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{{Short description|Type of atomic emission spectroscopy}}
{{more footnotes|date=December 2010}}
{{redirect|Libs|the abbreviation|Liberal (disambiguation){{!}}Liberal}}
[[File:Libs Laser-induced breakdown spectroscopy.jpg|thumb|right|200px|'''Schematic of a LIBS system''' - Courtesy of US Army Research Laboratory]]
[[File:Libs Laser-induced breakdown spectroscopy.jpg|thumb|right|200px|'''Schematic of a LIBS system''' Courtesy of US Army Research Laboratory]]
'''Laser-induced breakdown spectroscopy''' ('''LIBS''') is a type of [[Atomic emission spectroscopy|atomic emission]] [[spectroscopy]] which uses a highly energetic [[laser]] pulse as the excitation source.<ref name="isbn0-470-09299-8">{{cite book |author1=Radziemski, Leon J. |author2=Cremers, David A. |title=Handbook of laser-induced breakdown spectroscopy |publisher=John Wiley |location=New York |date=2006 |pages= |isbn=0-470-09299-8 |oclc= |doi= }}</ref><ref name="isbn0-521-85274-9">{{cite book |author1=Schechter, Israel |author2=Miziolek, Andrzej W. |author3=Vincenzo Palleschi |title=Laser-induced breakdown spectroscopy (LIBS): fundamentals and applications |publisher=Cambridge University Press |location=Cambridge, UK |date=2006 |pages= |isbn=0-521-85274-9 |oclc= |doi= }}</ref> The laser is focused to form a plasma, which atomizes and excites samples. The formation of the plasma only begins when the focused laser achieves a certain threshold for optical breakdown, which generally depends on the environment and the target material.<ref>J. P. Singh and S. N. Thakur, Laser-Induced Breakdown Spectroscopy, 1st ed.. (Elsevier, 2007).</ref> In principle, LIBS can analyze any [[matter]] regardless of its [[physical state]], be it solid, liquid or gas. Because all [[chemical element|elements]] emit light of characteristic frequencies when excited to sufficiently high temperatures, LIBS can (in principle) detect all elements, limited only by the power of the laser as well as the sensitivity and wavelength range of the spectrograph & detector. If the constituents of a material to be analyzed are known, LIBS may be used to evaluate the relative abundance of each constituent element, or to monitor the presence of impurities. In practice, detection limits are a function of a) the plasma [[excitation temperature]], b) the light collection window, and c) the line strength of the viewed transition. LIBS makes use of optical [[emission spectrometry]] and is to this extent very similar to arc/spark [[emission spectroscopy]].
'''Laser-induced breakdown spectroscopy''' ('''LIBS''') is a type of [[atomic emission spectroscopy]] which uses a highly energetic [[laser]] pulse as the excitation source.<ref name="isbn0-470-09299-8">{{cite book |author1=Radziemski, Leon J. |author2=Cremers, David A. |title=Handbook of laser-induced breakdown spectroscopy |publisher=John Wiley |location=New York |date=2006 |isbn=0-470-09299-8 }}</ref><ref name="isbn0-521-85274-9">{{cite book |author1=Schechter, Israel |author2=Miziolek, Andrzej W. |author3=Vincenzo Palleschi |title=Laser-induced breakdown spectroscopy (LIBS): fundamentals and applications |publisher=Cambridge University Press |location=Cambridge, UK |date=2006 |isbn=0-521-85274-9 }}</ref> The laser is focused to form a plasma, which atomizes and excites samples. The formation of the plasma only begins when the focused laser achieves a certain threshold for optical breakdown, which generally depends on the environment and the target material.<ref>J. P. Singh and S. N. Thakur, Laser-Induced Breakdown Spectroscopy, 1st ed.. (Elsevier, 2007).</ref>

LIBS operates by focusing the laser onto a small area at the surface of the specimen; when the laser is discharged it [[ablation|ablates]] a very small amount of material, in the range of nanograms to picograms, which generates a [[Plasma (physics)|plasma]] plume with temperatures in excess of 100,000 K. During data collection, typically after local thermodynamic equilibrium is established, plasma temperatures range from 5,000–20,000 K. At the high temperatures during the early plasma, the ablated material dissociates (breaks down) into excited [[ion]]ic and [[atom]]ic species. During this time, the plasma emits a [[Continuum (theory)|continuum]] of radiation which does not contain any useful information about the species present, but within a very small timeframe the plasma expands at [[supersonic]] velocities and cools. At this point the characteristic atomic emission lines of the elements can be observed. The delay between the emission of continuum radiation and characteristic radiation is in the order of 10 μs, which is why it is necessary to temporally gate the detector.

LIBS is sometimes referred to as laser-induced plasma spectroscopy (LIPS); however that acronym also has alternative meanings that are outside the field of analytical spectroscopy.

LIBS is technically very similar to a number of other laser-based analytical techniques, sharing much of the same hardware. These techniques are the [[vibrational spectroscopy|vibrational spectroscopic]] technique of [[Raman spectroscopy]], and the [[Fluorescence spectroscopy|fluorescence spectroscopic]] technique of [[laser-induced fluorescence]] (LIF). In fact devices are now being manufactured which combine these techniques in a single instrument, allowing the [[atom]]ic, [[molecular]] and structural characterisation of a specimen as well as giving a deeper insight into physical properties.

==Design==
A typical LIBS system consists of a [[Nd:YAG]] [[solid-state laser]] and a [[spectrometer]] with a wide spectral range and a high sensitivity, fast response rate, time gated detector. This is coupled to a computer which can rapidly process and interpret the acquired data. As such LIBS is one of the most experimentally simple spectroscopic analytical techniques, making it one of the cheapest to purchase and to operate.

The Nd:YAG laser generates energy in the near [[infrared]] region of the [[electromagnetic spectrum]], with a wavelength of 1064 [[nanometre|nm]]. The pulse duration is in the region of 10 ns generating a power density which can exceed 1 GW·cm<sup>−2</sup> at the focal point. Other lasers have been used for LIBS, mainly the [[Excimer]] ('''Exc'''ited d'''imer''') type that generates energy in the [[Visible spectrum|visible]] and [[ultraviolet]] regions.

The spectrometer consists of either a [[monochromator]] (scanning) or a [[polychromator]] (non-scanning) and a [[photomultiplier]] or [[Charge-coupled device|CCD]] detector respectively. The most common monochromator is the [[Monochromator#Czerny–Turner monochromator|Czerny–Turner]] type whilst the most common polychromator is the Echelle type. However, even the Czerny-Turner type can be (and is often) used to disperse the radiation onto a CCD effectively making it a polychromator. The polychromator spectrometer is the type most commonly used in LIBS as it allows simultaneous acquisition of the entire wavelength range of interest.

The spectrometer collects electromagnetic radiation over the widest wavelength range possible, maximising the number of emission lines detected for each particular element. Spectrometer response is typically from 1100&nbsp;nm ([[near infrared]]) to 170&nbsp;nm ([[deep ultraviolet]]), the approximate response range of a CCD detector. All elements have emission lines within this wavelength range. The energy resolution of the spectrometer can also affect the quality of the LIBS measurement, since high resolution systems can separate spectral emission lines in close [[Juxtaposition (literary)|juxtaposition]], reducing interference and increasing selectivity. This feature is particularly important in specimens which have a complex [[matrix (chemical analysis)|matrix]], containing a large number of different elements. Accompanying the spectrometer and detector is a delay generator which accurately gates the detector's response time, allowing [[temporal resolution]] of the spectrum.

==Advantages==
Because such a small amount of material is consumed during the LIBS process the technique is considered essentially non-destructive or minimally-destructive, and with an average power density of less than one watt radiated onto the specimen there is almost no specimen heating surrounding the ablation site.
Due to the nature of this technique sample preparation is typically minimised to homogenisation or is often unnecessary where heterogeneity is to be investigated or where a specimen is known to be sufficiently [[wiktionary:Homogeneous|homogeneous]], this reduces the possibility of contamination during chemical preparation steps. One of the major advantages of the LIBS technique is its ability to depth profile a specimen by repeatedly discharging the laser in the same position, effectively going deeper into the specimen with each shot. This can also be applied to the removal of surface contamination, where the laser is discharged a number of times prior to the analysing shot. LIBS is also a very rapid technique giving results within seconds, making it particularly useful for high volume analyses or on-line industrial monitoring.

LIBS is an entirely optical technique, therefore it requires only optical access to the specimen. This is of major significance as fiber optics can be employed for remote analyses. And being an optical technique it is non-invasive, non-contact and can even be used as a stand-off analytical technique when coupled to appropriate telescopic apparatus. These attributes have significance for use in areas from hazardous environments to space exploration. Additionally LIBS systems can easily be coupled to an optical microscope for micro-sampling adding a new dimension of analytical flexibility.

With specialised optics or a mechanically positioned specimen stage the laser can be scanned over the surface of the specimen allowing spatially resolved chemical analysis and the creation of 'elemental maps'. This is very significant as chemical imaging is becoming more important in all branches of science and technology.

Portable LIBS systems are more sensitive, faster and can detect a wider range of elements (particularly the light elements) than competing techniques such as portable [[x-ray fluorescence]]. And LIBS does not use [[ionizing radiation]] to excite the sample, which is both penetrating and potentially [[carcinogenic]].

==Disadvantages==
LIBS, like all other analytical techniques is not without limitations. It is subject to variation in the laser spark and resultant plasma which often limits reproducibility. The [[accuracy]] of LIBS measurements is typically better than 10% and [[Accuracy and precision|precision]] is often better than 5%. The detection limits for LIBS vary from one element to the next depending on the specimen type and the experimental apparatus used. Even so, detection limits of 1 to 30 [[Parts per million|ppm]] by mass are not uncommon, but can range from {{nowrap|>100 ppm}} to {{nowrap|<1 ppm.}}


== 2000s developments ==
== 2000s developments ==


From 2000–2010, the [[United States Army Research Laboratory|U.S. Army Research Laboratory]] (ARL) researched potential extensions to LIBS technology, which focused on hazardous material detection.<ref>{{Cite web|url=http://www.spectroscopyonline.com/current-status-standoff-libs-security-applications-united-states-army-research-laboratory-0|title=Current Status of Standoff LIBS Security Applications at the United States Army Research Laboratory|last=Munson|first=Jennifer L. Gottfried Frank C. De Lucia Jr. Andrzej W. Miziolek Chase A.|website=www.spectroscopyonline.com|language=en|access-date=2018-08-27}}</ref><ref name=":0">{{Cite web|url=https://www.arl.army.mil/arlreports/2010/ARL-TR-5238.pdf|title=Laser-Induced Breakdown Spectroscopy: Capabilities and Applications}}</ref> Applications investigated at ARL included the standoff detection of explosive residues and other hazardous materials, plastic landmine discrimination, and material characterization of various metal alloys and polymers. Results presented by ARL suggest that LIBS may be able to discriminate between energetic and non-energetic materials.<ref>{{Cite web|url=https://www.arl.army.mil/arlreports/2007/ARL-TR-4240.pdf|title=Detection of Energetic Materials and Explosive ResiduesWith Laser-Induced Breakdown Spectroscopy: I. Laboratory Measurements}}</ref>
From 2000 to 2010, the [[United States Army Research Laboratory|U.S. Army Research Laboratory]] (ARL) researched potential extensions to LIBS technology, which focused on hazardous material detection.<ref>{{Cite journal|url=http://www.spectroscopyonline.com/current-status-standoff-libs-security-applications-united-states-army-research-laboratory-0|title=Current Status of Standoff LIBS Security Applications at the United States Army Research Laboratory|last=Munson|first=Jennifer L. Gottfried Frank C. De Lucia Jr. Andrzej W. Miziolek Chase A.|journal=Spectroscopy|series=Spectroscopy-06-01-2009 |date=June 2009 |volume=24 |issue=6 |language=en|access-date=2018-08-27}}</ref><ref name=":0">{{Cite journal|doi=10.21236/ada528756|title=Laser-Induced Breakdown Spectroscopy: Capabilities and Applications|year=2010|last1=Gottfried|first1=Jennifer L.|last2=De Lucia|first2=Frank C. Jr.}}</ref> Applications investigated at ARL included the standoff detection of explosive residues and other hazardous materials, plastic landmine discrimination, and material characterization of various metal alloys and polymers. Results presented by ARL suggest that LIBS may be able to discriminate between energetic and non-energetic materials.<ref>{{Cite web|url=https://apps.dtic.mil/dtic/tr/fulltext/u2/a472707.pdf|archive-url=https://web.archive.org/web/20200510012357/https://apps.dtic.mil/dtic/tr/fulltext/u2/a472707.pdf|url-status=live|archive-date=May 10, 2020|title=Detection of Energetic Materials and Explosive Residues With Laser-Induced Breakdown Spectroscopy: I. Laboratory Measurements}}</ref>


=== Research ===
=== Research ===


In 2000, ARL and Ocean Optics Inc. developed a broadband high-resolution spectrometer which was commercialized in 2003. Designed for material analysis, the spectrometer allowed the LIBS system to be sensitive to chemical elements in low concentration.<ref>{{Cite web|url=https://www.qualitydigest.com/inside/twitter-ed/us-army-researchers-explore-laser-detection-techniques.html|title=U.S. Army Researchers Explore Laser Detection Techniques {{!}} Quality Digest|website=www.qualitydigest.com|language=en|access-date=2018-08-27}}</ref>
Broadband high-resolution spectrometers were developed in 2000 and commercialized in 2003. Designed for material analysis, the spectrometer allowed the LIBS system to be sensitive to chemical elements in low concentration.<ref>{{Cite web|url=https://www.qualitydigest.com/inside/twitter-ed/us-army-researchers-explore-laser-detection-techniques.html|title=U.S. Army Researchers Explore Laser Detection Techniques {{!}} Quality Digest|website=www.qualitydigest.com|language=en|access-date=2018-08-27}}</ref>


ARL LIBS applications studied from 2000 to 2010 included:<ref name=":0" />  
ARL LIBS applications studied from 2000 to 2010 included:<ref name=":0" />


* Tested for detection of Halon alternative agents
* Tested for detection of Halon alternative agents
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* Studied the spectral emission of aluminum and aluminum oxides from bulk aluminum in different bath gases
* Studied the spectral emission of aluminum and aluminum oxides from bulk aluminum in different bath gases
* Performed kinetic modeling of LIBS plumes
* Performed kinetic modeling of LIBS plumes
* Demonstrated the detection and discrimination of geological materials, plastic landmines, explosives, and chemical and biological warfare agent surrogates 
* Demonstrated the detection and discrimination of geological materials, plastic landmines, explosives, and chemical and biological warfare agent surrogates


ARL LIBS prototypes studied during this period included:<ref name=":0" />
ARL LIBS prototypes studied during this period included:<ref name=":0" />


* Laboratory LIBS setup
* Laboratory LIBS setup
* Commercial LIBS system by Ocean Optics, Inc.
* Commercial LIBS system
* Man-portable LIBS device
* Man-portable LIBS device
* Standoff LIBS system developed for 100+ m detection and discriminate on of explosive residues.
* Standoff LIBS system developed for 100+ m detection and discriminate on of explosive residues.


==2010s developments==
==2010s developments==
LIBS is one of several analytical techniques that can be deployed in the field as opposed to pure laboratory techniques e.g. spark [[Optical Emissions Spectrometer|OES]]. {{As of | 2015}}, recent research on LIBS focuses on compact and (man-)portable systems. Some industrial applications of LIBS include the detection of material mix-ups,<ref>{{cite journal|doi=10.1016/s0584-8547(01)00214-2|title=Laser-induced breakdown spectrometry — applications for production control and quality assurance in the steel industry|year=2001|last1=Noll|first1=Reinhard|last2=Bette|first2=Holger|last3=Brysch|first3=Adriane|last4=Kraushaar|first4=Marc|last5=Mönch|first5=Ingo|last6=Peter|first6=Laszlo|last7=Sturm|first7=Volker|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=56|issue=6|pages=637–649|bibcode=2001AcSpe..56..637N}}</ref> analysis of inclusions in steel, analysis of slags in secondary metallurgy,<ref>{{cite journal|doi=10.1016/j.sab.2015.10.009|title=Analysis of slags using laser-induced breakdown spectroscopy|year=2016|last1=Sanghapi|first1=Hervé K.|last2=Ayyalasomayajula|first2=Krishna K.|last3=Yueh|first3=Fang Y.|last4=Singh|first4=Jagdish P.|last5=McIntyre|first5=Dustin L.|last6=Jain|first6=Jinesh C.|last7=Nakano|first7=Jinichiro|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=115|pages=40–45|bibcode=2016AcSpe.115...40S|doi-access=free}}</ref> analysis of combustion processes,<ref>{{cite journal|doi=10.1364/ao.55.008042|title=Sensitivity, stability, and precision of quantitative Ns-LIBS-based fuel-air-ratio measurements for methane-air flames at 1–11 bar|year=2016|last1=Hsu|first1=Paul S.|last2=Gragston|first2=Mark|last3=Wu|first3=Yue|last4=Zhang|first4=Zhili|last5=Patnaik|first5=Anil K.|last6=Kiefer|first6=Johannes|last7=Roy|first7=Sukesh|last8=Gord|first8=James R.|journal=Applied Optics|volume=55|issue=28|pages=8042–8048|pmid=27828047|bibcode=2016ApOpt..55.8042H|doi-access=free}}</ref> and high-speed identification of scrap pieces for material-specific recycling tasks. Armed with data analysis techniques, this technique is being extended to pharmaceutical samples.<ref>{{cite journal|doi=10.1016/s0584-8547(02)00062-9|title=Quantitative analysis of pharmaceutical products by laser-induced breakdown spectroscopy|year=2002|last1=St-Onge|first1=L.|last2=Kwong|first2=E.|last3=Sabsabi|first3=M.|last4=Vadas|first4=E.B|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=57|issue=7|pages=1131–1140|bibcode=2002AcSpe..57.1131S}}</ref><ref name="Ashwin2011">{{cite journal|doi= 10.1016/j.talanta.2011.09.040|pmid= 22099648|title= Laser-induced breakdown spectroscopy-based investigation and classification of pharmaceutical tablets using multivariate chemometric analysis|journal= Talanta|volume= 87|pages= 53–59|pmc= 3418677|year= 2011|last1= Myakalwar|first1= Ashwin Kumar|last2= Sreedhar|first2= S.|last3= Barman|first3= Ishan|last4= Dingari|first4= Narahara Chari|last5= Venugopal Rao|first5= S.|last6= Prem Kiran|first6= P.|last7= Tewari|first7= Surya P.|last8= Manoj Kumar|first8= G.}}</ref>
In the 2010s, interest developed in LIBS that focused on the miniaturization of the components and the development of compact, low-power, portable systems. Interest from groups such as [[NASA]] and [[ESA]] - as well as the [[military]] - has furthered these developments. The [[Mars Science Laboratory]] mission brought [[Curiosity rover#Chemistry and Camera complex .28ChemCam.29|ChemCam]], a LIBS instrument, to the surface of Mars in 2012.

Recent developments in LIBS have seen the introduction of double-pulsed laser systems.<ref name="AhmedBaig2009">{{cite journal|last1=Ahmed|first1=Rizwan|last2=Baig|first2=M. Aslam|title=A comparative study of single and double pulse laser induced breakdown spectroscopy|journal=Journal of Applied Physics|volume= 106|issue= 3|date= 2009|pages= 033307–033307–6|issn= 0021-8979|doi= 10.1063/1.3190516|bibcode=2009JAP...106c3307A}}</ref><ref name="AhmedBaig2010">{{cite journal|last1=Ahmed|first1=R|last2=Baig|first2=M A|title=On the Optimization for Enhanced Dual-Pulse Laser-Induced Breakdown Spectroscopy|journal=IEEE Transactions on Plasma Science|volume= 38|issue= 8|date= 2010|pages= 2052–2055|issn= 0093-3813|doi= 10.1109/TPS.2010.2050784|bibcode=2010ITPS...38.2052A}}</ref> For double-pulse LIBS one distinguishes between orthogonal and perpendicular configuration. In perpendicular configuration the laser fires twice on the same spot on the specimen with a pulse separation in the order of one to a couple of tens of microseconds. Depending on pulse separation, the second pulse is more or less absorbed by the plasma plume caused by the previous pulse, resulting in a reheating of the laser plasma leading to signal enhancement.
In orthogonal configuration a laser pulse is fired parallel to the sample surface either before or after the perpendicular pulse hits the specimen. The laser plasma ignited in the surrounding medium above the surface by a first pulse causes (by its shock wave) an area of reduced pressure above the specimen into which the actual plasma from the sample can expand. This has similar positive effects on sensitivity like LIBS performed at reduced pressures.
If the orthogonal laser pulse is delayed with respect to the perpendicular one, the effects are similar as in the perpendicular configuration. Timing electronics such as digital delay generators can precisely control the timing of both pulses. In recent, fully 3D simulation/modeling captured the shockwave movement and interactions with wall.<ref>Wang, Y., Yuan, H., Fu, Y., & Wang, Z. (2016). Experimental and computational investigation of confined laser-induced breakdown spectroscopy. Spectrochimica Acta Part B: Atomic Spectroscopy, 126, 44-52.</ref>

Both double-pulse LIBS as well as LIBS at reduced pressures aim at increasing the sensitivity of LIBS and the reduction of errors caused by the differential volatility of elements (e.g. hydrogen as an impurity in solids).<!-- Paper from Kagawa group would be suitable as reference --> It also significantly reduces the matrix effects. Double-pulsed systems have proven useful in conducting analysis in liquids, as the initial laser pulse forms a cavity bubble in which the second pulse acts on the evaporated material.

LIBS is one of several analytical techniques that can be deployed in the field as opposed to pure laboratory techniques e.g. spark [[Optical Emissions Spectrometer|OES]]. {{As of | 2015}}, recent research on LIBS focuses on compact and (man-)portable systems. Some industrial applications of LIBS include the detection of material mix-ups,<ref>R. Noll, H. Bette, A. Brysch, M. Kraushaar, I. Mönch, L. Peter, and V. Sturm, "Laser-induced breakdown spectrometry — applications for production control and quality assurance in the steel industry," Spectrochim. Acta Part B At. Spectrosc. 56, 637–649 (2001).</ref> analysis of inclusions in steel, analysis of slags in secondary metallurgy,<ref>H. K. Sanghapi, K. K. Ayyalasomayajula, F. Y. Yueh, J. P. Singh, D. L. McIntyre, J. C. Jain, and J. Nakano, "Analysis of slags using laser-induced breakdown spectroscopy," Spectrochim. Acta Part B At. Spectrosc. 115, 40–45 (2016).</ref> analysis of combustion processes,<ref>P. S. Hsu, M. Gragston, Y. Wu, Z. Zhang, A. K. Patnaik, J. Kiefer, S. Roy, and J. R. Gord, "Sensitivity, stability, and precision of quantitative Ns-LIBS-based fuel-air-ratio measurements for methane-air flames at 1–11 bar," Appl. Opt. 55, 8042 (2016).</ref> and high-speed identification of scrap pieces for material-specific recycling tasks. Armed with data analysis techniques, this technique is being extended to pharmaceutical samples.<ref>L. St-Onge, E. Kwong, M. Sabsabi, and E. B. Vadas, "Quantitative analysis of pharmaceutical products by laser-induced breakdown spectroscopy," Spectrochim. Acta Part B At. Spectrosc. 57, 1131–1140 (2002).</ref><ref name="Ashwin2011">{{cite journal|doi= 10.1016/j.talanta.2011.09.040|title= Laser-induced breakdown spectroscopy-based investigation and classification of pharmaceutical tablets using multivariate chemometric analysis|journal= Talanta|volume= 87|pages= 53–59|pmc= 3418677|year= 2011|last1= Myakalwar|first1= Ashwin Kumar|last2= Sreedhar|first2= S.|last3= Barman|first3= Ishan|last4= Dingari|first4= Narahara Chari|last5= Venugopal Rao|first5= S.|last6= Prem Kiran|first6= P.|last7= Tewari|first7= Surya P.|last8= Manoj Kumar|first8= G.}}</ref>


===LIBS using short laser pulses===
===LIBS using short laser pulses===
Following [[Multiphoton ionization|multiphoton]] or [[tunnel ionization]] the electron is being accelerated by inverse [[Bremsstrahlung]] and can collide with the nearby molecules and generate new electrons through collisions. If the pulse duration is long, the newly ionized electrons can be accelerated and eventually avalanche or cascade ionization follows. Once the density of the electrons reaches a critical value, breakdown occurs and high density plasma is created which has no memory of the laser pulse. So, the criterion for the shortness of a pulse in dense media is as follows: A pulse interacting with a dense matter is considered to be short if during the interaction the threshold for the avalanche ionization is not reached. At the first glance this definition may appear to be too limiting. Fortunately, due to the delicately balanced behavior of the pulses in dense media, the threshold cannot be reached easily.<ref>S. Mehdi Sharifi and Abdossamad Talebpour, Applications of Short Laser Pulses, cdn.intechopen.com</ref> The phenomenon responsible for the balance is the intensity clamping<ref>Xu, Shengqi, et al. "Simple method of measuring laser peak intensity inside a femtosecond laser filament in air." Opt. Express 20.1 (2012): 299-307.</ref> through the onset of [[Filament propagation|filamentation]]<nowiki/> process during the propagation of strong laser pulses in dense media.
Following [[Multiphoton ionization|multiphoton]] or [[tunnel ionization]] the electron is being accelerated by inverse [[Bremsstrahlung]] and can collide with the nearby molecules and generate new electrons through collisions. If the pulse duration is long, the newly ionized electrons can be accelerated and eventually avalanche or cascade ionization follows. Once the density of the electrons reaches a critical value, breakdown occurs and high density plasma is created which has no memory of the laser pulse. So, the criterion for the shortness of a pulse in dense media is as follows: A pulse interacting with a dense matter is considered to be short if during the interaction the threshold for the avalanche ionization is not reached. At the first glance this definition may appear to be too limiting. Fortunately, due to the delicately balanced behavior of the pulses in dense media, the threshold cannot be reached easily.{{Citation needed|date=December 2019|reason=removed citation to predatory publisher content}} The phenomenon responsible for the balance is the intensity clamping<ref>{{cite journal|doi=10.1364/oe.20.000299|title=Simple method of measuring laser peak intensity inside femtosecond laser filament in air|year=2012|last1=Xu|first1=Shengqi|last2=Sun|first2=Xiaodong|last3=Zeng|first3=Bin|last4=Chu|first4=Wei|last5=Zhao|first5=Jiayu|last6=Liu|first6=Weiwei|last7=Cheng|first7=Ya|last8=Xu|first8=Zhizhan|last9=Chin|first9=See Leang|journal=Optics Express|volume=20|issue=1|pages=299–307|pmid=22274353|bibcode=2012OExpr..20..299X|doi-access=free}}</ref> through the onset of [[Filament propagation|filamentation]] process during the propagation of strong laser pulses in dense media.


A potentially important development to LIBS involves the use of a short laser pulse as a spectroscopic source.<ref>A. Talebpour et al., Spectroscopy of the Gases Interactingwith Intense Femtosecond Laser Pulses, 2001, ''Laser Physics'', '''11:'''68–76</ref> In this method, a plasma column is created as a result of focusing ultrafast laser pulses in a gas. The self-luminous plasma is far superior in terms of low level of continuum and also smaller line broadening. This is attributed to the lower density of the plasma in the case of short laser pulses due to the defocusing effects which limits the intensity of the pulse in the interaction region and thus prevents further multiphoton/tunnel ionization of the gas.<ref>A. Talebpour ''et al''., Focusing limits of intense ultrafast laser pulses in a high pressure gas: road to new spectroscopic source, 2000, ''Optics Communications, '''''183:'''479–484</ref><ref>
A potentially important development to LIBS involves the use of a short laser pulse as a spectroscopic source.<ref>A. Talebpour et al., Spectroscopy of the Gases Interactingwith Intense Femtosecond Laser Pulses, 2001, ''Laser Physics'', '''11:'''68–76</ref> In this method, a plasma column is created as a result of focusing ultrafast laser pulses in a gas. The self-luminous plasma is far superior in terms of low level of continuum and also smaller line broadening. This is attributed to the lower density of the plasma in the case of short laser pulses due to the defocusing effects which limits the intensity of the pulse in the interaction region and thus prevents further multiphoton/tunnel ionization of the gas.<ref>{{cite journal|doi=10.1016/s0030-4018(00)00903-2|title=Focusing limits of intense ultrafast laser pulses in a high pressure gas: Road to new spectroscopic source|year=2000|last1=Talebpour|first1=A.|last2=Abdel-Fattah|first2=M.|last3=Chin|first3=S.L|journal=Optics Communications|volume=183|issue=5–6|pages=479–484|bibcode=2000OptCo.183..479T}}</ref><ref>{{cite journal|doi=10.1140/epjd/e2009-00260-0|title=On the focusing limit of high-power femtosecond laser pulse propagation in air|year=2009|last1=Geints|first1=Yu. E.|last2=Zemlyanov|first2=A. A.|journal=The European Physical Journal D|volume=55|issue=3|pages=745–754|bibcode=2009EPJD...55..745G|s2cid=121616255}}</ref>
Geints, Y. E., & Zemlyanov, A. A. (2009). On the focusing limit of high-power femtosecond laser pulse propagation in air. The European Physical Journal D,55(3), 745-754.
</ref>


== Line intensity ==
== Line intensity ==
For an optically thin plasma composed of a single, neutral atomic species in local thermal equilibrium (LTE), the density of photons emitted by a transition from level ''i'' to level ''j'' is<ref>{{Cite book|title=Laser-induced breakdown spectroscopy : fundamentals and applications|last=Reinhard.|first=Noll|date=2012|publisher=Springer-Verlag Berlin Heidelberg|isbn=9783642206672|oclc=773812336}}</ref>
For an optically thin plasma composed of a single, neutral atomic species in local thermal equilibrium (LTE), the density of photons emitted by a transition from level ''i'' to level ''j'' is<ref>{{Cite book|title=Laser-induced breakdown spectroscopy: fundamentals and applications|last=Reinhard.|first=Noll|date=2012|publisher=Springer-Verlag Berlin Heidelberg|isbn=978-3-642-20667-2|oclc=773812336}}</ref>


<math>I_{ij}(\lambda)=\frac{1}{4\pi} n_0 A_{ij}\frac{ g_i \exp^{-E_i/k_B T}}{U(T)} I(\lambda)</math>
<math>I_{ij}(\lambda)=\frac{1}{4\pi} n_0 A_{ij}\frac{ g_i \exp^{-E_i/k_B T}}{U(T)} I(\lambda)</math>
Line 82: Line 45:
* <math>A_{ij}</math> is the transition probability between level ''i'' and level ''j'' (in s<sup>−1</sup>)
* <math>A_{ij}</math> is the transition probability between level ''i'' and level ''j'' (in s<sup>−1</sup>)
* <math>g_i</math> is the degeneracy of the upper level ''i'' (2''J''+1)
* <math>g_i</math> is the degeneracy of the upper level ''i'' (2''J''+1)
* <math>U(T)</math> is the partition function (in s<sup>−1</sup>)
* <math>U(T)</math> is the partition function (unitless)
* <math>E_i</math> is the energy level of the upper level ''i'' (in eV)
* <math>E_i</math> is the energy level of the upper level ''i'' (in eV)
* <math>k_B</math> is the [[Boltzmann constant]] (in eV/K)
* <math>k_B</math> is the [[Boltzmann constant]] (in eV/K)
Line 94: Line 57:


==LIBS for food analysis==
==LIBS for food analysis==
Recently, LIBS has been investigated as a fast, micro-destructive food analysis tool. It is considered a potential analytical tool for qualitative and quantitative chemical analysis, making it suitable as a PAT (Process Analytical Technology) or portable tool. Milk, bakery products, tea, vegetable oils, water, cereals, flour, potatoes, palm date and different types of meat have been analyzed using LIBS.<ref name="LIBS Rev">{{cite journal |last1=Markiewicz-Keszycka |first1=Maria |display-authors=etal |title=Laser-induced breakdown spectroscopy (LIBS) for food analysis: A review |journal=Trends in Food Science & Technology |date=2017 |volume=65 |pages=80–93 |doi=10.1016/j.tifs.2017.05.005}}</ref> Few studies have shown its potential as an adulteration detection tool for certain foods.<ref>{{cite journal |last1=Sezer |first1=Banu |display-authors=etal |title=Identification of milk fraud using laser-induced breakdown spectroscopy (LIBS) |journal=International Dairy Journal |date=2018 |volume=81 |pages=1–7 |doi=10.1016/j.idairyj.2017.12.005}}</ref><ref name="Yash LIBS">{{cite journal |last1=Dixit |first1=Yash |display-authors=etal |title=Laser induced breakdown spectroscopy for quantification of sodium and potassium in minced beef: a potential technique for detecting beef kidney adulteration |journal=Analytical Methods |date=2017 |volume=9 |issue=22 |pages=3314–3322 |doi=10.1039/C7AY00757D|url=https://arrow.dit.ie/schfsehart/291 }}</ref> LIBS has also been evaluated as a promising elemental imaging technique in meat.<ref name="LIBS imaging">{{cite journal |last1=Dixit |first1=Yash |display-authors=etal |title=Introduction to laser induced breakdown spectroscopy imaging in food: Salt diffusion in meat |journal=Journal of Food Engineering |date=2018 |volume=216 |pages=120–124 |doi=10.1016/j.jfoodeng.2017.08.010|url=https://arrow.dit.ie/schfsehart/273 }}</ref>
Recently, LIBS has been investigated as a fast, micro-destructive food analysis tool. It is considered a potential analytical tool for qualitative and quantitative chemical analysis, making it suitable as a PAT (Process Analytical Technology) or portable tool. Milk, bakery products, tea, vegetable oils, water, cereals, flour, potatoes, palm date and different types of meat have been analyzed using LIBS.<ref name="LIBS Rev">{{cite journal |last1=Markiewicz-Keszycka |first1=Maria |display-authors=etal |title=Laser-induced breakdown spectroscopy (LIBS) for food analysis: A review |journal=Trends in Food Science & Technology |date=2017 |volume=65 |pages=80–93 |doi=10.1016/j.tifs.2017.05.005|url=https://arrow.tudublin.ie/cgi/viewcontent.cgi?article=1508&context=schfsehart |doi-access=free }}</ref> Few studies have shown its potential as an adulteration detection tool for certain foods.<ref>{{cite journal |last1=Sezer |first1=Banu |display-authors=etal |title=Identification of milk fraud using laser-induced breakdown spectroscopy (LIBS) |journal=International Dairy Journal |date=2018 |volume=81 |pages=1–7 |doi=10.1016/j.idairyj.2017.12.005}}</ref><ref name="Yash LIBS">{{cite journal |last1=Dixit |first1=Yash |display-authors=etal |title=Laser induced breakdown spectroscopy for quantification of sodium and potassium in minced beef: a potential technique for detecting beef kidney adulteration |journal=Analytical Methods |date=2017 |volume=9 |issue=22 |pages=3314–3322 |doi=10.1039/C7AY00757D|url=https://arrow.dit.ie/schfsehart/291 }}</ref> LIBS has also been evaluated as a promising elemental imaging technique in meat.<ref name="LIBS imaging">{{cite journal |last1=Dixit |first1=Yash |display-authors=etal |title=Introduction to laser induced breakdown spectroscopy imaging in food: Salt diffusion in meat |journal=Journal of Food Engineering |date=2018 |volume=216 |pages=120–124 |doi=10.1016/j.jfoodeng.2017.08.010|url=https://arrow.dit.ie/schfsehart/273 |doi-access=free }}</ref>


In 2019, researchers of the [[University of York]] and of the [[Liverpool John Moores University]] employed LIBS for studying 12 European oysters (''[[Ostrea edulis]]'', [[Carl Linnaeus|Linnaeus]], 1758) from the Late [[Mesolithic]] shell midden at Conors Island ([[Republic of Ireland]]). The results highlighted the applicability of LIBS to determine prehistoric seasonality practices as well as biological age and growth at an improved rate and reduced cost than was previously achievable<ref>{{Cite journal|last=Hausmann|first=Niklas|last2=Robson|first2=Harry K.|last3=Hunt|first3=Chris|date=2019-09-30|title=Annual Growth Patterns and Interspecimen Variability in Mg/Ca Records of Archaeological Ostrea edulis (European Oyster) from the Late Mesolithic Site of Conors Island|url=http://www.openquaternary.com/articles/10.5334/oq.59/|journal=Open Quaternary|language=en|volume=5|issue=1|pages=9|doi=10.5334/oq.59|issn=2055-298X}}</ref>.
In 2019, researchers of the [[University of York]] and of the [[Liverpool John Moores University]] employed LIBS for studying 12 European oysters (''[[Ostrea edulis]]'', [[Carl Linnaeus|Linnaeus]], 1758) from the Late [[Mesolithic]] shell midden at Conors Island ([[Republic of Ireland]]). The results highlighted the applicability of LIBS to determine prehistoric seasonality practices as well as biological age and growth at an improved rate and reduced cost than was previously achievable.<ref>{{Cite journal |last1=Hausmann |first1=N. |last2=Prendergast |first2=A. L. |last3=Lemonis |first3=A. |last4=Zech |first4=J. |last5=Roberts |first5=P. |last6=Siozos |first6=P. |last7=Anglos |first7=D. |date=2019-03-06 |title=Extensive elemental mapping unlocks Mg/Ca ratios as climate proxy in seasonal records of Mediterranean limpets |journal=Scientific Reports |language=en |volume=9 |issue=1 |page=3698 |doi=10.1038/s41598-019-39959-9 |issn=2045-2322 |pmc=6403426 |pmid=30842602|bibcode=2019NatSR...9.3698H }}</ref><ref>{{Cite journal|last1=Hausmann|first1=Niklas|last2=Robson|first2=Harry K.|last3=Hunt|first3=Chris|date=2019-09-30|title=Annual Growth Patterns and Interspecimen Variability in Mg/Ca Records of Archaeological Ostrea edulis (European Oyster) from the Late Mesolithic Site of Conors Island|journal=Open Quaternary|language=en|volume=5|issue=1|page=9|doi=10.5334/oq.59|issn=2055-298X|doi-access=free}}</ref>


==See also==
==See also==
*[[Spectroscopy]]
*[[Atomic spectroscopy]]
*[[Atomic spectroscopy]]
*[[Raman spectroscopy]]
*[[Laser ablation]]
*[[Laser-induced fluorescence]]
*[[Laser-induced fluorescence]]
*[[List of plasma (physics) articles]]
*[[List of surface analysis methods]]
*[[List of surface analysis methods]]
*[[Laser ablation]]
*[[Photoacoustic spectroscopy]]
*[[Photoacoustic spectroscopy]]
*[[Raman spectroscopy]]
*[[Spectroscopy]]


==References==
==References==
{{reflist}}
{{reflist}}
*{{cite journal|last1=Lee|first1=Won-Bae|last2=Wu|first2=Jianyong|last3=Lee|first3=Yong-Ill|last4=Sneddon|first4=Joseph|title=Recent Applications of Laser-Induced Breakdown Spectrometry: A Review of Material Approaches|journal=Applied Spectroscopy Reviews|volume=39|issue=1|date=2004|pages=27–97|issn=0570-4928|doi=10.1081/ASR-120028868|bibcode=2004ApSRv..39...27L}}
*{{cite journal|last1=Lee|first1=Won-Bae|last2=Wu|first2=Jianyong|last3=Lee|first3=Yong-Ill|last4=Sneddon|first4=Joseph|title=Recent Applications of Laser-Induced Breakdown Spectrometry: A Review of Material Approaches|journal=Applied Spectroscopy Reviews|volume=39|issue=1|date=2004|pages=27–97|issn=0570-4928|doi=10.1081/ASR-120028868|bibcode=2004ApSRv..39...27L|s2cid=98545359}}
*{{cite journal|last1=Noll|first1=Reinhard|last2=Bette|first2=Holger|last3=Brysch|first3=Adriane|last4=Kraushaar |first4=Marc |last5=Mönch |first5=Ingo |last6=Peter|first6=Laszlo|last7=Sturm|first7=Volker|title=Laser-induced breakdown spectrometry — applications for production control and quality assurance in the steel industry|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=56|issue=6|date=2001|pages=637–649|issn=0584-8547|doi=10.1016/S0584-8547(01)00214-2|bibcode=2001AcSpe..56..637N}}
*{{cite journal|last1=Noll|first1=Reinhard|last2=Bette|first2=Holger|last3=Brysch|first3=Adriane|last4=Kraushaar |first4=Marc |last5=Mönch |first5=Ingo |last6=Peter|first6=Laszlo|last7=Sturm|first7=Volker|title=Laser-induced breakdown spectrometry — applications for production control and quality assurance in the steel industry|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=56|issue=6|date=2001|pages=637–649|issn=0584-8547|doi=10.1016/S0584-8547(01)00214-2|bibcode=2001AcSpe..56..637N}}


==Further reading==
==Further reading==
*{{Cite book|author1=Andrzej W. Miziolek |author2=Vincenzo Palleschi |author3=Israel Schechter |title=Laser Induced Breakdown Spectroscopy|location=New York|publisher= Cambridge University Press|date= 2006| isbn= 0-521-85274-9}}
*{{Cite book|author1=Andrzej W. Miziolek |author2=Vincenzo Palleschi |author3=Israel Schechter |title=Laser Induced Breakdown Spectroscopy|location=New York|publisher= Cambridge University Press|date= 2006| isbn= 0-521-85274-9}}
*{{Cite journal|title=Microchip Laser Induced Breakdown Spectroscopy: Preliminary Feasibility Investigation|journal=Applied Spectroscopy|date=2004|volume=58|issue=7|pages=762–769|url=http://www.s-a-s.org/journal/viewer/abstract/4678/|doi=10.1366/0003702041389427|pmid=15282039|last1=Gornushkin|first1=I.B.|last2=Amponsah-Manager|first2=K.|last3=Smith|first3=B.W.|last4=Omenetto|first4=N.|last5=Winefordner|first5=J.D.|url-status=dead|archiveurl=https://archive.is/20130415182955/http://www.s-a-s.org/journal/viewer/abstract/4678/|archivedate=2013-04-15|bibcode=2004ApSpe..58..762G}}
*{{Cite journal|title=Microchip Laser Induced Breakdown Spectroscopy: Preliminary Feasibility Investigation|journal=Applied Spectroscopy|date=2004|volume=58|issue=7|pages=762–769|url=http://www.s-a-s.org/journal/viewer/abstract/4678/|doi=10.1366/0003702041389427|pmid=15282039|last1=Gornushkin|first1=I.B.|last2=Amponsah-Manager|first2=K.|last3=Smith|first3=B.W.|last4=Omenetto|first4=N.|last5=Winefordner|first5=J.D.|archive-url=https://archive.today/20130415182955/http://www.s-a-s.org/journal/viewer/abstract/4678/|archive-date=2013-04-15|bibcode=2004ApSpe..58..762G|s2cid=41416641}}
*{{Cite journal|doi=10.1039/B419109A|title=Microchip laser ablation of metals: Investigation of the ablation process in view of its application to laser-induced breakdown spectroscopy|date=2005|last1=Amponsah-Manager|first1=K.|last2=Omenetto|first2=N.|last3=Smith|first3=B. W.|last4=Gornushkin|first4=I. B.|last5=Winefordner|first5=J. D.|journal=Journal of Analytical Atomic Spectrometry|volume=20|issue=6|pages=544 }}
*{{Cite journal|doi=10.1039/B419109A|title=Microchip laser ablation of metals: Investigation of the ablation process in view of its application to laser-induced breakdown spectroscopy|date=2005|last1=Amponsah-Manager|first1=K.|last2=Omenetto|first2=N.|last3=Smith|first3=B. W.|last4=Gornushkin|first4=I. B.|last5=Winefordner|first5=J. D.|journal=Journal of Analytical Atomic Spectrometry|volume=20|issue=6|page=544 }}
*{{Cite journal|doi=10.1039/B419173K|title=Quantitative analysis of low-alloy steel by microchip laser induced breakdown spectroscopy|date=2005|last1=Lopez-Moreno|first1=C.|last2=Amponsah-Manager|first2=K.|last3=Smith|first3=B. W.|last4=Gornushkin|first4=I. B.|last5=Omenetto|first5=N.|last6=Palanco|first6=S.|last7=Laserna|first7=J. J.|last8=Winefordner|first8=J. D.|journal=Journal of Analytical Atomic Spectrometry|volume=20|issue=6|pages=552 }}
*{{Cite journal|doi=10.1039/B419173K|title=Quantitative analysis of low-alloy steel by microchip laser induced breakdown spectroscopy|date=2005|last1=Lopez-Moreno|first1=C.|last2=Amponsah-Manager|first2=K.|last3=Smith|first3=B. W.|last4=Gornushkin|first4=I. B.|last5=Omenetto|first5=N.|last6=Palanco|first6=S.|last7=Laserna|first7=J. J.|last8=Winefordner|first8=J. D.|journal=Journal of Analytical Atomic Spectrometry|volume=20|issue=6|page=552 |s2cid=39938942}}
*{{Cite journal|doi=10.1088/0022-3727/37/8/018|title=High speed laser-induced breakdown spectrometry for scanning microanalysis|date=2004|last1=Bette|first1=H|last2=Noll|first2=R|journal=Journal of Physics D: Applied Physics|volume=37|issue=8|pages=1281|bibcode=2004JPhD...37.1281B}}
*{{Cite journal|doi=10.1088/0022-3727/37/8/018|title=High speed laser-induced breakdown spectrometry for scanning microanalysis|date=2004|last1=Bette|first1=H|last2=Noll|first2=R|journal=Journal of Physics D: Applied Physics|volume=37|issue=8|page=1281|bibcode=2004JPhD...37.1281B|s2cid=250750854 }}
*{{Cite journal|doi=10.1007/s00216-006-0347-z|title=New approach to online monitoring of the Al depth profile of the hot-dip galvanised sheet steel using LIBS|date=2006|last1=Balzer|first1=Herbert|last2=Hoehne|first2=Manuela|last3=Noll|first3=Reinhard|last4=Sturm|first4=Volker|journal=Analytical and Bioanalytical Chemistry|volume=385|issue=2|pages=225–33|pmid=16570144}}
*{{Cite journal|doi=10.1007/s00216-006-0347-z|title=New approach to online monitoring of the Al depth profile of the hot-dip galvanised sheet steel using LIBS|date=2006|last1=Balzer|first1=Herbert|last2=Hoehne|first2=Manuela|last3=Noll|first3=Reinhard|last4=Sturm|first4=Volker|journal=Analytical and Bioanalytical Chemistry|volume=385|issue=2|pages=225–33|pmid=16570144|s2cid=42607960}}
*{{Cite journal|title=Steel analysis with laser-induced breakdown spectrometry in the vacuum ultraviolet|journal= Appl. Spectroscopy|date= 2000|volume= 54|pages=1275–1278|url=http://www.opticsinfobase.org/as/abstract.cfm?URI=as-54-9-1275|doi=10.1366/0003702001951183|issue=9|last1=Sturm|first1=V.|last2=Peter|first2=L.|last3=Noll|first3=R.|bibcode=2000ApSpe..54.1275S}}
*{{Cite journal|title=Steel analysis with laser-induced breakdown spectrometry in the vacuum ultraviolet|journal= Applied Spectroscopy|date= 2000|volume= 54|pages=1275–1278|url=http://www.opticsinfobase.org/as/abstract.cfm?URI=as-54-9-1275|doi=10.1366/0003702001951183|issue=9|last1=Sturm|first1=V.|last2=Peter|first2=L.|last3=Noll|first3=R.|bibcode=2000ApSpe..54.1275S|s2cid= 32765892}}
*{{Cite journal|doi=10.1016/j.sab.2003.11.006|title=Laser-induced plasma spectrometry: Truly a surface analytical tool|date=2004|last1=Vadillo|first1=José M.|last2=Laserna|first2=J.Javier|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=59|issue=2|pages=147 |bibcode=2004AcSpe..59..147V}}
*{{Cite journal|doi=10.1016/j.sab.2003.11.006|title=Laser-induced plasma spectrometry: Truly a surface analytical tool|date=2004|last1=Vadillo|first1=José M.|last2=Laserna|first2=J.Javier|journal=Spectrochimica Acta Part B: Atomic Spectroscopy|volume=59|issue=2|page=147 |bibcode=2004AcSpe..59..147V}}
*{{Cite journal|doi=10.1039/b714219f|title=Quantitative molecular analysis with molecular bands emission using laser-induced breakdown spectroscopy and chemometrics|date=2008|last1=Doucet|first1=François R.|last2=Faustino|first2=Patrick J.|last3=Sabsabi|first3=Mohamad|last4=Lyon|first4=Robbe C.|journal=Journal of Analytical Atomic Spectrometry|volume=23|issue=5|pages=694}}
*{{Cite journal|doi=10.1039/b714219f|title=Quantitative molecular analysis with molecular bands emission using laser-induced breakdown spectroscopy and chemometrics|date=2008|last1=Doucet|first1=François R.|last2=Faustino|first2=Patrick J.|last3=Sabsabi|first3=Mohamad|last4=Lyon|first4=Robbe C.|journal=Journal of Analytical Atomic Spectrometry|volume=23|issue=5|page=694|s2cid=97020157 |url=https://nrc-publications.canada.ca/eng/view/accepted/?id=be2795ea-0e53-488c-9b00-209d48a9a8ff}}
*{{cite journal|url=http://www.photonics.su/journal/article/2606|author= В.Копачевский, В.Шпектор, Д.Клемято, В.Бойков, М.Кривошеева, Л.Боброва. |title=Количественный анализ состава тарных стекол анализатором LEA S500|journal= Фотоника |date=2008|language=Russian|issue=1|pages=38–40}}
*{{cite journal|url=http://www.photonics.su/journal/article/2606|author= В.Копачевский, В.Шпектор, Д.Клемято, В.Бойков, М.Кривошеева, Л.Боброва. |title=Количественный анализ состава тарных стекол анализатором LEA S500|journal= Фотоника |date=2008|language=ru|issue=1|pages=38–40}}
*{{cite book |first=Reinhard|last= Noll |title=Laser-Induced Breakdown Spectroscopy: Fundamentals and Applications |publisher=Springer |location=Berlin |date=2012 |pages= |isbn=978-3-642-20667-2 |oclc= |doi= }}
*{{cite book |first=Reinhard|last= Noll |title=Laser-Induced Breakdown Spectroscopy: Fundamentals and Applications |publisher=Springer |location=Berlin |date=2012 |isbn=978-3-642-20667-2 }}


==External links==
==External links==
* [https://pml.nist.gov/PhysRefData/ASD/LIBS/libs-form.html NIST LIBS Database]
* [https://pml.nist.gov/PhysRefData/ASD/LIBS/libs-form.html NIST LIBS Database]


{{Branches of spectroscopy}}
{{BranchesofSpectroscopy}}
{{lasers}}
{{Lasers}}


{{DEFAULTSORT:Laser-Induced Breakdown Spectroscopy}}
[[Category:Scientific techniques]]
[[Category:Scientific techniques]]
[[Category:Spectroscopy]]
[[Category:Spectroscopy]]
[[Category:Emission spectroscopy]]

Latest revision as of 17:42, 12 December 2023

Schematic of a LIBS system – Courtesy of US Army Research Laboratory

Laser-induced breakdown spectroscopy (LIBS) is a type of atomic emission spectroscopy which uses a highly energetic laser pulse as the excitation source.[1][2] The laser is focused to form a plasma, which atomizes and excites samples. The formation of the plasma only begins when the focused laser achieves a certain threshold for optical breakdown, which generally depends on the environment and the target material.[3]

2000s developments

[edit]

From 2000 to 2010, the U.S. Army Research Laboratory (ARL) researched potential extensions to LIBS technology, which focused on hazardous material detection.[4][5] Applications investigated at ARL included the standoff detection of explosive residues and other hazardous materials, plastic landmine discrimination, and material characterization of various metal alloys and polymers. Results presented by ARL suggest that LIBS may be able to discriminate between energetic and non-energetic materials.[6]

Research

[edit]

Broadband high-resolution spectrometers were developed in 2000 and commercialized in 2003. Designed for material analysis, the spectrometer allowed the LIBS system to be sensitive to chemical elements in low concentration.[7]

ARL LIBS applications studied from 2000 to 2010 included:[5]

  • Tested for detection of Halon alternative agents
  • Tested a field-portable LIBS system for the detection of lead in soil and paint
  • Studied the spectral emission of aluminum and aluminum oxides from bulk aluminum in different bath gases
  • Performed kinetic modeling of LIBS plumes
  • Demonstrated the detection and discrimination of geological materials, plastic landmines, explosives, and chemical and biological warfare agent surrogates

ARL LIBS prototypes studied during this period included:[5]

  • Laboratory LIBS setup
  • Commercial LIBS system
  • Man-portable LIBS device
  • Standoff LIBS system developed for 100+ m detection and discriminate on of explosive residues.

2010s developments

[edit]

LIBS is one of several analytical techniques that can be deployed in the field as opposed to pure laboratory techniques e.g. spark OES. As of 2015, recent research on LIBS focuses on compact and (man-)portable systems. Some industrial applications of LIBS include the detection of material mix-ups,[8] analysis of inclusions in steel, analysis of slags in secondary metallurgy,[9] analysis of combustion processes,[10] and high-speed identification of scrap pieces for material-specific recycling tasks. Armed with data analysis techniques, this technique is being extended to pharmaceutical samples.[11][12]

LIBS using short laser pulses

[edit]

Following multiphoton or tunnel ionization the electron is being accelerated by inverse Bremsstrahlung and can collide with the nearby molecules and generate new electrons through collisions. If the pulse duration is long, the newly ionized electrons can be accelerated and eventually avalanche or cascade ionization follows. Once the density of the electrons reaches a critical value, breakdown occurs and high density plasma is created which has no memory of the laser pulse. So, the criterion for the shortness of a pulse in dense media is as follows: A pulse interacting with a dense matter is considered to be short if during the interaction the threshold for the avalanche ionization is not reached. At the first glance this definition may appear to be too limiting. Fortunately, due to the delicately balanced behavior of the pulses in dense media, the threshold cannot be reached easily.[citation needed] The phenomenon responsible for the balance is the intensity clamping[13] through the onset of filamentation process during the propagation of strong laser pulses in dense media.

A potentially important development to LIBS involves the use of a short laser pulse as a spectroscopic source.[14] In this method, a plasma column is created as a result of focusing ultrafast laser pulses in a gas. The self-luminous plasma is far superior in terms of low level of continuum and also smaller line broadening. This is attributed to the lower density of the plasma in the case of short laser pulses due to the defocusing effects which limits the intensity of the pulse in the interaction region and thus prevents further multiphoton/tunnel ionization of the gas.[15][16]

Line intensity

[edit]

For an optically thin plasma composed of a single, neutral atomic species in local thermal equilibrium (LTE), the density of photons emitted by a transition from level i to level j is[17]

where :

  • is the emission rate density of photons (in m−3 sr−1 s−1)
  • is the number of neutral atoms in the plasma (in m−3)
  • is the transition probability between level i and level j (in s−1)
  • is the degeneracy of the upper level i (2J+1)
  • is the partition function (unitless)
  • is the energy level of the upper level i (in eV)
  • is the Boltzmann constant (in eV/K)
  • is the temperature (in K)
  • is the line profile such that
  • is the wavelength (in nm)

The partition function is the statistical occupation fraction of every level of the atomic species :

LIBS for food analysis

[edit]

Recently, LIBS has been investigated as a fast, micro-destructive food analysis tool. It is considered a potential analytical tool for qualitative and quantitative chemical analysis, making it suitable as a PAT (Process Analytical Technology) or portable tool. Milk, bakery products, tea, vegetable oils, water, cereals, flour, potatoes, palm date and different types of meat have been analyzed using LIBS.[18] Few studies have shown its potential as an adulteration detection tool for certain foods.[19][20] LIBS has also been evaluated as a promising elemental imaging technique in meat.[21]

In 2019, researchers of the University of York and of the Liverpool John Moores University employed LIBS for studying 12 European oysters (Ostrea edulis, Linnaeus, 1758) from the Late Mesolithic shell midden at Conors Island (Republic of Ireland). The results highlighted the applicability of LIBS to determine prehistoric seasonality practices as well as biological age and growth at an improved rate and reduced cost than was previously achievable.[22][23]

See also

[edit]

References

[edit]
  1. ^ Radziemski, Leon J.; Cremers, David A. (2006). Handbook of laser-induced breakdown spectroscopy. New York: John Wiley. ISBN 0-470-09299-8.
  2. ^ Schechter, Israel; Miziolek, Andrzej W.; Vincenzo Palleschi (2006). Laser-induced breakdown spectroscopy (LIBS): fundamentals and applications. Cambridge, UK: Cambridge University Press. ISBN 0-521-85274-9.
  3. ^ J. P. Singh and S. N. Thakur, Laser-Induced Breakdown Spectroscopy, 1st ed.. (Elsevier, 2007).
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Further reading

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