Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem
Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that th...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Alles, W. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1972 |
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| Anmerkung: |
© Società Italiana di Fisica 1972 |
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| Übergeordnetes Werk: |
Enthalten in: Il nuovo cimento - [S.l.] : Italian Physical Society, 1965, 10(1972), 2 vom: Juli, Seite 325-342 |
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| Übergeordnetes Werk: |
volume:10 ; year:1972 ; number:2 ; month:07 ; pages:325-342 |
| Links: |
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| DOI / URN: |
10.1007/BF02895768 |
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| Katalog-ID: |
SPR037374222 |
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| 008 | 201007s1972 xx |||||o 00| ||eng c | ||
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| 035 | |a (DE-627)SPR037374222 | ||
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| 041 | |a eng | ||
| 100 | 1 | |a Alles, W. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
| 264 | 1 | |c 1972 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
| 338 | |a Online-Ressource |b cr |2 rdacarrier | ||
| 500 | |a © Società Italiana di Fisica 1972 | ||
| 520 | |a Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. | ||
| 700 | 1 | |a Pati, J. C. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Il nuovo cimento |d [S.l.] : Italian Physical Society, 1965 |g 10(1972), 2 vom: Juli, Seite 325-342 |w (DE-627)627248667 |w (DE-600)2556213-7 |x 1826-9869 |7 nnns |
| 773 | 1 | 8 | |g volume:10 |g year:1972 |g number:2 |g month:07 |g pages:325-342 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/BF02895768 |z lizenzpflichtig |3 Volltext |
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| 952 | |d 10 |j 1972 |e 2 |c 07 |h 325-342 | ||
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article:18269869:1972----::etfrpsilcasfpnainsltosohk |
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1972 |
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1972 |
| allfields |
10.1007/BF02895768 doi (DE-627)SPR037374222 (SPR)BF02895768-e DE-627 ger DE-627 rakwb eng Alles, W. verfasserin aut Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem 1972 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1972 Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. Pati, J. C. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 10(1972), 2 vom: Juli, Seite 325-342 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:10 year:1972 number:2 month:07 pages:325-342 https://dx.doi.org/10.1007/BF02895768 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 10 1972 2 07 325-342 |
| spelling |
10.1007/BF02895768 doi (DE-627)SPR037374222 (SPR)BF02895768-e DE-627 ger DE-627 rakwb eng Alles, W. verfasserin aut Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem 1972 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1972 Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. Pati, J. C. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 10(1972), 2 vom: Juli, Seite 325-342 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:10 year:1972 number:2 month:07 pages:325-342 https://dx.doi.org/10.1007/BF02895768 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 10 1972 2 07 325-342 |
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10.1007/BF02895768 doi (DE-627)SPR037374222 (SPR)BF02895768-e DE-627 ger DE-627 rakwb eng Alles, W. verfasserin aut Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem 1972 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1972 Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. Pati, J. C. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 10(1972), 2 vom: Juli, Seite 325-342 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:10 year:1972 number:2 month:07 pages:325-342 https://dx.doi.org/10.1007/BF02895768 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 10 1972 2 07 325-342 |
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10.1007/BF02895768 doi (DE-627)SPR037374222 (SPR)BF02895768-e DE-627 ger DE-627 rakwb eng Alles, W. verfasserin aut Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem 1972 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1972 Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. Pati, J. C. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 10(1972), 2 vom: Juli, Seite 325-342 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:10 year:1972 number:2 month:07 pages:325-342 https://dx.doi.org/10.1007/BF02895768 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 10 1972 2 07 325-342 |
| allfieldsSound |
10.1007/BF02895768 doi (DE-627)SPR037374222 (SPR)BF02895768-e DE-627 ger DE-627 rakwb eng Alles, W. verfasserin aut Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem 1972 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1972 Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. Pati, J. C. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 10(1972), 2 vom: Juli, Seite 325-342 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:10 year:1972 number:2 month:07 pages:325-342 https://dx.doi.org/10.1007/BF02895768 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 10 1972 2 07 325-342 |
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Enthalten in Il nuovo cimento 10(1972), 2 vom: Juli, Seite 325-342 volume:10 year:1972 number:2 month:07 pages:325-342 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR037374222</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230328184136.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s1972 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02895768</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR037374222</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)BF02895768-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Alles, W.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1972</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Società Italiana di Fisica 1972</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. 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Alles, W. |
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Alles, W. Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
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Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
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Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
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Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
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Alles, W. |
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10.1007/BF02895768 |
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tests for a possible class ofcp invariant solutions to the%$k_l \to \mu \bar \mu %$ problem |
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Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
| abstract |
Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. © Società Italiana di Fisica 1972 |
| abstractGer |
Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. © Società Italiana di Fisica 1972 |
| abstract_unstemmed |
Summary The possibility that the unitarity sum for the absorptive part of the%$K_L \to \mu \bar \mu %$ amplitude receives contribution in aCP-invariant manner from an on-mass-shell intermediate state involving a yet undetected light neutral boson (we call itx0) is considered. It is suggested that the most relevant intermediate state is thex0λ state withx0 having spin-parity $ 1^{−} $. It is pointed out that the existence of such a particle, if it is not already excluded by present experiments, can be tested unambiguously and relatively easily by two experiments:a) the measurement of the rate of the $ K_{L} $→x0+λ decay (thex0 may be looked for easily via its decays to ($ e^{−} %$ e^{+} $) and ($ μ^{−} %$ μ^{+} $) systems), andb) the production of thex0 by low-invariant-mass ($ e^{−} %$ e^{+} $) colliding-beam experiments. It is noted that thex0, if it exists, receives a «natural» interpretation only in framework of hadron symmetries higher than the familiarSU3-group. The production ofx0 by a host of production and decay processes is discussed subject to such an interpretation. © Società Italiana di Fisica 1972 |
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| container_issue |
2 |
| title_short |
Tests for a possible class ofCP invariant solutions to the%$K_L \to \mu \bar \mu %$ problem |
| url |
https://dx.doi.org/10.1007/BF02895768 |
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| author2 |
Pati, J. C. |
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Pati, J. C. |
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10.1007/BF02895768 |
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2024-07-03T22:28:58.364Z |
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| score |
7.398225 |