neuSIM4: A comprehensive GEANT4 based neutron simulation code

被引:3
作者
Park, Jeonghyeok [1 ,2 ]
Teh, Fanurs Chi-En [3 ,4 ]
Tsang, ManYee Betty [3 ,4 ]
Brown, Kyle W. [3 ,5 ]
Chajecki, Zbigniew [6 ]
Hong, Byungsik [1 ,2 ]
Lokotko, Taras [3 ]
Lynch, William G. [3 ,4 ]
Wieske, Joeseph M. [3 ,4 ]
Zhu, Kuan [3 ,4 ]
机构
[1] Korea Univ, Ctr Extreme Nucl Matters CENuM, Seoul 02841, South Korea
[2] Korea Univ, Dept Phys, Seoul 02841, South Korea
[3] Michigan State Univ, Facil Rare Isotope Beams FRIB, E Lansing, MI 48824 USA
[4] Michigan State Univ, Dept Phys & Astron, E Lansing, MI 48824 USA
[5] Michigan State Univ, Dept Chem, E Lansing, MI 48824 USA
[6] Western Michigan Univ, Dept Phys, Kalamazoo, MI 49008 USA
基金
新加坡国家研究基金会; 美国国家科学基金会;
关键词
Neutron detector; Neutron detection array; SCINFUL; Transport model; GEANT4; Cascade model; Neutron detection efficiency; Light response functions; HIGH-ENERGY; SCINTILLATOR; ARRAY; DISCRIMINATION; HYDROGEN; SPECTRA;
D O I
10.1016/j.nima.2024.169475
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
A new neu tron SIM ulation program based on the versatile GEANT 4 toolkit, neuSIM4 , has been developed to describe interactions of neutrons in the NE213 liquid scintillator from 0.1 to 3000 MeV. neuSIM4 is designed to accommodate complicated modern detector geometry setups with multiple scintillator detectors, each of which can be outfitted with more than one photo -multiplier. To address a broad spectrum of neutron energies, two new neutron interaction physics models, KSCIN and NxQMD, have been implemented in GEANT4. For neutrons with energy below 110 MeV, we incorporate a total of eleven neutron induced reaction channels on hydrogen and carbon nuclei, including nine carbon inelastic reaction channels, into KSCIN. Beyond 110 MeV, we implement a neutron induced reaction model, NxQMD, in GEANT4. We use its results as reference to evaluate other neutron -interaction physics models in GEANT4. We find that results from an existing cascade physics model (INCL) in GEANT4 agree very well with the results from NxQMD, and results from both codes agree with new and existing light response data. To connect KSCIN to NxQMD or INCL, we introduce a transition region where the contribution of neuSIM4 linearly decreases with corresponding increased contributions from NxQMD or INCL. To demonstrate the application of the new code, we simulate the light response and performance of a 2 x 2 m 2 neutron detector wall array consisting of 25 2m -long scintillation bars. We are able to compare the predicted light response functions to the shape of the experimental response functions and calculate the efficiency of the neutron detector array for neutron energies up to 200 MeV. These simulation results will be pivotal for understanding the performance of modern neutron arrays with intricate geometries, especially in the measurements of neutron energy spectra in heavy -ion reactions.
引用
收藏
页数:8
相关论文
共 43 条
[1]   GEANT4-a simulation toolkit [J].
Agostinelli, S ;
Allison, J ;
Amako, K ;
Apostolakis, J ;
Araujo, H ;
Arce, P ;
Asai, M ;
Axen, D ;
Banerjee, S ;
Barrand, G ;
Behner, F ;
Bellagamba, L ;
Boudreau, J ;
Broglia, L ;
Brunengo, A ;
Burkhardt, H ;
Chauvie, S ;
Chuma, J ;
Chytracek, R ;
Cooperman, G ;
Cosmo, G ;
Degtyarenko, P ;
Dell'Acqua, A ;
Depaola, G ;
Dietrich, D ;
Enami, R ;
Feliciello, A ;
Ferguson, C ;
Fesefeldt, H ;
Folger, G ;
Foppiano, F ;
Forti, A ;
Garelli, S ;
Giani, S ;
Giannitrapani, R ;
Gibin, D ;
Cadenas, JJG ;
González, I ;
Abril, GG ;
Greeniaus, G ;
Greiner, W ;
Grichine, V ;
Grossheim, A ;
Guatelli, S ;
Gumplinger, P ;
Hamatsu, R ;
Hashimoto, K ;
Hasui, H ;
Heikkinen, A ;
Howard, A .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 2003, 506 (03) :250-303
[2]   STUDY OF THE REACTION C-12(N,3-ALPHA)N FROM THRESHOLD TO EN = 35 MEV [J].
ANTOLKOVIC, B ;
SLAUS, I ;
PLENKOVIC, D ;
MACQ, P ;
MEULDERS, JP .
NUCLEAR PHYSICS A, 1983, 394 (1-2) :87-108
[3]   The FLUKA Code: Developments and Challenges for High Energy and Medical Applications [J].
Boehlen, T. T. ;
Cerutti, F. ;
Chin, M. P. W. ;
Fosso, A. ;
Ferrari, A. ;
Ortega, P. G. ;
Mairani, A. ;
Sala, P. R. ;
Smirnov, G. ;
Vlachoudisl, V. .
NUCLEAR DATA SHEETS, 2014, 120 :211-214
[4]   Intranuclear cascade model for a comprehensive description of spallation reaction data [J].
Boudard, A ;
Cugnon, J ;
Leray, S ;
Volant, C .
PHYSICAL REVIEW C, 2002, 66 (04) :28
[5]   New potentialities of the Liege intranuclear cascade model for reactions induced by nucleons and light charged particles [J].
Boudard, A. ;
Cugnon, J. ;
David, J. -C. ;
Leray, S. ;
Mancusi, D. .
PHYSICAL REVIEW C, 2013, 87 (01)
[6]  
Brun R., 1987, CERN-DD-EE-84-1
[7]   Evaluation of neutron cross sections of hydrogen from 20 MeV to 1 GeV [J].
Chiba, S ;
Morioka, S ;
Fukahori, T .
JOURNAL OF NUCLEAR SCIENCE AND TECHNOLOGY, 1996, 33 (08) :654-662
[8]  
Coupland Daniel David Schechtman, 2013, Doctoral Dissertation
[9]  
Dickens J.K., 1988, SCINFUL: A Monte Carlo Based Computer Program to Determine a Scintillator Full Energy Response to Neutron Detection for En Between 0.1 and 80 MeV: Program Development and Comparisons of Program Predictions with Experimental Data
[10]   GAMMA-CALIBRATION OF NE-213 SCINTILLATION-COUNTERS [J].
DIETZE, G ;
KLEIN, H .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH, 1982, 193 (03) :549-556