MCNP 6 Fission Cross Section Calculations at Intermediate and High Energies

MCNP6 has been Validated and Verified (V&V) against intermediateand high-energy fission-cross-section experimental data. A previously unobserved error in the calculation of fission cross sections of Ta and other nearby target nuclei by the CEM03.03 event generator in MCNP6 and a technical “bug” in the calculation of fission cross sections with the GENXS option of MCNP6 while using the LAQGSM03.03 event generator were detected during our current V&V work. After fixing both these problems, we find that MCNP6 using the CEM03.03 and LAQGSM03.03 event generators calculates fission cross sections in a good agreement with available experimental data for reactions induced by nucleons, pions, and photons on both subactinide and actinide nuclei (from Ho to Pu) at incident energies from several tens of MeV to about 1 TeV.

[1]  R. A. Forster,et al.  Initial MCNP6 Release Overview - MCNP6 version 1.0 , 2013 .

[2]  R. A. Forster,et al.  Initial MCNP6 Release Overview - MCNP6 Beta 3 , 2012 .

[3]  E. Casarejos,et al.  Total Fission Cross Sections in Reactions p+181Ta Investigated in Inverse Kinematics at Relativistic Energies , 2011 .

[4]  N. Matsuda,et al.  Verification of high-energy transport codes on the basis of activation data , 2011, 1106.0054.

[5]  K. Nishihara,et al.  Measurement and simulation of the cross sections for nuclide production in natW and 181Ta targets irradiated with 0.04- to 2.6-GeV protons , 2011 .

[6]  Francisco Calviño Tavares,et al.  Neutron-induced fission cross section of natPb and 209 Bi from threshold to 1 GeV : An improved parametrization , 2011 .

[7]  Richard Edward Prael,et al.  Tally edits for the MCNP6 GENXS option , 2011 .

[8]  A. I. Shchetkovskii,et al.  New approximations to the energy dependences of the total cross sections for the proton-induced fission of 197Au, 203Tl, natPb, and 209Bi nuclei , 2011 .

[9]  Stepan G. Mashnik,et al.  Validation and verification of MCNP6 against intermediate and high-energy experimental data and results by other codes , 2010, 1011.4978.

[10]  M. A. Rana,et al.  Negative Pion Induced Fission with Heavy Target Nuclei , 2011 .

[11]  R. Peterson Nuclear Fission Induced by Pi Mesons , 2010 .

[12]  N. V. Mokhov,et al.  CEM03.03 and LAQGSM03.03 Event Generators for the MCNP6, MCNPX, and MARS15 Transport Codes , 2008, 0805.0751.

[13]  A. N. Smirnov,et al.  Nucleon-induced fission cross sections of tantalum and separated tungsten isotopes and "compound nucleus" effect in intermediate energy region , 2007, 0705.2387.

[14]  S. Mashnik,et al.  Proton-Induced Fission Cross Section Calculation with the LANL Codes CEM2K+GEM2 and LAQGSM+GEM2 , 2003, nucl-th/0307014.

[15]  S. Mashnik,et al.  Merging the CEM2K and LAQGSM Codes with GEM2 to Describe Fission and Light-fragment Production , 2003, nucl-th/0304012.

[16]  W. B. Wilson,et al.  Systematics of Proton-Induced Fission Cross Sections for Intermediate Energy Applications , 2002, nucl-th/0210071.

[17]  S. Mashnik,et al.  Complex particle and light fragment emission in the cascade-excitation model of nuclear reactions , 2002, nucl-th/0208048.

[18]  A. Prokofiev Compilation and systematics of proton-induced fission cross-section data , 2001 .

[19]  J. Sanabria,et al.  Photofission of Heavy Nuclei from 0.2 to 3.8 GeV , 2002 .

[20]  S. Mashnik,et al.  CEM2K - RECENT DEVELOPMENTS IN CEM , 2000, nucl-th/0011064.

[21]  J. Sanabria,et al.  Photofission of actinide nuclei in the quasideuteron and lower part of the {delta} energy region , 2000 .

[22]  S. Mashnik,et al.  Modeling fission in the cascade exciton model , 1998, nucl-th/9812070.

[23]  M. Schmitz,et al.  Photofission of235U and238U at intermediate energies: absolute cross sections and fragment mass distributions , 1994 .

[24]  Rossi,et al.  Photofissility of 232Th measured with tagged photons from 250 to 1200 MeV. , 1993, Physical review. C, Nuclear physics.

[25]  D. Ryckbosch,et al.  Absolute photofission cross sections for 232Th and 235,238U measured with monochromatic tagged photons (20 Mev < Eγ < 110 Mev) , 1987 .

[26]  H. A. Khan,et al.  FISSION AND SPALLATION INDUCED BY 7-GEV PROTONS ON U, BI, PB, AU, W, HO, AND AG , 1984 .

[27]  H. Stroeher,et al.  Absolute photofission cross sections for /sup 235,238/U in the energy range 11. 5--30 MeV , 1984 .

[28]  P. Bourgeois,et al.  Absolute photofission cross sections of 235,238U measured with tagged photons between 40 and 105 MeV , 1984 .

[29]  P. Lister,et al.  190 MeV proton-induced symmetric and asymmetric fission , 1983 .

[30]  V. Toneev,et al.  Cascade-exciton model of nuclear reactions , 1983 .

[31]  L. Andronenko,et al.  Fission cross sections of medium-weight and heavy nuclei induced by 1 GeV protons , 1981 .

[32]  Y. Yariv,et al.  Intranuclear cascade calculation of high-energy heavy-ion interactions , 1979 .

[33]  R. Antanasijević,et al.  An analysis of gold fission induced by high-energy protons , 1976 .

[34]  S. Katcoff,et al.  Interaction of 0. 6--300 GeV protons with U, Bi, Au, and Ag; mica track detector study , 1976 .

[35]  J. Piekarz,et al.  The study of nuclear fission induced by high-energy protons , 1972 .

[36]  S. Katcoff,et al.  HIGH-ENERGY-PROTON FISSION CROSS SECTIONS OF U, Bi, Au, AND Ag MEASURED WITH MICA TRACK DETECTORS. , 1969 .

[37]  M. Perlman,et al.  FISSION OF URANIUM AND TANTALUM INDUCED BY 156-MeV PROTONS. , 1967 .

[38]  Z. Fraenkel,et al.  Monte Carlo Calculations of Nuclear Evaporation Processes. III. Applications to Low-Energy Reactions , 1959 .

[39]  P. Kruger,et al.  HIGH-ENERGY FISSION OF HEAVY ELEMENTS. NUCLEAR CHARGE DEPENDENCE , 1955 .

[40]  H. Steiner,et al.  PROTON-INDUCED FISSION CROSS SECTIONS FOR U238, U235, Th232, Bi209, AND Au197 AT 100 TO 340 MEV , 1955 .

[41]  Nervik TANTALUM SPALLATION AND FISSION INDUCED BY 340 MEV PROTONS (thesis) , 1955 .

[42]  Victor F. Weisskopf,et al.  On the Yield of Nuclear Reactions with Heavy Elements , 1940 .