Medium-energy nuclear data libraries - A case study, neutron- and proton-induced reactions in Fe-56

Pearlstein, S.

doi:10.1086/168089

Cited by 44 publications

(10 citation statements)

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“…In PHITS2.24, a model proposed by Pearlstein [53,54] and modified by Niita et al [3] was employed for calculating nucleon-nucleus reaction cross sections, while models proposed by Shen et al [55] and Tripathi et al [56,57] were alternatively adopted for nucleus-nucleus reaction cross sections. In addition to these models, the Kurotama model was implemented into PHITS2.52 for calculating both nucleon-nucleus and nucleus-nucleus interaction cross sections.…”

Section: Implementation Of the Kurotama Modelmentioning

confidence: 99%

Particle and Heavy Ion Transport code System, PHITS, version 2.52

Sato

Niita

Matsuda

et al. 2013

Journal of Nuclear Science and Technology

749

332

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An upgraded version of the Particle and Heavy Ion Transport code System, PHITS2.52, was developed and released to the public. The new version has been greatly improved from the previously released version, PHITS2.24, in terms of not only the code itself but also the contents of its package, such as the attached data libraries. In the new version, a higher accuracy of simulation was achieved by implementing several latest nuclear reaction models. The reliability of the simulation was improved by modifying both the algorithms for the electron-, positron-, and photon-transport simulations and the procedure for calculating the statistical uncertainties of the tally results. Estimation of the time evolution of radioactivity became feasible by incorporating the activation calculation program DCHAIN-SP into the new package. The efficiency of the simulation was also improved as a result of the implementation of shared-memory parallelization and the optimization of several time-consuming algorithms. Furthermore, a number of new user-support tools and functions that help users to intuitively and effectively perform PHITS simulations were developed and incorporated. Due to these improvements, PHITS is now a more powerful tool for particle transport simulation applicable to various research and development fields, such as nuclear technology, accelerator design, medical physics, and cosmic-ray research.

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Section: Implementation Of the Kurotama Modelmentioning

confidence: 99%

Particle and Heavy Ion Transport code System, PHITS, version 2.52

Sato

Niita

Matsuda

et al. 2013

Journal of Nuclear Science and Technology

749

332

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“…11.52. For 56 Fe (p, pn) 55 Fe, use cross sections given by Pearlstein (1989). All of these reactions, except for (p, pn) on 56 Fe, also produce positrons, whose production cross sections were considered in detail by , and use those values.…”

Section: Neutron-producing Reactions and Their Threshold Energiesmentioning

confidence: 99%

Solar Neutrons and Related Phenomena

Дорман¹

2010

Astrophysics and Space Science Library

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“…At present, however, the use of this reaction to monitor a proton flux is regarded as incorrect because the (n,α) reaction may also contribute to the yield of 24 Na, thus overestimating the proton flux density Φ. Therefore, the 27 Al(p,x) 22 Na monitor has been preferred recently. The situation can be seen clearly in Fig.…”

Section: Monitor Reactionsmentioning

confidence: 99%

“…Here we used Letaw's formulae described in [22] to obtain the unified cross section to be 1663 mbarn at 130 MeV and 1873 mbarn at 1500 MeV.…”

Section: Measurement Errorsmentioning

confidence: 99%

Experimental and computer simulation study of the radionuclides produced in thin 209Bi targets by 130 MeV and 1.5 GeV proton-induced reactions

Titarenko¹,

Shvedov²,

Igumnov³

et al. 1998

Nuclear Instruments and Methods in Physics Research Section A:

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The results of experimental and computer simulation studies of the yields of residual product nuclei in 209 Bi thin targets irradiated by 130 MeV and 1.5 GeV protons are presented. The yields were measured by direct high-precision γ-spectrometry. The γ-spectrometer resolution was 1.8 keV in the 1332 keV line. The γ-spectra were processed by the ASPRO code. The γ-lines were identified, and the cross sections defined, by the SIGMA code using the GDISP radioactive database. The process was monitored by the 27 Al(p,x) 24 Na reaction. Results are presented for comparisons between the 209 Bi(p,x) reaction yields obtained experimentally and simulated by the HETC, GNASH, LAHET, INUCL, CEM95, CASCADE, and ALICE codes.

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Medium-energy nuclear data libraries - A case study, neutron- and proton-induced reactions in Fe-56

Cited by 44 publications

References 0 publications

Particle and Heavy Ion Transport code System, PHITS, version 2.52

Particle and Heavy Ion Transport code System, PHITS, version 2.52

Solar Neutrons and Related Phenomena

Experimental and computer simulation study of the radionuclides produced in thin 209Bi targets by 130 MeV and 1.5 GeV proton-induced reactions

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