On fermion number and its conservation

Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Pati, J. C. [verfasserIn] Salam, A. Strathdee, J.

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	1975

Anmerkung:	© Società Italiana di Fisica 1975

Übergeordnetes Werk:	Enthalten in: Il nuovo cimento - [S.l.] : Italian Physical Society, 1965, 26(1975), 1 vom: 01. März, Seite 72-83
Übergeordnetes Werk:	volume:26 ; year:1975 ; number:1 ; day:01 ; month:03 ; pages:72-83

Links:	Volltext

DOI / URN:	10.1007/BF02849600

Katalog-ID:	SPR037385054

Internformat


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100	1		\|a Pati, J. C. \|e verfasserin \|4 aut
245	1	0	\|a On fermion number and its conservation
264		1	\|c 1975
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520			\|a Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator.
700	1		\|a Salam, A. \|4 aut
700	1		\|a Strathdee, J. \|4 aut
773	0	8	\|i Enthalten in \|t Il nuovo cimento \|d [S.l.] : Italian Physical Society, 1965 \|g 26(1975), 1 vom: 01. März, Seite 72-83 \|w (DE-627)627248667 \|w (DE-600)2556213-7 \|x 1826-9869 \|7 nnns
773	1	8	\|g volume:26 \|g year:1975 \|g number:1 \|g day:01 \|g month:03 \|g pages:72-83
856	4	0	\|u https://dx.doi.org/10.1007/BF02849600 \|z lizenzpflichtig \|3 Volltext
912			\|a GBV_USEFLAG_A
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912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
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_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_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 26 \|j 1975 \|e 1 \|b 01 \|c 03 \|h 72-83

Indexfelder

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matchkey_str	article:18269869:1975----::nemonmeadtcn
hierarchy_sort_str	1975
publishDate	1975
allfields	10.1007/BF02849600 doi (DE-627)SPR037385054 (SPR)BF02849600-e DE-627 ger DE-627 rakwb eng Pati, J. C. verfasserin aut On fermion number and its conservation 1975 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1975 Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. Salam, A. aut Strathdee, J. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 26(1975), 1 vom: 01. März, Seite 72-83 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:26 year:1975 number:1 day:01 month:03 pages:72-83 https://dx.doi.org/10.1007/BF02849600 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_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_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 26 1975 1 01 03 72-83
spelling	10.1007/BF02849600 doi (DE-627)SPR037385054 (SPR)BF02849600-e DE-627 ger DE-627 rakwb eng Pati, J. C. verfasserin aut On fermion number and its conservation 1975 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1975 Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. Salam, A. aut Strathdee, J. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 26(1975), 1 vom: 01. März, Seite 72-83 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:26 year:1975 number:1 day:01 month:03 pages:72-83 https://dx.doi.org/10.1007/BF02849600 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_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_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 26 1975 1 01 03 72-83
allfields_unstemmed	10.1007/BF02849600 doi (DE-627)SPR037385054 (SPR)BF02849600-e DE-627 ger DE-627 rakwb eng Pati, J. C. verfasserin aut On fermion number and its conservation 1975 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1975 Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. Salam, A. aut Strathdee, J. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 26(1975), 1 vom: 01. März, Seite 72-83 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:26 year:1975 number:1 day:01 month:03 pages:72-83 https://dx.doi.org/10.1007/BF02849600 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_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_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 26 1975 1 01 03 72-83
allfieldsGer	10.1007/BF02849600 doi (DE-627)SPR037385054 (SPR)BF02849600-e DE-627 ger DE-627 rakwb eng Pati, J. C. verfasserin aut On fermion number and its conservation 1975 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1975 Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. Salam, A. aut Strathdee, J. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 26(1975), 1 vom: 01. März, Seite 72-83 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:26 year:1975 number:1 day:01 month:03 pages:72-83 https://dx.doi.org/10.1007/BF02849600 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_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_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 26 1975 1 01 03 72-83
allfieldsSound	10.1007/BF02849600 doi (DE-627)SPR037385054 (SPR)BF02849600-e DE-627 ger DE-627 rakwb eng Pati, J. C. verfasserin aut On fermion number and its conservation 1975 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1975 Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. Salam, A. aut Strathdee, J. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 26(1975), 1 vom: 01. März, Seite 72-83 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:26 year:1975 number:1 day:01 month:03 pages:72-83 https://dx.doi.org/10.1007/BF02849600 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_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_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 26 1975 1 01 03 72-83
language	English
source	Enthalten in Il nuovo cimento 26(1975), 1 vom: 01. März, Seite 72-83 volume:26 year:1975 number:1 day:01 month:03 pages:72-83
sourceStr	Enthalten in Il nuovo cimento 26(1975), 1 vom: 01. März, Seite 72-83 volume:26 year:1975 number:1 day:01 month:03 pages:72-83
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container_title	Il nuovo cimento
authorswithroles_txt_mv	Pati, J. C. @@aut@@ Salam, A. @@aut@@ Strathdee, J. @@aut@@
publishDateDaySort_date	1975-03-01T00:00:00Z
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author	Pati, J. C.
spellingShingle	Pati, J. C. On fermion number and its conservation
authorStr	Pati, J. C.
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title	On fermion number and its conservation
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title_sort	on fermion number and its conservation
title_auth	On fermion number and its conservation
abstract	Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. © Società Italiana di Fisica 1975
abstractGer	Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. © Società Italiana di Fisica 1975
abstract_unstemmed	Summary We raise the question if the fermion number (F = B + L) is absolutely conserved. Neutrinoless double-β-decay experiments give upper limits on ¦ΔL¦ = 2 transitions. Experiments on the stability of the deuteron against decay into pions would give analogous limits on ¦ΔB¦ = 6 transitions, while proton stability experiments set limits on ¦δF¦ = 0, ΔB = - ΔL as well as on transitions involving ¦ΔF¦≠ 0. HereB = + 1 for (integer or zero charge) quarks,B = -1 for antiquarks, whileL is the lepton number. Remarking that the maximal symmetry group for the kinematic-energy terms of a set ofn four-component Dirac fields isSU2n rather than $ U_{1} $ $ xSU_{Ln} $ XSURn (with the extra gauge currents carrying fermion number ±2), we briefly investigate the possibility of constructing spontaneously broken gauge theories where the fermion number appears as a non-Abelian generator. © Società Italiana di Fisica 1975
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container_issue	1
title_short	On fermion number and its conservation
url	https://dx.doi.org/10.1007/BF02849600
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author2	Salam, A. Strathdee, J.
author2Str	Salam, A. Strathdee, J.
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doi_str	10.1007/BF02849600
up_date	2024-07-03T22:32:13.641Z
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score	7.3992968

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On fermion number and its conservation

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