The general neutron induced reaction cross sections with the projectile neutron energy are being studied. As a result of this, the compound nucleus is formed through de-excitation of the selected nuclei by emitted particles γ and 2n with the reaction cross section at intermediate energy. The production of residual nuclide by neutron induced reaction on the selected nuclei has been investigated by using computer code projection angular-momentum coupled evaporation Monte Carlo code (PACE4). Dependence of Reaction Cross Section for Projectile Neutron with Different K Values on Target 55Mn in the Energy Range (0.5 - 3.42) Mev and Dependence of Reaction Cross Section for Projectile Neutron with Different K Values on 55Mn Target in the Energy Range (11.5 - 38.5) Mev. Then, the theoretical estimated value compared with the Experimental value the data which obtained from International Atomic and Energy Agency, Exchange format. Results show us the reaction cross section vs energy of projectile neutron with target nucleus Manganese and the emitted particles were γ and 2n respectively with new residual nuclei, i.e. 56Mn and 54Mn, in addition to this the best fit K values are 10 and 8 for each channels respectively. Finally the level density parameter is the dominant parameter that can influence the reaction cross section from the outcome of this software by varying with free constant parameter (K). i.e., 8, 10 and 12.
Published in | Radiation Science and Technology (Volume 7, Issue 1) |
DOI | 10.11648/j.rst.20210701.11 |
Page(s) | 1-6 |
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Manganese, Level Density Parameter, Free Constant Parameter, Reaction Cross-section
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APA Style
Asmamaw Tsega Alemu, Yenesew Asradew. (2021). The Study of Neutron Induced Reaction on Manganese Reaction Cross-Section at Intermediate Energy. Radiation Science and Technology, 7(1), 1-6. https://doi.org/10.11648/j.rst.20210701.11
ACS Style
Asmamaw Tsega Alemu; Yenesew Asradew. The Study of Neutron Induced Reaction on Manganese Reaction Cross-Section at Intermediate Energy. Radiat. Sci. Technol. 2021, 7(1), 1-6. doi: 10.11648/j.rst.20210701.11
AMA Style
Asmamaw Tsega Alemu, Yenesew Asradew. The Study of Neutron Induced Reaction on Manganese Reaction Cross-Section at Intermediate Energy. Radiat Sci Technol. 2021;7(1):1-6. doi: 10.11648/j.rst.20210701.11
@article{10.11648/j.rst.20210701.11, author = {Asmamaw Tsega Alemu and Yenesew Asradew}, title = {The Study of Neutron Induced Reaction on Manganese Reaction Cross-Section at Intermediate Energy}, journal = {Radiation Science and Technology}, volume = {7}, number = {1}, pages = {1-6}, doi = {10.11648/j.rst.20210701.11}, url = {https://doi.org/10.11648/j.rst.20210701.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.rst.20210701.11}, abstract = {The general neutron induced reaction cross sections with the projectile neutron energy are being studied. As a result of this, the compound nucleus is formed through de-excitation of the selected nuclei by emitted particles γ and 2n with the reaction cross section at intermediate energy. The production of residual nuclide by neutron induced reaction on the selected nuclei has been investigated by using computer code projection angular-momentum coupled evaporation Monte Carlo code (PACE4). Dependence of Reaction Cross Section for Projectile Neutron with Different K Values on Target 55Mn in the Energy Range (0.5 - 3.42) Mev and Dependence of Reaction Cross Section for Projectile Neutron with Different K Values on 55Mn Target in the Energy Range (11.5 - 38.5) Mev. Then, the theoretical estimated value compared with the Experimental value the data which obtained from International Atomic and Energy Agency, Exchange format. Results show us the reaction cross section vs energy of projectile neutron with target nucleus Manganese and the emitted particles were γ and 2n respectively with new residual nuclei, i.e. 56Mn and 54Mn, in addition to this the best fit K values are 10 and 8 for each channels respectively. Finally the level density parameter is the dominant parameter that can influence the reaction cross section from the outcome of this software by varying with free constant parameter (K). i.e., 8, 10 and 12.}, year = {2021} }
TY - JOUR T1 - The Study of Neutron Induced Reaction on Manganese Reaction Cross-Section at Intermediate Energy AU - Asmamaw Tsega Alemu AU - Yenesew Asradew Y1 - 2021/01/12 PY - 2021 N1 - https://doi.org/10.11648/j.rst.20210701.11 DO - 10.11648/j.rst.20210701.11 T2 - Radiation Science and Technology JF - Radiation Science and Technology JO - Radiation Science and Technology SP - 1 EP - 6 PB - Science Publishing Group SN - 2575-5943 UR - https://doi.org/10.11648/j.rst.20210701.11 AB - The general neutron induced reaction cross sections with the projectile neutron energy are being studied. As a result of this, the compound nucleus is formed through de-excitation of the selected nuclei by emitted particles γ and 2n with the reaction cross section at intermediate energy. The production of residual nuclide by neutron induced reaction on the selected nuclei has been investigated by using computer code projection angular-momentum coupled evaporation Monte Carlo code (PACE4). Dependence of Reaction Cross Section for Projectile Neutron with Different K Values on Target 55Mn in the Energy Range (0.5 - 3.42) Mev and Dependence of Reaction Cross Section for Projectile Neutron with Different K Values on 55Mn Target in the Energy Range (11.5 - 38.5) Mev. Then, the theoretical estimated value compared with the Experimental value the data which obtained from International Atomic and Energy Agency, Exchange format. Results show us the reaction cross section vs energy of projectile neutron with target nucleus Manganese and the emitted particles were γ and 2n respectively with new residual nuclei, i.e. 56Mn and 54Mn, in addition to this the best fit K values are 10 and 8 for each channels respectively. Finally the level density parameter is the dominant parameter that can influence the reaction cross section from the outcome of this software by varying with free constant parameter (K). i.e., 8, 10 and 12. VL - 7 IS - 1 ER -