FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2313441605> ?p ?o ?g. }

• W2313441605 abstract "The principle of using multiple partial helical magnets to preserve the polarization of the proton beam during its acceleration was applied successfully to the alternating gradient synchrotron (AGS) which currently operates with two partial helical magnets. In this paper we further explore this idea by using four partial helical magnets placed symmetrically in the AGS ring. This provides many advantages over the present setup of the AGS, which uses two partial helical magnets. First, the symmetric placement of the four helical magnets and their relatively lower field of operation allows for better control of the AGS optics with reduced values of the beta functions especially near beam injection and allows both the vertical and horizontal tunes to be placed within the ``spin tune gap,'' therefore eliminating the horizontal and vertical intrinsic spin resonances of the AGS during the acceleration cycle. Second, it provides a wider spin tune gap. Third, the vertical spin direction during beam injection and extraction is closer to vertical. Although the spin tune gap, which is created with four partial helices, can also be created with a single or two partial helices, the high field strength of a single helical magnet which is required to generate such a spin tune gap makes the use of the single helical magnet impractical, and that of the two helical magnets rather difficult. In this paper we will provide results on the spin tune and on the optics of the AGS with four partial helical magnets, and compare them with those from the present setup of the AGS that uses two partial helical magnets. Although in this paper we specifically discuss the effect of the four partial helices on the AGS, this method which can eliminate simultaneously the vertical and horizontal intrinsic spin resonances is a general method and can be applied to any medium energy synchrotron which operates in similar energy range like the AGS and provides the required space to accommodate the four helices. In addition, the four partial helix solution is an optimum solution because it eliminates all the spin resonances for any synchrotron which operates in the same energy range as the AGS." @default.
• W2313441605 created "2016-06-24" @default.
• W2313441605 creator A5046752032 @default.
• W2313441605 creator A5049509325 @default.
• W2313441605 creator A5052942559 @default.
• W2313441605 creator A5055669238 @default.
• W2313441605 creator A5067224934 @default.
• W2313441605 creator A5090912488 @default.
• W2313441605 date "2013-04-11" @default.
• W2313441605 modified "2023-09-25" @default.
• W2313441605 title "BNL alternating gradient synchrotron with four helical magnets to minimize the losses of the polarized proton beam" @default.
• W2313441605 cites W1971248784 @default.
• W2313441605 cites W2036188410 @default.
• W2313441605 cites W2071463783 @default.
• W2313441605 doi "https://doi.org/10.1103/physrevstab.16.043501" @default.
• W2313441605 hasPublicationYear "2013" @default.
• W2313441605 type Work @default.
• W2313441605 sameAs 2313441605 @default.
• W2313441605 citedByCount "2" @default.
• W2313441605 countsByYear W23134416052014 @default.
• W2313441605 countsByYear W23134416052016 @default.
• W2313441605 crossrefType "journal-article" @default.
• W2313441605 hasAuthorship W2313441605A5046752032 @default.
• W2313441605 hasAuthorship W2313441605A5049509325 @default.
• W2313441605 hasAuthorship W2313441605A5052942559 @default.
• W2313441605 hasAuthorship W2313441605A5055669238 @default.
• W2313441605 hasAuthorship W2313441605A5067224934 @default.
• W2313441605 hasAuthorship W2313441605A5090912488 @default.
• W2313441605 hasBestOaLocation W23134416051 @default.
• W2313441605 hasConcept C120665830 @default.
• W2313441605 hasConcept C121332964 @default.
• W2313441605 hasConcept C147789679 @default.
• W2313441605 hasConcept C16389437 @default.
• W2313441605 hasConcept C168834538 @default.
• W2313441605 hasConcept C185592680 @default.
• W2313441605 hasConcept C205049153 @default.
• W2313441605 hasConcept C21368211 @default.
• W2313441605 hasConcept C42704618 @default.
• W2313441605 hasConcept C46141821 @default.
• W2313441605 hasConcept C62520636 @default.
• W2313441605 hasConcept C97355855 @default.
• W2313441605 hasConceptScore W2313441605C120665830 @default.
• W2313441605 hasConceptScore W2313441605C121332964 @default.
• W2313441605 hasConceptScore W2313441605C147789679 @default.
• W2313441605 hasConceptScore W2313441605C16389437 @default.
• W2313441605 hasConceptScore W2313441605C168834538 @default.
• W2313441605 hasConceptScore W2313441605C185592680 @default.
• W2313441605 hasConceptScore W2313441605C205049153 @default.
• W2313441605 hasConceptScore W2313441605C21368211 @default.
• W2313441605 hasConceptScore W2313441605C42704618 @default.
• W2313441605 hasConceptScore W2313441605C46141821 @default.
• W2313441605 hasConceptScore W2313441605C62520636 @default.
• W2313441605 hasConceptScore W2313441605C97355855 @default.
• W2313441605 hasLocation W23134416051 @default.
• W2313441605 hasOpenAccess W2313441605 @default.
• W2313441605 hasPrimaryLocation W23134416051 @default.
• W2313441605 hasRelatedWork W1566960139 @default.
• W2313441605 hasRelatedWork W1967031378 @default.
• W2313441605 hasRelatedWork W1982311884 @default.
• W2313441605 hasRelatedWork W1999118525 @default.
• W2313441605 hasRelatedWork W2003385151 @default.
• W2313441605 hasRelatedWork W207349022 @default.
• W2313441605 hasRelatedWork W2181760712 @default.
• W2313441605 hasRelatedWork W2182438210 @default.
• W2313441605 hasRelatedWork W2187282006 @default.
• W2313441605 hasRelatedWork W2187988734 @default.
• W2313441605 hasRelatedWork W2189488910 @default.
• W2313441605 hasRelatedWork W2554667635 @default.
• W2313441605 hasRelatedWork W2557390921 @default.
• W2313441605 hasRelatedWork W2564598978 @default.
• W2313441605 hasRelatedWork W2949134722 @default.
• W2313441605 hasRelatedWork W3034490210 @default.
• W2313441605 hasRelatedWork W3040669093 @default.
• W2313441605 hasRelatedWork W3131928836 @default.
• W2313441605 hasRelatedWork W3157203680 @default.
• W2313441605 hasRelatedWork W88565107 @default.
• W2313441605 isParatext "false" @default.
• W2313441605 isRetracted "false" @default.
• W2313441605 magId "2313441605" @default.
• W2313441605 workType "article" @default.