Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay

Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is all...
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Gespeichert in:

Autor*in:	Buchanan, C. D. Lande, K.

Format:	E-Artikel

Erschienen:	1968

Umfang:	Online-Ressource 4

Reproduktion:	APS Digital Backfile Archive 1893-2003
Übergeordnetes Werk:	Enthalten in: Physical review letters - College Park, Md. : APS, 1958, 21(1968), 3, Seite 169-172
Übergeordnetes Werk:	volume:21 ; year:1968 ; number:3 ; pages:169-172 ; extent:4

Links:	Link aufrufen

Katalog-ID:	NLEJ251216543

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520			\|a Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made.
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allfields	(DE-627)NLEJ251216543 (DE-601)aps:8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd DE-627 ger DE-627 rakwb Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay 1968 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made. APS Digital Backfile Archive 1893-2003 Buchanan, C. D. oth Lande, K. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 21(1968), 3, Seite 169-172 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:21 year:1968 number:3 pages:169-172 extent:4 https://www.tib.eu/de/suchen/id/aps%3A8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 21 1968 3 169-172 4
spelling	(DE-627)NLEJ251216543 (DE-601)aps:8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd DE-627 ger DE-627 rakwb Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay 1968 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made. APS Digital Backfile Archive 1893-2003 Buchanan, C. D. oth Lande, K. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 21(1968), 3, Seite 169-172 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:21 year:1968 number:3 pages:169-172 extent:4 https://www.tib.eu/de/suchen/id/aps%3A8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 21 1968 3 169-172 4
allfields_unstemmed	(DE-627)NLEJ251216543 (DE-601)aps:8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd DE-627 ger DE-627 rakwb Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay 1968 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made. APS Digital Backfile Archive 1893-2003 Buchanan, C. D. oth Lande, K. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 21(1968), 3, Seite 169-172 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:21 year:1968 number:3 pages:169-172 extent:4 https://www.tib.eu/de/suchen/id/aps%3A8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 21 1968 3 169-172 4
allfieldsGer	(DE-627)NLEJ251216543 (DE-601)aps:8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd DE-627 ger DE-627 rakwb Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay 1968 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made. APS Digital Backfile Archive 1893-2003 Buchanan, C. D. oth Lande, K. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 21(1968), 3, Seite 169-172 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:21 year:1968 number:3 pages:169-172 extent:4 https://www.tib.eu/de/suchen/id/aps%3A8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 21 1968 3 169-172 4
allfieldsSound	(DE-627)NLEJ251216543 (DE-601)aps:8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd DE-627 ger DE-627 rakwb Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay 1968 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made. APS Digital Backfile Archive 1893-2003 Buchanan, C. D. oth Lande, K. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 21(1968), 3, Seite 169-172 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:21 year:1968 number:3 pages:169-172 extent:4 https://www.tib.eu/de/suchen/id/aps%3A8e09cfa16e18be5e01c2a3b90f5d7c2256bfa5bd Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 21 1968 3 169-172 4
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title	Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay
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title_sort	effects of δs=-δq on cp-nonconservation phenomenology in k0 decay
title_auth	Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay
abstract	Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made.
abstractGer	Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made.
abstract_unstemmed	Incorporating the present experimental value of the ΔS=-ΔQ amplitude into the K0 CP-nonconservation phenomenology, we find that solution II (η00 and η+- in opposite quadrants) is as viable as solution I η00 and η+- in the same quadrant), though both have poor fits. Thus, if a ΔS=-ΔQ amplitude is allowed, a clear choice between these two solutions cannot yet be made.
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title_short	Effects of ΔS=-ΔQ on CP-Nonconservation Phenomenology in K0 Decay
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