Neutron stimulated emission computed tomography: Difference between revisions
No edit summary |
No edit summary |
||
| Line 2: | Line 2: | ||
== NSECT mechanism == |
== NSECT mechanism == |
||
A given [[atomic nucleus]], defined by its [[Proton_number | proton]] and [[Neutron_number | neutron numbers]], is a [[Quantization_(physics) | quantized]] system with a [[Nuclear_shell_model | set of characteristic higher energy levels]] that it can occupy as a [[nuclear isomer]]. When the [[nucleus]] in its [[ground state]] is struck by a [[Fast_neutron#Fast_neutrons|fast neutron]] with [[kinetic energy]] greater than that of its first excited state, it can undergo an [[isomeric transition | isomeric transition]] to one of its [[excited states]] by receiving the necessary energy from the fast neutron through [[Inelastic_scattering|inelastic scatter]]. Promptly (on the order of picoseconds, on average<ref>{{cite web|title=Isomeric transition|url=http://en.wikipedia.org/wiki/Isomeric_transition|work=Wikipedia|accessdate=08/03/2011}}</ref>) after excitation, the excited nuclear isomer de-excites (either directly or through a series of cascades) to the ground state, emitting a characteristic [[Gamma_rays|gamma ray]] for each decay transition with energy equal to the difference in the energy levels involved (see [[Induced_gamma_emission | induced gamma emission]]). After irradiating the sample with neutrons, the measured number of emitted gamma rays of energy characteristic to the nucleus of interest is directly proportional to the number of such nuclei along the incident neutron beam trajectory. After repeating the measurement for neutron beam incidence at positions around the sample, an image of the distribution of the nuclei in the sample can be reconstructed using [[tomography]]. |
A given [[atomic nucleus]], defined by its [[Proton_number | proton]] and [[Neutron_number | neutron numbers]], is a [[Quantization_(physics) | quantized]] system with a [[Nuclear_shell_model | set of characteristic higher energy levels]] that it can occupy as a [[nuclear isomer]]. When the [[nucleus]] in its [[ground state]] is struck by a [[Fast_neutron#Fast_neutrons|fast neutron]] with [[kinetic energy]] greater than that of its first excited state, it can undergo an [[isomeric transition | isomeric transition]] to one of its [[Excited_state | excited states]] by receiving the necessary energy from the fast neutron through [[Inelastic_scattering|inelastic scatter]]. Promptly (on the order of picoseconds, on average<ref>{{cite web|title=Isomeric transition|url=http://en.wikipedia.org/wiki/Isomeric_transition|work=Wikipedia|accessdate=08/03/2011}}</ref>) after excitation, the excited nuclear isomer de-excites (either directly or through a series of cascades) to the ground state, emitting a characteristic [[Gamma_rays|gamma ray]] for each decay transition with energy equal to the difference in the energy levels involved (see [[Induced_gamma_emission | induced gamma emission]]). After irradiating the sample with neutrons, the measured number of emitted gamma rays of energy characteristic to the nucleus of interest is directly proportional to the number of such nuclei along the incident neutron beam trajectory. After repeating the measurement for neutron beam incidence at positions around the sample, an image of the distribution of the nuclei in the sample can be reconstructed using [[tomography]]. |
||
== Clinical Applications == |
== Clinical Applications == |
||
Revision as of 13:25, 31 August 2011
Neutron stimulated emission computed tomography (NSECT) uses induced gamma emission through neutron inelastic scattering to generate images of the spatial distribution of elements in a sample[1].
NSECT mechanism
A given atomic nucleus, defined by its proton and neutron numbers, is a quantized system with a set of characteristic higher energy levels that it can occupy as a nuclear isomer. When the nucleus in its ground state is struck by a fast neutron with kinetic energy greater than that of its first excited state, it can undergo an isomeric transition to one of its excited states by receiving the necessary energy from the fast neutron through inelastic scatter. Promptly (on the order of picoseconds, on average[2]) after excitation, the excited nuclear isomer de-excites (either directly or through a series of cascades) to the ground state, emitting a characteristic gamma ray for each decay transition with energy equal to the difference in the energy levels involved (see induced gamma emission). After irradiating the sample with neutrons, the measured number of emitted gamma rays of energy characteristic to the nucleus of interest is directly proportional to the number of such nuclei along the incident neutron beam trajectory. After repeating the measurement for neutron beam incidence at positions around the sample, an image of the distribution of the nuclei in the sample can be reconstructed using tomography.
Clinical Applications
NSECT has been shown to be effective in detecting liver iron overload disorders[3] and breast cancer [4]. Due to its sensitivity in measuring elemental concentrations, NSECT is currently being developed for cancer staging, among other medical applications.
References
- ^ Kapadia, Anuj (2009). "Neutron Stimulated Emission Computed Tomography: A new spectroscopic technique". Neutron Imaging and Applications: 265–288.
- ^ "Isomeric transition". Wikipedia. Retrieved 08/03/2011.
{{cite web}}: Check date values in:|accessdate=(help) - ^ Kapadia, Anuj (2007). Accuracy and patient dose in neutron stimulated emission computed tomography for diagnosis of iron overload: Simulations in GEANT4. Durham, NC: Duke University.
- ^ Kapadia, Anuj (2008). "Neutron Stimulated Emission Computed Tomography for Diagnosis of Breast Cancer". IEEE Transactions on Nuclear Science. 55 (1): 501–509. doi:10.1109/TNS.2007.909847.
{{cite journal}}: Unknown parameter|coauthors=ignored (|author=suggested) (help)
Further Reading
- NSECT at Ravin Advanced Imaging Laboratories, Duke University
- PDF Floyd CE, Bender JE, Sharma AC, Kapadia A, Xia J, and Harrawood B, Tourassi GD, Lo JY, Crowell A, and Howell C. "Introduction to neutron stimulated emission computed tomography," Physics in medicine and biology. 51:3375. 2006.
- PDFSharma AC, Harrawood BP, Bender JE, Tourassi GD, and Kapadia AJ. "Neutron stimulated emission computed tomography: a Monte Carlo simulation approach,"Physics in medicine and biology. 52:6117. 2007.
- PDFFloyd CE, Kapadia, AJ, et al. "Neutron-stimulated emission computed tomography of a multi-element phantom," Physics in medicine and biology. 53:2313. 2008.