{"title":"圆孔铁隔膜磁铁","authors":"Hiroshi Noma, Tetuhiro Shioda, Yasukazu Yoshizawa","doi":"10.1016/0029-554X(81)90769-2","DOIUrl":null,"url":null,"abstract":"<div><p>An iron septum magnet was designed for the charged-particle beam splitting system. Magnetic field measurements of the septum model magnet with a circular hole were performed for several conditions. The hole field is <em>B</em><sub>0</sub> = 60–250 G for a hole radius of 12 mm and the gap field is <em>B</em><sub>g</sub> = 5–6 kG for a gap distance of 8 mm with a septum thickness of 1 mm. The multipole field strength in the circular hole is obtained from the field distribution.</p></div>","PeriodicalId":100971,"journal":{"name":"Nuclear Instruments and Methods","volume":"184 2","pages":"Pages 587-589"},"PeriodicalIF":0.0000,"publicationDate":"1981-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0029-554X(81)90769-2","citationCount":"0","resultStr":"{\"title\":\"Circular hole iron septum magnet\",\"authors\":\"Hiroshi Noma, Tetuhiro Shioda, Yasukazu Yoshizawa\",\"doi\":\"10.1016/0029-554X(81)90769-2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>An iron septum magnet was designed for the charged-particle beam splitting system. Magnetic field measurements of the septum model magnet with a circular hole were performed for several conditions. The hole field is <em>B</em><sub>0</sub> = 60–250 G for a hole radius of 12 mm and the gap field is <em>B</em><sub>g</sub> = 5–6 kG for a gap distance of 8 mm with a septum thickness of 1 mm. The multipole field strength in the circular hole is obtained from the field distribution.</p></div>\",\"PeriodicalId\":100971,\"journal\":{\"name\":\"Nuclear Instruments and Methods\",\"volume\":\"184 2\",\"pages\":\"Pages 587-589\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1981-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0029-554X(81)90769-2\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments and Methods\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0029554X81907692\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments and Methods","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0029554X81907692","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
An iron septum magnet was designed for the charged-particle beam splitting system. Magnetic field measurements of the septum model magnet with a circular hole were performed for several conditions. The hole field is B0 = 60–250 G for a hole radius of 12 mm and the gap field is Bg = 5–6 kG for a gap distance of 8 mm with a septum thickness of 1 mm. The multipole field strength in the circular hole is obtained from the field distribution.