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      KCI등재 SCI SCIE SCOPUS

      Characteristics of Proton Beams and Secondary Neutrons Arising from Two Different Beam Nozzles

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      https://www.riss.kr/link?id=A104097342

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      다국어 초록 (Multilingual Abstract)

      A tandem or a Van de Graaff accelerator with an energy of 3 MeV is typically used for Proton Induced X-ray Emission (PIXE) analysis. In this study, the beam line design used in the PIXE analysis, instead of the typical low-energy accelerator, was used...

      A tandem or a Van de Graaff accelerator with an energy of 3 MeV is typically used for Proton Induced X-ray Emission (PIXE) analysis. In this study, the beam line design used in the PIXE analysis, instead of the typical low-energy accelerator, was used to increase the production of isotopes from a 13-MeV cyclotron. For the PIXE analysis, the proton beam should be focused at the target through a nozzle after degrading the proton beams energy from 13 MeV to 3 MeV by using an energy degrader. Previous studies have been conducted to determine the most appropriate material for and the thickness of the energy degrader. From the energy distribution of the degraded proton beam and the neutron occurrence rate at the degrader, an aluminum nozzle of X thickness was determined to be the most appropriate nozzle construction. Neutrons are created by the collision of 3-MeV protons in the nozzle after passage through the energy degrader. In addition, a proton beam of sufficient intensity is required for a non-destructive PIXE analysis. Therefore, if nozzle design is to be optimized, the number of neutrons that arise from the collision of protons inside the nozzle, as well as the track direction of the generated secondary neutrons, must be considered, with the primary aim of ensuring that a sufficient number of protons pass through the nozzle as a direct beam. A number of laboratories are currently conducting research related to the design of nozzles used in accelerator fields, mostly medical fields. This paper presents a comparative analysis of two typical nozzle shapes in order to minimize the loss of protons and the generation of secondary neutrons. The neutron occurrence rate and the number of protons that pass through the nozzle were analyzed by using a Particle and Heavy Ion Transport code System (PHITS) program in order to identify the nozzle that generated the strongest proton beam.

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      참고문헌 (Reference)

      1 Hasnat Kabir, Kochi University 2007

      2 M. E. Fedi, 189 : 56-, 2002

      3 F. Mathis, 240 : 532-, 2005

      4 G. W. Grime, 181 : 66-, 2001

      5 N. Matsuda, "Particle and Heavy Ion Transport code System (PHITS) version 2.64" RIST 2013

      6 W. Loveland, "Modern Nuclear Chemistry" John Wiley & Sons, Inc 20-, 2006

      7 Sae-Hoon Park, "Characterization of the Beam Profile for the PIXE/PIGE Beam Line at the CRC Proton Cyclotron" 한국물리학회 63 (63): 1291-1295, 2013

      1 Hasnat Kabir, Kochi University 2007

      2 M. E. Fedi, 189 : 56-, 2002

      3 F. Mathis, 240 : 532-, 2005

      4 G. W. Grime, 181 : 66-, 2001

      5 N. Matsuda, "Particle and Heavy Ion Transport code System (PHITS) version 2.64" RIST 2013

      6 W. Loveland, "Modern Nuclear Chemistry" John Wiley & Sons, Inc 20-, 2006

      7 Sae-Hoon Park, "Characterization of the Beam Profile for the PIXE/PIGE Beam Line at the CRC Proton Cyclotron" 한국물리학회 63 (63): 1291-1295, 2013

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      2023 평가예정 해외DB학술지평가 신청대상 (해외등재 학술지 평가)
      2020-01-01 평가 등재학술지 유지 (해외등재 학술지 평가) KCI등재
      2011-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2009-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2007-01-01 평가 SCI 등재 (등재유지) KCI등재
      2005-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2002-07-01 평가 등재학술지 선정 (등재후보2차) KCI등재
      2000-01-01 평가 등재후보학술지 선정 (신규평가) KCI등재후보
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      기준연도 WOS-KCI 통합IF(2년) KCIF(2년) KCIF(3년)
      2016 0.47 0.15 0.31
      KCIF(4년) KCIF(5년) 중심성지수(3년) 즉시성지수
      0.26 0.2 0.26 0.03
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