957-8.
- ^ Hariharan, P. (1996). Optical Holography. Cambridge: Cambridge University Press. ISBN 9780521433488.
- ^ "The Nobel Prize in Physics 1971". Nobelprize.org. Retrieved 21 April 2012.
- ^ Denisyuk, Yuri N. (1962). "On the reflection of optical properties of an object in a wave field of light scattered by it". Doklady Akademii Nauk SSSR. 144 (6): 1275–1278.
- ^ Leith, E.N.; Upatnieks, J. (1962). "Reconstructed wavefronts and communication theory". J. Opt. Soc. Am. 52 (10): 1123–1130. Bibcode:1962JOSA...52.1123L. doi:10.1364/JOSA.52.001123.
- ^ Upatnieks, J; Leonard, C (1969). "Diffraction efficiency of bleached, photographically recorded interference patterns". Applied Optics. 8 (1): 85–89. Bibcode:1969ApOpt...8...85U. doi:10.1364/ao.8.000085. PMID 20072177.
- ^ Graube, A (1974). "Advances in bleaching methods for photographically recorded holograms". Applied Optics. 13 (12): 2942–6. Bibcode:1974ApOpt..13.2942G. doi:10.1364/ao.13.002942. PMID 20134813.
- ^ Phillips, N. J.; Porter, D. (1976). "An advance in the processing of holograms". Journal of Physics E: Scientific Instruments. 9 (8): 631. Bibcode:1976JPhE....9..631P. doi:10.1088/0022-3735/9/8/011.
- ^ Hariharan, P (2002). Basics of Holography. Cambridge: Cambridge University Press. ISBN 9780511755569.
- ^ Richards, Keith L. (2018). Design engineer's sourcebook. Boca Raton. ISBN 978-1-315-35052-3. OCLC 990152205.
{{cite book}}
: CS1 maint: location missing publisher (link) - ^ "The History and Development of Holography". Holophile.com. Retrieved 21 April 2012.
- ^ Coyle, Rebecca (1990). "Holography – Art in the space of technology". In Hayward, Philip (ed.). Culture, Technology & Creativity in the Late Twentieth Century. London, England: John Libbey and Company. pp. 65–88. ISBN 978-0-86196-266-2.
- ^ "Margaret Benyon Holography". Lisson Gallery. Retrieved 4 February 2016.
- ^ Integraf. "Dr. Tung J. Jeong Biography". Integraf.com. Retrieved 21 April 2012.
- ^ "holocenter". holocenter. Retrieved 21 April 2012.
- ^ "The Universal Hologram". Cherry Optical Holography.
- ^ Holographic metalwork http://www.zintaglio.com
- ^ "MIT Museum: Collections – Holography". Web.mit.edu. Retrieved 21 April 2012.
- ^ "The Jonathan Ross Hologram Collection". Jrholocollection.com. Retrieved 21 April 2012.
- ^ Lang, M.; Eschler, H. (1 October 1974). "Gigabyte capacities for holographic memories". Optics & Laser Technology. 6 (5): 219–224. Bibcode:1974OptLT...6..219L. doi:10.1016/0030-3992(74)90061-9. ISSN 0030-3992.
- ^ R. Ryf et al. High-frame-rate joint Fourier-transform correlator based on Sn2P2S6 crystal, Optics Letters 26, 1666–1668 (2001)
- ^ Strochlic, Nina (27 May 2014). "New York's Hologram King is Also the City's Last Pro Holographer". The Daily Beast.
- ^ Stephen Cass: Holiday Gifts 2005 Gifts and gadgets for technophiles of all ages: Do-It Yourself-3-D. In IEEE Spectrum, November 2005
- ^ Chiaverina, Chris: Litiholo holography – So easy even a caveman could have done it (apparatus review) Archived 8 February 2012 at the Wayback Machine. In The Physics Teacher, vol. 48, November 2010, pp. 551–552.
- ^ "A Holography FAQ". HoloWiki. 15 February 2011. Archived from the original on 6 November 2010. Retrieved 21 April 2012.
- ^ "Many methods are here". Holowiki.com. Archived from the original on 7 March 2012. Retrieved 21 April 2012.
- ^ "Jeff Blyth's Film Formulations". Cabd0.tripod.com. Retrieved 21 April 2012.
- ^ Powell, RL; Stetson, KA (1965). "Interferometric Vibration Analysis by Wavefront Reconstruction". J. Opt. Soc. Am. 55 (12): 1593–8. Bibcode:1965JOSA...55.1593P. doi:10.1364/josa.55.001593.
- ^ Jones, Robert; Wykes, Catherine (1989). Holographic and Speckle Interferometry. Cambridge: Cambridge University Press. ISBN 0-521-34417-4.
- ^ Beigzadeh, A.M.; Vaziri, M.R. Rashidian; Ziaie, F. (2017). "Modelling of a holographic interferometry based calorimeter for radiation dosimetry". Nuclear Instruments and Methods in Physics Research A. 864: 40–49. Bibcode:2017NIMPA.864...40B. doi:10.1016/j.nima.2017.05.019.
- ^ Y.Kuznetsova; A.Neumann, S.R.Brueck (2007). "Imaging interferometric microscopy–approaching the linear systems limits of optical resolution". Optics Express. 15 (11): 6651–6663. Bibcode:2007OExpr..15.6651K. doi:10.1364/OE.15.006651. PMID 19546975.
- ^ Yetisen, AK; Butt, H; da Cruz Vasconcellos, F; Montelongo, Y; Davidson, CAB; Blyth, J; Carmody, JB; Vignolini, S; Steiner, U; Baumberg, JJ; Wilkinson, TD; Lowe, CR (2013). "Light-Directed Writing of Chemically Tunable Narrow-Band Holographic Sensors". Advanced Optical Materials. 2 (3): 250–254. doi:10.1002/adom.201300375. S2CID 96257175.
- ^ MartíNez-Hurtado, J. L.; Davidson, C. A. B.; Blyth, J.; Lowe, C. R. (2010). "Holographic Detection of Hydrocarbon Gases and Other Volatile Organic Compounds". Langmuir. 26 (19): 15694–15699. doi:10.1021/la102693m. PMID 20836549.
- ^ 'Elastic hologram' pages 113–117, Proc. of the IGC 2010, ISBN 978-0-9566139-1-2 here: http://www.dspace.cam.ac.uk/handle/1810/225960
- ^ Beigzadeh, A.M. (2017). "Modelling of a holographic interferometry based calorimeter for radiation dosimetry". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 864: 40–49. Bibcode:2017NIMPA.864...40B. doi:10.1016/j.nima.2017.05.019.
- ^ Beigzadeh, A.M. (2018). "Double-exposure holographic interferometry for radiation dosimetry: A new developed model". Radiation Measurements. 119: 132–139. Bibcode:2018RadM..119..132B. doi:10.1016/j.radmeas.2018.10.010. S2CID 105842469.
- ^ "Why has the government made high security registration plates mandatory". The Economic Times. ET Online. Retrieved 18 July 2021.
- ^ R. E. Dunin-Borkowski et al., Micros. Res. and Tech. vol. 64, pp. 390–402 (2004)
- ^ Ogai, K.; et al. (1993). "An Approach for Nanolithography Using Electron Holography". Jpn. J. Appl. Phys. 32 (12S): 5988–5992. Bibcode:1993JaJAP..32.5988O. doi:10.1143/jjap.32.5988. S2CID 123606284.
- ^ "Acoustic Holography". Bruel and Kjaer. Retrieved 3 September 2022.
- ^ F. Shimizu; J.Fujita (March 2002). "Reflection-Type Hologram for Atoms". Physical Review Letters. 88 (12): 123201. Bibcode:2002PhRvL..88l3201S. doi:10.1103/PhysRevLett.88.123201. PMID 11909457.
- ^ Swenson, Gayle (20 October 2016). "Move Over, Lasers: Scientists Can Now Create Holograms from Neutrons, Too". NIST. Retrieved 4 April 2017.
- ^ Eisebitt, S.; et al. (2004). "Lensless imaging of magnetic nanostructures by X-ray spectro-holography". Nature. 432 (7019): 885–888. Bibcode:2004Natur.432..885E. doi:10.1038/nature03139. PMID 15602557. S2CID 4423853.
- ^ Pfau, B.; et al. (2014). "Influence of stray fields on the switching-field distribution for bit-patterned media based on pre-patterned substrates" (PDF). Applied Physics Letters. 105 (13): 132407. Bibcode:2014ApPhL.105m2407P. doi:10.1063/1.4896982. S2CID 121512138.
- ^ Chapman, H. N.; et al. (2007). "Femtosecond time-delay X-ray holography" (PDF). Nature. 448 (7154): 676–679. Bibcode:2007Natur.448..676C. doi:10.1038/nature06049. PMID 17687320. S2CID 4406541.
- ^ Günther, C.M.; et al. (2011). "Sequential femtosecond X-ray imaging". Nature Photonics. 5 (2): 99–102. Bibcode:2011NaPho...5...99G. doi:10.1038/nphoton.2010.287.
- ^ von Korff, Schmising; et al. (2014). "Imaging Ultrafast Demagnetization Dynamics after a Spatially Localized Optical Excitation" (PDF). Physical Review Letters. 112 (21): 217203. Bibcode:2014PhRvL.112u7203V. doi:10.1103/PhysRevLett.112.217203. Archived (PDF) from the original on 7 December 2023.
- ^ "Holographic announcers at Luton airport". BBC News. 31 January 2011. Retrieved 21 April 2012.
- ^ Farivar, Cyrus (16 April 2012). "Tupac "hologram" merely pretty cool optical illusion". Ars Technica. Retrieved 21 April 2012.
- ^ "Holographic 3D Technology: From Sci-fi Fantasy to Engineering Reality". International Year of Light Blog. 28 September 2015. Archived from the original on 30 October 2017.
- ^ Gordon, Marcus A. (2017). Habitat 44º (MFA). OCAD University. doi:10.13140/RG.2.2.30421.88802.
- ^ Sung, Carolyn; Gauk-Roger, Topher; Quan, Denise; Iavazzi, Jessica (16 April 2012). "Tupac returns as a hologram at Coachella". The Marquee Blog. CNN Blogs. Archived from the original on 4 May 2012. Retrieved 21 April 2012.
- ^ Brause; Mills (27 May 2022). "Super Trouper: ABBA returns to stage as virtual avatars for London gigs". Reuters. Retrieved 4 June 2022.
- ^ Carter, Ninian (27 November 2018). "ABBA's mysterious "Abbatars" revealed". Graphic News. Retrieved 4 June 2022.
- ^ Amorosi, A. D. (3 December 2023). "KISS Says Farewell at Madison Square Garden, Before Passing the Torch to Band's Avatar Successors: Concert Review". Variety. Retrieved 3 December 2023.
- ^ "Crypton" クリプトン (in Japanese). Crypton.co.jp. Retrieved 21 April 2012.
- ^ G., Adrian. "LA's Anime Expo hosting Hatsune Miku's first US live performance on 2 July". Archived from the original on 18 October 2012. Retrieved 20 April 2012.
- ^ ""We can invite Hatsune Miku in my room!", Part 2 (video)". Youtube.com. 7 September 2011. Archived from the original on 30 October 2021. Retrieved 21 April 2012.
- ^ "Technically incorrect: Tomorrow's Miley Cyrus? A hologram live in concert!". Retrieved 29 April 2011.
- ^ "Hatsune Miku – World is Mine Live in HD". YouTube. Retrieved 29 April 2011.
- ^ "Burberry Beijing – Full Show". Youtube.com. Archived from the original on 4 October 2011. Retrieved 21 April 2012.
- ^ "Burberry lands in China". Retrieved 14 June 2011.
- ^ "First Hologram Protest in History Held Against Spain's Gag Law". revolution-news.com. Archived from the original on 13 April 2015. Retrieved 13 April 2015.
- ^ "specular holography: how". Zintaglio.com. Retrieved 21 April 2012.
- ^ a b c d Johnston, Sean (2006). "The Hologram and Popular Culture". Holographic Visions: a History of New Science. Oxford: Oxford University Press, UK. pp. 405–408. ISBN 978-0191513886. OCLC 437109030.
- ^ a b Johnston, Sean F. (2015). "11 - Channeling Dreams". Holograms: A Cultural History. Oxford University Press. ISBN 978-0191021381.
- ^ "Nova - Heroes of the Storm". us.battle.net. Retrieved 20 October 2019.
- ^ Richardson, Martin (13 November 2017). The Hologram: Principles and Techniques. Wiltshire, John D. Hoboken, NJ. ISBN 978-1119088905. OCLC 1000385946.
{{cite book}}
: CS1 maint: location missing publisher (link)
Bibliography
[edit]- Hariharan P, 1996, Optical Holography, Cambridge University Press, ISBN 0-521-43965-5
- Hariharan P, 2002, Basics of Holography, Cambridge University Press, ISBN 0-521-00200-1
- Lipson A., Lipson SG, Lipson H, Optical Physics, 2011, Cambridge University Press, ISBN 978-0-521-49345-1
Further reading
[edit]- Lasers and holography: an introduction to coherent optics W. E. Kock, Dover Publications (1981), ISBN 978-0-486-24041-1
- Principles of holography H. M. Smith, Wiley (1976), ISBN 978-0-471-80341-6
- G. Berger et al., Digital Data Storage in a phase-encoded holographic memory system: data quality and security, Proceedings of SPIE, Vol. 4988, pp. 104–111 (2003)
- Holographic Visions: A History of New Science Sean F. Johnston, Oxford University Press (2006), ISBN 0-19-857122-4
- Saxby, Graham (2003). Practical Holography, Third Edition. Taylor and Francis. ISBN 978-0-7503-0912-7.
- Three-Dimensional Imaging Techniques Takanori Okoshi, Atara Press (2011), ISBN 978-0-9822251-4-1
- Holographic Microscopy of Phase Microscopic Objects: Theory and Practice Tatyana Tishko, Tishko Dmitry, Titar Vladimir, World Scientific (2010), ISBN 978-981-4289-54-2
- Richardson, Martin J.; Wiltshire, John D. (2017). Richardson, Martin J.; Wiltshire, John D. (eds.). The Hologram: Principles and Techniques. Wiley. Bibcode:2017hpt..book.....R. doi:10.1002/9781119088929. ISBN 9781119088905. OCLC 1000385946.
External links
[edit]- "Dennis Gabor – Autobiography", 30 September 2004, Nobelprize.org
- "Holography, 1948-1971 Nobel Lecture", 11 December 1971, by Dennis Gabor
- "How Holograms Work", How Stuff Works, by Tracy V. Wilson, 30 August 2023
- "Holography" by The Strange Theory of Light, QED
- "Making Real Holograms!!!!!!" at YouTube by The Thought Emporium, 19 November 2020