Chromatic Corrections for Large Storage Rings
The use of the achromat concept (1) to facilitate chromatic corrections in large storage rings is illustrated. The example given in this report is a lattice for a 75 GeV/c ring with six interaction regions having a betax = 1.6 m, a betay = 0.lm and a luminosity of 1.4 1032cm-2s-1. The chromatic corr...
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Veröffentlicht in: | IEEE transactions on nuclear science 1979-01, Vol.26 (3), p.3598-3600, Article 3598 |
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description | The use of the achromat concept (1) to facilitate chromatic corrections in large storage rings is illustrated. The example given in this report is a lattice for a 75 GeV/c ring with six interaction regions having a betax = 1.6 m, a betay = 0.lm and a luminosity of 1.4 1032cm-2s-1. The chromatic corrections are done with four families of sextupoles, two for each transverse plane, the strengths of which are determined by the solution of four linear equations in four unknowns. The basic simplicity of the method allows on-line control of the sextupole adjustments. |
doi_str_mv | 10.1109/TNS.1979.4330113 |
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V. ; Browm, K. L.</creator><creatorcontrib>Servranckx, R. V. ; Browm, K. L.</creatorcontrib><description>The use of the achromat concept (1) to facilitate chromatic corrections in large storage rings is illustrated. The example given in this report is a lattice for a 75 GeV/c ring with six interaction regions having a betax = 1.6 m, a betay = 0.lm and a luminosity of 1.4 1032cm-2s-1. The chromatic corrections are done with four families of sextupoles, two for each transverse plane, the strengths of which are determined by the solution of four linear equations in four unknowns. The basic simplicity of the method allows on-line control of the sextupole adjustments.</description><identifier>ISSN: 0018-9499</identifier><identifier>EISSN: 1558-1578</identifier><identifier>DOI: 10.1109/TNS.1979.4330113</identifier><identifier>CODEN: IETNAE</identifier><language>eng</language><publisher>IEEE</publisher><subject>Degradation ; Equations ; Lattices ; Magnets ; Positrons ; Reflection ; Storage rings</subject><ispartof>IEEE transactions on nuclear science, 1979-01, Vol.26 (3), p.3598-3600, Article 3598</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c369t-728926379a7fb9be9c28c4887366734f9afea1bd023d5c99120ece16a439dd973</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/4330113$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,792,27901,27902,54733</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/4330113$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Servranckx, R. V.</creatorcontrib><creatorcontrib>Browm, K. L.</creatorcontrib><title>Chromatic Corrections for Large Storage Rings</title><title>IEEE transactions on nuclear science</title><addtitle>TNS</addtitle><description>The use of the achromat concept (1) to facilitate chromatic corrections in large storage rings is illustrated. The example given in this report is a lattice for a 75 GeV/c ring with six interaction regions having a betax = 1.6 m, a betay = 0.lm and a luminosity of 1.4 1032cm-2s-1. The chromatic corrections are done with four families of sextupoles, two for each transverse plane, the strengths of which are determined by the solution of four linear equations in four unknowns. The basic simplicity of the method allows on-line control of the sextupole adjustments.</description><subject>Degradation</subject><subject>Equations</subject><subject>Lattices</subject><subject>Magnets</subject><subject>Positrons</subject><subject>Reflection</subject><subject>Storage rings</subject><issn>0018-9499</issn><issn>1558-1578</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1979</creationdate><recordtype>article</recordtype><recordid>eNp9j01LxDAURYMoWEf3gpv-gda8pvl4SynqCEXBGdclTZMxMjOVJBv_vS0zunDh6vK4nHc5hFwDLQEo3q6fVyWgxLJmjAKwE5IB56oALtUpySgFVWCNeE4uYvyYzppTnpGieQ_jTidv8mYMwZrkx33M3RjyVoeNzVdpDHrKV7_fxEty5vQ22qtjLsjbw_26WRbty-NTc9cWhglMhawUVoJJ1NL12Fs0lTK1UpIJIVntUDuroR9oxQZuEKGi1lgQumY4DCjZgtDDXxPGGIN13WfwOx2-OqDdrNtNut2s2x11J0T8QYxPerZJQfvtf-DNAfTW2t-dn_Yb_9hhWw</recordid><startdate>19790101</startdate><enddate>19790101</enddate><creator>Servranckx, R. V.</creator><creator>Browm, K. L.</creator><general>IEEE</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19790101</creationdate><title>Chromatic Corrections for Large Storage Rings</title><author>Servranckx, R. V. ; Browm, K. L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c369t-728926379a7fb9be9c28c4887366734f9afea1bd023d5c99120ece16a439dd973</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1979</creationdate><topic>Degradation</topic><topic>Equations</topic><topic>Lattices</topic><topic>Magnets</topic><topic>Positrons</topic><topic>Reflection</topic><topic>Storage rings</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Servranckx, R. V.</creatorcontrib><creatorcontrib>Browm, K. L.</creatorcontrib><collection>CrossRef</collection><jtitle>IEEE transactions on nuclear science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Servranckx, R. V.</au><au>Browm, K. L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Chromatic Corrections for Large Storage Rings</atitle><jtitle>IEEE transactions on nuclear science</jtitle><stitle>TNS</stitle><date>1979-01-01</date><risdate>1979</risdate><volume>26</volume><issue>3</issue><spage>3598</spage><epage>3600</epage><pages>3598-3600</pages><artnum>3598</artnum><issn>0018-9499</issn><eissn>1558-1578</eissn><coden>IETNAE</coden><abstract>The use of the achromat concept (1) to facilitate chromatic corrections in large storage rings is illustrated. The example given in this report is a lattice for a 75 GeV/c ring with six interaction regions having a betax = 1.6 m, a betay = 0.lm and a luminosity of 1.4 1032cm-2s-1. The chromatic corrections are done with four families of sextupoles, two for each transverse plane, the strengths of which are determined by the solution of four linear equations in four unknowns. The basic simplicity of the method allows on-line control of the sextupole adjustments.</abstract><pub>IEEE</pub><doi>10.1109/TNS.1979.4330113</doi><tpages>3</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Degradation Equations Lattices Magnets Positrons Reflection Storage rings |
title | Chromatic Corrections for Large Storage Rings |
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