Design of a compact, permanent magnet electron cyclotron resonance ion source for proton and H{sub 2}{sup +} beam production
A 2.45 GHz microwave ion source was developed at China Institute of Atomic Energy (CIAE) for proton beam production of over 60 mA [B.-Q. Cui, Y.-W. Bao, L.-Q. Li, W.-S. Jiang, and R.-W. Wang, Proceedings of the High Current Electron Cyclotron Resonance (ECR) Ion Source for Proton Accelerator, APAC-2...
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creator | Jia Xianlu Zhang Tianjue Wang Chuan Zheng Xia Yin Zhiguo Zhong Junqing Wu Longcheng Qin Jiuchang Luo Shan |
description | A 2.45 GHz microwave ion source was developed at China Institute of Atomic Energy (CIAE) for proton beam production of over 60 mA [B.-Q. Cui, Y.-W. Bao, L.-Q. Li, W.-S. Jiang, and R.-W. Wang, Proceedings of the High Current Electron Cyclotron Resonance (ECR) Ion Source for Proton Accelerator, APAC-2001, 2001 (unpublished)]. For various proton beam applications, another 2.45 GHz microwave ion source with a compact structure is designed and will be built at CIAE as well for high current proton beam production. It is also considered to be used for the test of H{sub 2}{sup +} beam, which could be injected into the central region model cyclotron at CIAE, and accelerated to 5 MeV before extraction by stripping. The required ECR magnetic field is supplied by all the permanent magnets rather than electrical solenoids and six poles. The magnetic field distribution provided by this permanent magnets configuration is a large and uniformly volume of ECR zone, with central magnetic field of a magnitude of {approx}875 Gs[T. Taylor and J. S. C. Wills, Nucl. Instrum. Methods Phys. Res. A 309, 37 (1991)]. The field adjustment at the extraction end can be implemented by moving the position of the magnet blocks. The results of plasma, coupling with 2.45 GHz microwave in the ECR zone inside the ion source are simulated by particle-in-cell code to optimize the density by adjusting the magnetic field distribution. The design configuration of the ion source will be summarized in the paper. |
doi_str_mv | 10.1063/1.3267838 |
format | Article |
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Cui, Y.-W. Bao, L.-Q. Li, W.-S. Jiang, and R.-W. Wang, Proceedings of the High Current Electron Cyclotron Resonance (ECR) Ion Source for Proton Accelerator, APAC-2001, 2001 (unpublished)]. For various proton beam applications, another 2.45 GHz microwave ion source with a compact structure is designed and will be built at CIAE as well for high current proton beam production. It is also considered to be used for the test of H{sub 2}{sup +} beam, which could be injected into the central region model cyclotron at CIAE, and accelerated to 5 MeV before extraction by stripping. The required ECR magnetic field is supplied by all the permanent magnets rather than electrical solenoids and six poles. The magnetic field distribution provided by this permanent magnets configuration is a large and uniformly volume of ECR zone, with central magnetic field of a magnitude of {approx}875 Gs[T. Taylor and J. S. C. Wills, Nucl. Instrum. Methods Phys. Res. A 309, 37 (1991)]. The field adjustment at the extraction end can be implemented by moving the position of the magnet blocks. The results of plasma, coupling with 2.45 GHz microwave in the ECR zone inside the ion source are simulated by particle-in-cell code to optimize the density by adjusting the magnetic field distribution. The design configuration of the ion source will be summarized in the paper.</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/1.3267838</identifier><language>eng</language><publisher>United States</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; BEAM PRODUCTION ; CIAE ; CYCLOTRONS ; DESIGN ; ECR ION SOURCES ; ELECTRON CYCLOTRON-RESONANCE ; GHZ RANGE ; HYDROGEN IONS 2 PLUS ; MAGNETIC FIELDS ; MEV RANGE ; MICROWAVE RADIATION ; PARTICLE ACCELERATORS ; PERMANENT MAGNETS ; PLASMA ; PROTON BEAMS ; SOLENOIDS ; STRIPPING</subject><ispartof>Review of scientific instruments, 2010-02, Vol.81 (2)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22053672$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Jia Xianlu</creatorcontrib><creatorcontrib>Zhang Tianjue</creatorcontrib><creatorcontrib>Wang Chuan</creatorcontrib><creatorcontrib>Zheng Xia</creatorcontrib><creatorcontrib>Yin Zhiguo</creatorcontrib><creatorcontrib>Zhong Junqing</creatorcontrib><creatorcontrib>Wu Longcheng</creatorcontrib><creatorcontrib>Qin Jiuchang</creatorcontrib><creatorcontrib>Luo Shan</creatorcontrib><title>Design of a compact, permanent magnet electron cyclotron resonance ion source for proton and H{sub 2}{sup +} beam production</title><title>Review of scientific instruments</title><description>A 2.45 GHz microwave ion source was developed at China Institute of Atomic Energy (CIAE) for proton beam production of over 60 mA [B.-Q. Cui, Y.-W. Bao, L.-Q. Li, W.-S. Jiang, and R.-W. Wang, Proceedings of the High Current Electron Cyclotron Resonance (ECR) Ion Source for Proton Accelerator, APAC-2001, 2001 (unpublished)]. For various proton beam applications, another 2.45 GHz microwave ion source with a compact structure is designed and will be built at CIAE as well for high current proton beam production. It is also considered to be used for the test of H{sub 2}{sup +} beam, which could be injected into the central region model cyclotron at CIAE, and accelerated to 5 MeV before extraction by stripping. The required ECR magnetic field is supplied by all the permanent magnets rather than electrical solenoids and six poles. The magnetic field distribution provided by this permanent magnets configuration is a large and uniformly volume of ECR zone, with central magnetic field of a magnitude of {approx}875 Gs[T. Taylor and J. S. C. Wills, Nucl. Instrum. Methods Phys. Res. A 309, 37 (1991)]. The field adjustment at the extraction end can be implemented by moving the position of the magnet blocks. The results of plasma, coupling with 2.45 GHz microwave in the ECR zone inside the ion source are simulated by particle-in-cell code to optimize the density by adjusting the magnetic field distribution. The design configuration of the ion source will be summarized in the paper.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>BEAM PRODUCTION</subject><subject>CIAE</subject><subject>CYCLOTRONS</subject><subject>DESIGN</subject><subject>ECR ION SOURCES</subject><subject>ELECTRON CYCLOTRON-RESONANCE</subject><subject>GHZ RANGE</subject><subject>HYDROGEN IONS 2 PLUS</subject><subject>MAGNETIC FIELDS</subject><subject>MEV RANGE</subject><subject>MICROWAVE RADIATION</subject><subject>PARTICLE ACCELERATORS</subject><subject>PERMANENT MAGNETS</subject><subject>PLASMA</subject><subject>PROTON BEAMS</subject><subject>SOLENOIDS</subject><subject>STRIPPING</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqNjUlOw0AQRVsIJMyw4AYlsQSHHpK2WTMoB2AfdSrlYGRXWd3tBYLcnQZxgPzN-78GfaVujF4Y7d2DWTjrm9a1J6oyun2sG2_dqaq0dsvaN8v2XF2k9KGLVsZU6vuZUr9nkA4CoIxTwHwPE8UxMHGGMeyZMtBAmKMw4CcO8uciJeHASNCXlGSOxXYSYYqSyyTwDtZfad6CPRRMcHeALYXxd7-bMZevK3XWhSHR9T8v1e3ry9vTupaU-03CPhO-ozCX8o21euV8Y91xVz-kulR7</recordid><startdate>20100215</startdate><enddate>20100215</enddate><creator>Jia Xianlu</creator><creator>Zhang Tianjue</creator><creator>Wang Chuan</creator><creator>Zheng Xia</creator><creator>Yin Zhiguo</creator><creator>Zhong Junqing</creator><creator>Wu Longcheng</creator><creator>Qin Jiuchang</creator><creator>Luo Shan</creator><scope>OTOTI</scope></search><sort><creationdate>20100215</creationdate><title>Design of a compact, permanent magnet electron cyclotron resonance ion source for proton and H{sub 2}{sup +} beam production</title><author>Jia Xianlu ; Zhang Tianjue ; Wang Chuan ; Zheng Xia ; Yin Zhiguo ; Zhong Junqing ; Wu Longcheng ; Qin Jiuchang ; Luo Shan</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-osti_scitechconnect_220536723</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>BEAM PRODUCTION</topic><topic>CIAE</topic><topic>CYCLOTRONS</topic><topic>DESIGN</topic><topic>ECR ION SOURCES</topic><topic>ELECTRON CYCLOTRON-RESONANCE</topic><topic>GHZ RANGE</topic><topic>HYDROGEN IONS 2 PLUS</topic><topic>MAGNETIC FIELDS</topic><topic>MEV RANGE</topic><topic>MICROWAVE RADIATION</topic><topic>PARTICLE ACCELERATORS</topic><topic>PERMANENT MAGNETS</topic><topic>PLASMA</topic><topic>PROTON BEAMS</topic><topic>SOLENOIDS</topic><topic>STRIPPING</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Jia Xianlu</creatorcontrib><creatorcontrib>Zhang Tianjue</creatorcontrib><creatorcontrib>Wang Chuan</creatorcontrib><creatorcontrib>Zheng Xia</creatorcontrib><creatorcontrib>Yin Zhiguo</creatorcontrib><creatorcontrib>Zhong Junqing</creatorcontrib><creatorcontrib>Wu Longcheng</creatorcontrib><creatorcontrib>Qin Jiuchang</creatorcontrib><creatorcontrib>Luo Shan</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Jia Xianlu</au><au>Zhang Tianjue</au><au>Wang Chuan</au><au>Zheng Xia</au><au>Yin Zhiguo</au><au>Zhong Junqing</au><au>Wu Longcheng</au><au>Qin Jiuchang</au><au>Luo Shan</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Design of a compact, permanent magnet electron cyclotron resonance ion source for proton and H{sub 2}{sup +} beam production</atitle><jtitle>Review of scientific instruments</jtitle><date>2010-02-15</date><risdate>2010</risdate><volume>81</volume><issue>2</issue><issn>0034-6748</issn><eissn>1089-7623</eissn><abstract>A 2.45 GHz microwave ion source was developed at China Institute of Atomic Energy (CIAE) for proton beam production of over 60 mA [B.-Q. Cui, Y.-W. Bao, L.-Q. Li, W.-S. Jiang, and R.-W. Wang, Proceedings of the High Current Electron Cyclotron Resonance (ECR) Ion Source for Proton Accelerator, APAC-2001, 2001 (unpublished)]. For various proton beam applications, another 2.45 GHz microwave ion source with a compact structure is designed and will be built at CIAE as well for high current proton beam production. It is also considered to be used for the test of H{sub 2}{sup +} beam, which could be injected into the central region model cyclotron at CIAE, and accelerated to 5 MeV before extraction by stripping. The required ECR magnetic field is supplied by all the permanent magnets rather than electrical solenoids and six poles. The magnetic field distribution provided by this permanent magnets configuration is a large and uniformly volume of ECR zone, with central magnetic field of a magnitude of {approx}875 Gs[T. Taylor and J. S. C. Wills, Nucl. Instrum. Methods Phys. Res. A 309, 37 (1991)]. The field adjustment at the extraction end can be implemented by moving the position of the magnet blocks. The results of plasma, coupling with 2.45 GHz microwave in the ECR zone inside the ion source are simulated by particle-in-cell code to optimize the density by adjusting the magnetic field distribution. The design configuration of the ion source will be summarized in the paper.</abstract><cop>United States</cop><doi>10.1063/1.3267838</doi></addata></record> |
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subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY BEAM PRODUCTION CIAE CYCLOTRONS DESIGN ECR ION SOURCES ELECTRON CYCLOTRON-RESONANCE GHZ RANGE HYDROGEN IONS 2 PLUS MAGNETIC FIELDS MEV RANGE MICROWAVE RADIATION PARTICLE ACCELERATORS PERMANENT MAGNETS PLASMA PROTON BEAMS SOLENOIDS STRIPPING |
title | Design of a compact, permanent magnet electron cyclotron resonance ion source for proton and H{sub 2}{sup +} beam production |
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