TY - GEN
T1 - Nuclear resonance fluorescence using different photon sources
AU - Warren, Glen
AU - Caggiano, Joseph
AU - Ahmed, Mohammad
AU - Bertozzi, William
AU - Hunt, Alan
AU - Johnson, James
AU - Jones, James
AU - Korbly, Stephen
AU - Reedy, Edward
AU - Seipel, Heather
AU - Stave, Sean
AU - Watson, Scott
AU - Weller, Henry
PY - 2008
Y1 - 2008
N2 - Nuclear resonance fluorescence (NRF) is a photon-based active interrogation approach that provides isotope-specific signatures that can be used to detect and characterize samples. As NRF systems are designed to address specific applications, an obvious first question to address is the type of photon source to be employed for the application. Our collaboration has conducted a series of NRF measurements using different photon sources to begin to examine this issue. The measurements were designed to be as similar as possible to facilitate a straightforward comparison of the different sources. Measurements were conducted with a high-duty factor electron accelerator using bremsstrahlung photons, with a pulsed linear accelerator using bremsstrahlung photons, and with a narrow bandwidth photon source using Compton backscattered photons. We present our observations on the advantages and disadvantages of each photon source type. Issues such as signal rate, the signal-to-noise ratio, and absorbed dose are discussed.
AB - Nuclear resonance fluorescence (NRF) is a photon-based active interrogation approach that provides isotope-specific signatures that can be used to detect and characterize samples. As NRF systems are designed to address specific applications, an obvious first question to address is the type of photon source to be employed for the application. Our collaboration has conducted a series of NRF measurements using different photon sources to begin to examine this issue. The measurements were designed to be as similar as possible to facilitate a straightforward comparison of the different sources. Measurements were conducted with a high-duty factor electron accelerator using bremsstrahlung photons, with a pulsed linear accelerator using bremsstrahlung photons, and with a narrow bandwidth photon source using Compton backscattered photons. We present our observations on the advantages and disadvantages of each photon source type. Issues such as signal rate, the signal-to-noise ratio, and absorbed dose are discussed.
UR - https://www.scopus.com/pages/publications/67649240512
U2 - 10.1109/NSSMIC.2008.4775055
DO - 10.1109/NSSMIC.2008.4775055
M3 - Conference contribution
AN - SCOPUS:67649240512
SN - 9781424427154
T3 - IEEE Nuclear Science Symposium Conference Record
SP - 3318
EP - 3323
BT - 2008 IEEE Nuclear Science Symposium Conference Record, NSS/MIC 2008
T2 - 2008 IEEE Nuclear Science Symposium Conference Record, NSS/MIC 2008
Y2 - 19 October 2008 through 25 October 2008
ER -