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A 30 MeV-cyclotron-based quasi-monoenergetic neutron source

  • Kuo-Yuan Chu (Isotope Application Division, Institute of Nuclear Energy Research) ;
  • Weng-Sheng Kuo (Nuclear Engineering Division, Institute of Nuclear Energy Research) ;
  • How-Ming Lee (Physics Division, Institute of Nuclear Energy Research) ;
  • Yiin-Kuen Fuh (Department of Mechanical Engineering, National Central University)
  • Received : 2022.10.20
  • Accepted : 2023.01.20
  • Published : 2023.05.25

Abstract

This study developed a quasi-monoenergetic neutron source (QMN) for the semiconductor device's soft error rate test (SER). Quasi-monoenergetic neutrons are generated by 9Be(p, n)9B nuclear reaction with a 1 mm beryllium target and 30 MeV protons from a cyclotron. An 8 mm water in the back of the beryllium target is used for avoiding proton penetration. The neutron spectra simulated by MCNP showed that the peak energy was around 26.5 MeV. The heat flow and mechanical properties are numerically analyzed, and the safe operating conditions are therefore determined.

Keywords

References

  1. T.J. O'Gorman, et al., Field testing for cosmic ray soft errors in semiconductor memories, in: IBM Journal of Research and Development, vol. 40, 1996, pp. 41-50.  https://doi.org/10.1147/rd.401.0041
  2. A. Lesea, et al., The rosetta experiment: atmospheric soft error rate testing in differing technology FPGAs, in: IEEE Transactions on Device and Materials Reliability, vol. 5, 2005, pp. 317-328.  https://doi.org/10.1109/TDMR.2005.854207
  3. JEDEC® Standard JESD89, Measurement and Reporting of Alpha Particles and Terrestrial Cosmic Ray-Induced Soft Errors in Semiconductor Devices, JEDEC® Solid State Technology Association, 2001. 
  4. JEDEC® Standard JESD89A, Measurement and Reporting of Alpha Particle and Terrestrial Cosmic Ray Induced Soft Errors in Semiconductor Devices, JEDEC® Solid State Technology Association, 2006. 
  5. JEDEC® Standard JESD89B, Measurement and Reporting of Alpha Particle and Terrestrial Cosmic Ray Induced Soft Errors in Semiconductor Devices, JEDEC® Solid State Technology Association, 2021. 
  6. D.T.L. Jones, Monoenergetic neutron sources below 100 MeV, Radiat. Phys. Chem. 61 (2001) 469-472.  https://doi.org/10.1016/S0969-806X(01)00303-6
  7. Zdenek Mat ej, et al., The methodology for validation of cross sections in quasi monoenergetic neutron field, Nucl. Instrum. Methods Phys. Res. A 1040 (2022), 167075. 
  8. Vivek Chavan, et al., Monoenergetic neutrons from the 9Be(p,n)9B reaction induced by 35, 40 and 45-MeV protons, Nucl. Phys. 1018 (2022), 122374. 
  9. James F. Ziegler, et al., Srim - the stopping and range of ions in matter, Nucl. Instrum. Methods Phys. Res. B 268 (2010) 1818-1823, 2010.  https://doi.org/10.1016/j.nimb.2010.02.091
  10. J.H. Kim, et al., A measurement of monoenergetic neutrons from 9Be(p,n)9B, J. Kor. Phys. Soc. 32 (1998) 462-467. 
  11. S. Kamata, et al., Tail correction in quasi-monoenergetic neutron source, CYRIC Annual Report 2005 (2005) 31-33. 
  12. J. Novak, et al., The p + 9Be (thin target) reaction as a source of quasimonoenergetic neutrons, EPJ Web Conf. 146 (2017), 03013, https://doi.org/10.1051/epjconf/201714603013. ND2016. 
  13. H. Iwashita, et al., Energy-resolved soft-error rate measurements for 1-800 MeV neutrons by the time-of-flight technique at LANSCE, IEEE Trans. Nucl. Sci. 67 (2020). 
  14. COMSOL® Multiphysics v.5.5. https://www.comsol.com/. (Accessed 26 August 2022).