001035057 001__ 1035057
001035057 005__ 20250724210252.0
001035057 0247_ $$2doi$$a10.1016/j.physo.2024.100248
001035057 0247_ $$2datacite_doi$$a10.34734/FZJ-2025-00153
001035057 0247_ $$2WOS$$aWOS:001394447600001
001035057 037__ $$aFZJ-2025-00153
001035057 041__ $$aEnglish
001035057 1001_ $$0P:(DE-Juel1)192187$$aFaatz, Nicolas$$b0$$eCorresponding author$$ufzj
001035057 245__ $$aDevelopment of a complete spin filter for metastable hydrogen atoms and its isotopes
001035057 260__ $$aAmsterdam$$bElsevier$$c2025
001035057 3367_ $$2DRIVER$$aarticle
001035057 3367_ $$2DataCite$$aOutput Types/Journal article
001035057 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1736840169_28647
001035057 3367_ $$2BibTeX$$aARTICLE
001035057 3367_ $$2ORCID$$aJOURNAL_ARTICLE
001035057 3367_ $$00$$2EndNote$$aJournal Article
001035057 520__ $$aSince the early days of quantum mechanics, hydrogen, as the simplest of all atoms, has been studied or used to investigate new physics. In the past this knowledge has been applied to develop a polarimeter where the initial nuclear polarization of a proton beam could be determined. The key component of this Lamb-shift polarimeter is the so called spin filter, which is able to separate one of four metastable hydrogen hyperfine states by quenching the remaining three hyperfine states to the ground state. Unfortunately, the conventional spin filter is only able to filter two out of the four hyperfine states individually. Therefore, this work provides the necessary theory as well as experimental conditions to build a new generation of spin filter which permits the separation and transmission of any metastable hydrogen hyperfine state as well as for its isotopes in a corresponding beam. This knowledge is applicable for other experiments in different fields of research, e.g. the bound beta decay, axion research or parity violation experiments.
001035057 536__ $$0G:(DE-HGF)POF4-612$$a612 - Cosmic Matter in the Laboratory (POF4-612)$$cPOF4-612$$fPOF IV$$x0
001035057 536__ $$0G:(GEPRIS)533904660$$aDFG project G:(GEPRIS)533904660 - Eine vielseitige Polarisationsmethode für Teilchen mit einfachen Hyperfeinstrukturen (533904660)$$c533904660$$x1
001035057 588__ $$aDataset connected to CrossRef, Journals: juser.fz-juelich.de
001035057 65027 $$0V:(DE-MLZ)SciArea-200$$2V:(DE-HGF)$$aNuclear Physics$$x0
001035057 65017 $$0V:(DE-MLZ)GC-2001-2016$$2V:(DE-HGF)$$aNuclei and Particles$$x0
001035057 7001_ $$0P:(DE-Juel1)131141$$aEngels, Ralf W.$$b1$$ufzj
001035057 7001_ $$0P:(DE-Juel1)133754$$aSoltner, Helmut$$b2$$ufzj
001035057 7001_ $$0P:(DE-Juel1)178627$$aKannis, Chrysovalantis$$b3$$ufzj
001035057 7001_ $$0P:(DE-Juel1)166211$$aBreitkreutz, Bernd$$b4$$ufzj
001035057 773__ $$0PERI:(DE-600)3008350-3$$a10.1016/j.physo.2024.100248$$gVol. 22, p. 100248 -$$p100248$$tPhysics open$$v22$$x2666-0326$$y2025
001035057 8564_ $$uhttps://juser.fz-juelich.de/record/1035057/files/PhysicsOpen22-100248.pdf$$yOpenAccess
001035057 8767_ $$8E-2025-00432-b$$92025-05-28$$a1200214540$$d2025-07-24$$eAPC$$jZahlung erfolgt
001035057 909CO $$ooai:juser.fz-juelich.de:1035057$$pVDB$$pdriver$$pOpenAPC$$popen_access$$popenaire$$popenCost$$pdnbdelivery
001035057 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)192187$$aForschungszentrum Jülich$$b0$$kFZJ
001035057 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131141$$aForschungszentrum Jülich$$b1$$kFZJ
001035057 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)133754$$aForschungszentrum Jülich$$b2$$kFZJ
001035057 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)178627$$aForschungszentrum Jülich$$b3$$kFZJ
001035057 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)166211$$aForschungszentrum Jülich$$b4$$kFZJ
001035057 9131_ $$0G:(DE-HGF)POF4-612$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vCosmic Matter in the Laboratory$$x0
001035057 9141_ $$y2025
001035057 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
001035057 915__ $$0StatID:(DE-HGF)0501$$2StatID$$aDBCoverage$$bDOAJ Seal$$d2023-05-02T08:54:37Z
001035057 915__ $$0StatID:(DE-HGF)0500$$2StatID$$aDBCoverage$$bDOAJ$$d2023-05-02T08:54:37Z
001035057 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
001035057 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bDOAJ : Anonymous peer review$$d2023-05-02T08:54:37Z
001035057 915__ $$0StatID:(DE-HGF)0561$$2StatID$$aArticle Processing Charges$$d2023-09-05
001035057 915__ $$0StatID:(DE-HGF)0700$$2StatID$$aFees$$d2023-09-05
001035057 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2024-12-05
001035057 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2024-12-05
001035057 915__ $$0StatID:(DE-HGF)0112$$2StatID$$aWoS$$bEmerging Sources Citation Index$$d2024-12-05
001035057 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2024-12-05
001035057 915pc $$0PC:(DE-HGF)0000$$2APC$$aAPC keys set
001035057 915pc $$0PC:(DE-HGF)0001$$2APC$$aLocal Funding
001035057 915pc $$0PC:(DE-HGF)0002$$2APC$$aDFG OA Publikationskosten
001035057 915pc $$0PC:(DE-HGF)0125$$2APC$$aDEAL: Elsevier 09/01/2023
001035057 915pc $$0PC:(DE-HGF)0003$$2APC$$aDOAJ Journal
001035057 920__ $$lyes
001035057 9201_ $$0I:(DE-Juel1)IKP-2-20111104$$kIKP-2$$lExperimentelle Hadrondynamik$$x0
001035057 9201_ $$0I:(DE-Juel1)ZEA-1-20090406$$kZEA-1$$lZentralinstitut für Technologie$$x1
001035057 9801_ $$aFullTexts
001035057 980__ $$ajournal
001035057 980__ $$aVDB
001035057 980__ $$aUNRESTRICTED
001035057 980__ $$aI:(DE-Juel1)IKP-2-20111104
001035057 980__ $$aI:(DE-Juel1)ZEA-1-20090406
001035057 980__ $$aAPC
001035057 981__ $$aI:(DE-Juel1)ITE-20250108