TY - JOUR
T1 - Gamma-ray interaction in Ge
T2 - A Monte Carlo simulation
AU - Gao, F.
AU - Campbell, L. W.
AU - Devanathan, R.
AU - Xie, Y. L.
AU - Zhang, Y.
AU - Peurrung, A. J.
AU - Weber, W. J.
N1 - Funding Information:
This research was supported by the Radiation Detection Materials Discovery (RDMD) initiative that is a Laboratory Directed Research and Development Program at the Pacific Northwest National Laboratory (PNNL). The authors also wish to thank the Molecular Science Computing Facility in the Environmental Molecular Sciences Laboratory for a grant of computer time at PNNL, a multiprogram national laboratory operated by Battelle for the US Department of Energy under Contract DE-AC05-76RL01830.
PY - 2007/2
Y1 - 2007/2
N2 - The interactions of X-ray and gamma-ray photons with materials are of fundamental interest to many fields. The interactions of these primary photons with atoms result in the creation of fast electrons. The subsequent electron-solid interactions involve the partitioning of energy loss into different quantum mechanical processes that are important to determining the mean energy required to create an electron-hole pair, W, and the intrinsic variance (or Fano factor, F) for radiation detectors. In the present work, a Monte Carlo method previously developed has been employed to simulate the interaction of photons with Ge over the energy range from 50 eV to ∼2 MeV and the subsequent electron cascades. Various quantum mechanical processes for energy loss of fast electrons, which control the broadening of variance, are investigated in detail. At energies lower than 1 keV, W generally decreases with increasing photon energy from 2.95 to 2.75 eV in Ge, whereas it has a constant value of 2.64 eV for higher energies. Also, the function, F, decreases with increasing photon energy. Above the L shell edge, F has a value of 0.11 that is smaller than that in Si (0.14). However, F exhibits a sawtooth variation, and discontinuities at the shell edges that follow the photoelectric cross sections. These results are in good agreement with experimental measurements. The simulated distribution indicates that the interband transition and plasmon excitation are the most important mechanisms of electron-hole pair creation in Ge, while core shell ionization appears to be significant only at high energies.
AB - The interactions of X-ray and gamma-ray photons with materials are of fundamental interest to many fields. The interactions of these primary photons with atoms result in the creation of fast electrons. The subsequent electron-solid interactions involve the partitioning of energy loss into different quantum mechanical processes that are important to determining the mean energy required to create an electron-hole pair, W, and the intrinsic variance (or Fano factor, F) for radiation detectors. In the present work, a Monte Carlo method previously developed has been employed to simulate the interaction of photons with Ge over the energy range from 50 eV to ∼2 MeV and the subsequent electron cascades. Various quantum mechanical processes for energy loss of fast electrons, which control the broadening of variance, are investigated in detail. At energies lower than 1 keV, W generally decreases with increasing photon energy from 2.95 to 2.75 eV in Ge, whereas it has a constant value of 2.64 eV for higher energies. Also, the function, F, decreases with increasing photon energy. Above the L shell edge, F has a value of 0.11 that is smaller than that in Si (0.14). However, F exhibits a sawtooth variation, and discontinuities at the shell edges that follow the photoelectric cross sections. These results are in good agreement with experimental measurements. The simulated distribution indicates that the interband transition and plasmon excitation are the most important mechanisms of electron-hole pair creation in Ge, while core shell ionization appears to be significant only at high energies.
KW - Computer simulation
KW - Electron cascade
KW - Fano factor
KW - Germanium
KW - Monte Carlo
UR - https://www.scopus.com/pages/publications/33846908477
U2 - 10.1016/j.nimb.2006.11.031
DO - 10.1016/j.nimb.2006.11.031
M3 - Article
AN - SCOPUS:33846908477
SN - 0168-583X
VL - 255
SP - 286
EP - 290
JO - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
JF - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
IS - 1 SPEC. ISS.
ER -