CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton

Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged l...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Barshay, Saul [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	1997

Schlagwörter:	Decay Width Charged Lepton Planck Scale Baryon Asymmetry Lepton Asymmetry

Anmerkung:	© Springer-Verlag 1997

Übergeordnetes Werk:	Enthalten in: Zeitschrift für Physik - Berlin : Springer, 1979, 74(1997), 4 vom: Dez., Seite 709-713
Übergeordnetes Werk:	volume:74 ; year:1997 ; number:4 ; month:12 ; pages:709-713

Links:	Volltext

DOI / URN:	10.1007/s002880050435

Katalog-ID:	SPR003727890

Internformat


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520			\|a Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV.
650		4	\|a Decay Width \|7 (dpeaa)DE-He213
650		4	\|a Charged Lepton \|7 (dpeaa)DE-He213
650		4	\|a Planck Scale \|7 (dpeaa)DE-He213
650		4	\|a Baryon Asymmetry \|7 (dpeaa)DE-He213
650		4	\|a Lepton Asymmetry \|7 (dpeaa)DE-He213
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912			\|a GBV_USEFLAG_A
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912			\|a GBV_ILN_24
912			\|a GBV_ILN_31
912			\|a GBV_ILN_32
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_65
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_121
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_267
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_374
912			\|a GBV_ILN_602
912			\|a GBV_ILN_647
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2018
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2043
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2116
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2119
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2144
912			\|a GBV_ILN_2147
912			\|a GBV_ILN_2148
912			\|a GBV_ILN_2152
912			\|a GBV_ILN_2153
912			\|a GBV_ILN_2158
912			\|a GBV_ILN_2188
912			\|a GBV_ILN_2190
912			\|a GBV_ILN_2193
912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
912			\|a GBV_ILN_2470
912			\|a GBV_ILN_2472
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_2548
912			\|a GBV_ILN_2808
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4246
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4251
912			\|a GBV_ILN_4277
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4320
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4328
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4346
912			\|a GBV_ILN_4367
912			\|a GBV_ILN_4393
912			\|a GBV_ILN_4700
912			\|a GBV_ILN_4753
951			\|a AR
952			\|d 74 \|j 1997 \|e 4 \|c 12 \|h 709-713

Indexfelder

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matchkey_str	article:14315858:1997----::pnnnainemdloaiiiletnsmerdeonqamse
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publishDate	1997
allfields	10.1007/s002880050435 doi (DE-627)SPR003727890 (SPR)s002880050435-e DE-627 ger DE-627 rakwb eng Barshay, Saul verfasserin aut CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. Decay Width (dpeaa)DE-He213 Charged Lepton (dpeaa)DE-He213 Planck Scale (dpeaa)DE-He213 Baryon Asymmetry (dpeaa)DE-He213 Lepton Asymmetry (dpeaa)DE-He213 Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 74(1997), 4 vom: Dez., Seite 709-713 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:74 year:1997 number:4 month:12 pages:709-713 https://dx.doi.org/10.1007/s002880050435 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 74 1997 4 12 709-713
spelling	10.1007/s002880050435 doi (DE-627)SPR003727890 (SPR)s002880050435-e DE-627 ger DE-627 rakwb eng Barshay, Saul verfasserin aut CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. Decay Width (dpeaa)DE-He213 Charged Lepton (dpeaa)DE-He213 Planck Scale (dpeaa)DE-He213 Baryon Asymmetry (dpeaa)DE-He213 Lepton Asymmetry (dpeaa)DE-He213 Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 74(1997), 4 vom: Dez., Seite 709-713 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:74 year:1997 number:4 month:12 pages:709-713 https://dx.doi.org/10.1007/s002880050435 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 74 1997 4 12 709-713
allfields_unstemmed	10.1007/s002880050435 doi (DE-627)SPR003727890 (SPR)s002880050435-e DE-627 ger DE-627 rakwb eng Barshay, Saul verfasserin aut CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. Decay Width (dpeaa)DE-He213 Charged Lepton (dpeaa)DE-He213 Planck Scale (dpeaa)DE-He213 Baryon Asymmetry (dpeaa)DE-He213 Lepton Asymmetry (dpeaa)DE-He213 Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 74(1997), 4 vom: Dez., Seite 709-713 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:74 year:1997 number:4 month:12 pages:709-713 https://dx.doi.org/10.1007/s002880050435 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 74 1997 4 12 709-713
allfieldsGer	10.1007/s002880050435 doi (DE-627)SPR003727890 (SPR)s002880050435-e DE-627 ger DE-627 rakwb eng Barshay, Saul verfasserin aut CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. Decay Width (dpeaa)DE-He213 Charged Lepton (dpeaa)DE-He213 Planck Scale (dpeaa)DE-He213 Baryon Asymmetry (dpeaa)DE-He213 Lepton Asymmetry (dpeaa)DE-He213 Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 74(1997), 4 vom: Dez., Seite 709-713 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:74 year:1997 number:4 month:12 pages:709-713 https://dx.doi.org/10.1007/s002880050435 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 74 1997 4 12 709-713
allfieldsSound	10.1007/s002880050435 doi (DE-627)SPR003727890 (SPR)s002880050435-e DE-627 ger DE-627 rakwb eng Barshay, Saul verfasserin aut CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. Decay Width (dpeaa)DE-He213 Charged Lepton (dpeaa)DE-He213 Planck Scale (dpeaa)DE-He213 Baryon Asymmetry (dpeaa)DE-He213 Lepton Asymmetry (dpeaa)DE-He213 Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 74(1997), 4 vom: Dez., Seite 709-713 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:74 year:1997 number:4 month:12 pages:709-713 https://dx.doi.org/10.1007/s002880050435 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 74 1997 4 12 709-713
language	English
source	Enthalten in Zeitschrift für Physik 74(1997), 4 vom: Dez., Seite 709-713 volume:74 year:1997 number:4 month:12 pages:709-713
sourceStr	Enthalten in Zeitschrift für Physik 74(1997), 4 vom: Dez., Seite 709-713 volume:74 year:1997 number:4 month:12 pages:709-713
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Decay Width Charged Lepton Planck Scale Baryon Asymmetry Lepton Asymmetry
isfreeaccess_bool	false
container_title	Zeitschrift für Physik
authorswithroles_txt_mv	Barshay, Saul @@aut@@
publishDateDaySort_date	1997-12-01T00:00:00Z
hierarchy_top_id	254911307
id	SPR003727890
language_de	englisch
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author	Barshay, Saul
spellingShingle	Barshay, Saul misc Decay Width misc Charged Lepton misc Planck Scale misc Baryon Asymmetry misc Lepton Asymmetry CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton
authorStr	Barshay, Saul
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topic_title	CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton Decay Width (dpeaa)DE-He213 Charged Lepton (dpeaa)DE-He213 Planck Scale (dpeaa)DE-He213 Baryon Asymmetry (dpeaa)DE-He213 Lepton Asymmetry (dpeaa)DE-He213
topic	misc Decay Width misc Charged Lepton misc Planck Scale misc Baryon Asymmetry misc Lepton Asymmetry
topic_unstemmed	misc Decay Width misc Charged Lepton misc Planck Scale misc Baryon Asymmetry misc Lepton Asymmetry
topic_browse	misc Decay Width misc Charged Lepton misc Planck Scale misc Baryon Asymmetry misc Lepton Asymmetry
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton
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title_full	CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton
author_sort	Barshay, Saul
journal	Zeitschrift für Physik
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author_browse	Barshay, Saul
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author-letter	Barshay, Saul
doi_str_mv	10.1007/s002880050435
title_sort	cpt noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton
title_auth	CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton
abstract	Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. © Springer-Verlag 1997
abstractGer	Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. © Springer-Verlag 1997
abstract_unstemmed	Abstract A primary lepton-antilepton asymmetry provides the seed for the present empirical baryon-antibaryon asymmetry in a phenomenological model with a small, effectively spontaneous violation of CPT invariance at the origin. An experimentally accessible possibility is that the mass of a charged lepton, measured in the present era, can differ slightly from the mass of the antilepton, with a maximum possible difference at the level of (10 −9 - 10 −8). For electron and positron this is a mass difference with magnitude (0.001 - 0.01) eV, somewhat below the present empirical upper limit of 0.02 eV. © Springer-Verlag 1997
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container_issue	4
title_short	CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton
url	https://dx.doi.org/10.1007/s002880050435
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doi_str	10.1007/s002880050435
up_date	2024-07-03T21:17:20.550Z
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CPT noninvariance: a model for an initial lepton asymmetry due to unequal masses for lepton and antilepton

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