$ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction
Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Day, T. B. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1959 |
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| Anmerkung: |
© Società Italiana di Fisica 1959 |
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| Übergeordnetes Werk: |
Enthalten in: Il nuovo cimento - Pisa, 1855, 13(1959), 3 vom: Aug., Seite 614-627 |
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| Übergeordnetes Werk: |
volume:13 ; year:1959 ; number:3 ; month:08 ; pages:614-627 |
| Links: |
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| DOI / URN: |
10.1007/BF02732777 |
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| Katalog-ID: |
SPR037316672 |
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| 008 | 201007s1959 xx |||||o 00| ||eng c | ||
| 024 | 7 | |a 10.1007/BF02732777 |2 doi | |
| 035 | |a (DE-627)SPR037316672 | ||
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| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 100 | 1 | |a Day, T. B. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
| 264 | 1 | |c 1959 | |
| 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 1959 | ||
| 520 | |a Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. | ||
| 700 | 1 | |a Snow, G. A. |4 aut | |
| 700 | 1 | |a Sucher, J. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Il nuovo cimento |d Pisa, 1855 |g 13(1959), 3 vom: Aug., Seite 614-627 |w (DE-627)626757762 |w (DE-600)2554784-7 |x 1827-6121 |7 nnns |
| 773 | 1 | 8 | |g volume:13 |g year:1959 |g number:3 |g month:08 |g pages:614-627 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/BF02732777 |z lizenzpflichtig |3 Volltext |
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| 912 | |a GBV_ILN_2112 | ||
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| 912 | |a GBV_ILN_2118 | ||
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| 912 | |a GBV_ILN_2143 | ||
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| 952 | |d 13 |j 1959 |e 3 |c 08 |h 614-627 | ||
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article:18276121:1959----::br0eaieaiyntedhrexhneecineaieaiynt |
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1959 |
| publishDate |
1959 |
| allfields |
10.1007/BF02732777 doi (DE-627)SPR037316672 (SPR)BF02732777-e DE-627 ger DE-627 rakwb eng Day, T. B. verfasserin aut $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction 1959 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1959 Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. Snow, G. A. aut Sucher, J. aut Enthalten in Il nuovo cimento Pisa, 1855 13(1959), 3 vom: Aug., Seite 614-627 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:13 year:1959 number:3 month:08 pages:614-627 https://dx.doi.org/10.1007/BF02732777 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_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 13 1959 3 08 614-627 |
| spelling |
10.1007/BF02732777 doi (DE-627)SPR037316672 (SPR)BF02732777-e DE-627 ger DE-627 rakwb eng Day, T. B. verfasserin aut $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction 1959 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1959 Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. Snow, G. A. aut Sucher, J. aut Enthalten in Il nuovo cimento Pisa, 1855 13(1959), 3 vom: Aug., Seite 614-627 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:13 year:1959 number:3 month:08 pages:614-627 https://dx.doi.org/10.1007/BF02732777 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_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 13 1959 3 08 614-627 |
| allfields_unstemmed |
10.1007/BF02732777 doi (DE-627)SPR037316672 (SPR)BF02732777-e DE-627 ger DE-627 rakwb eng Day, T. B. verfasserin aut $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction 1959 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1959 Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. Snow, G. A. aut Sucher, J. aut Enthalten in Il nuovo cimento Pisa, 1855 13(1959), 3 vom: Aug., Seite 614-627 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:13 year:1959 number:3 month:08 pages:614-627 https://dx.doi.org/10.1007/BF02732777 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_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 13 1959 3 08 614-627 |
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10.1007/BF02732777 doi (DE-627)SPR037316672 (SPR)BF02732777-e DE-627 ger DE-627 rakwb eng Day, T. B. verfasserin aut $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction 1959 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1959 Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. Snow, G. A. aut Sucher, J. aut Enthalten in Il nuovo cimento Pisa, 1855 13(1959), 3 vom: Aug., Seite 614-627 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:13 year:1959 number:3 month:08 pages:614-627 https://dx.doi.org/10.1007/BF02732777 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_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 13 1959 3 08 614-627 |
| allfieldsSound |
10.1007/BF02732777 doi (DE-627)SPR037316672 (SPR)BF02732777-e DE-627 ger DE-627 rakwb eng Day, T. B. verfasserin aut $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction 1959 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1959 Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. Snow, G. A. aut Sucher, J. aut Enthalten in Il nuovo cimento Pisa, 1855 13(1959), 3 vom: Aug., Seite 614-627 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:13 year:1959 number:3 month:08 pages:614-627 https://dx.doi.org/10.1007/BF02732777 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_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 13 1959 3 08 614-627 |
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Enthalten in Il nuovo cimento 13(1959), 3 vom: Aug., Seite 614-627 volume:13 year:1959 number:3 month:08 pages:614-627 |
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Il nuovo cimento |
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Day, T. B. @@aut@@ Snow, G. A. @@aut@@ Sucher, J. @@aut@@ |
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1959-08-01T00:00:00Z |
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|
| author |
Day, T. B. |
| spellingShingle |
Day, T. B. $ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
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Day, T. B. |
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$ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Il nuovo cimento |
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Il nuovo cimento |
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| title |
$ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
| ctrlnum |
(DE-627)SPR037316672 (SPR)BF02732777-e |
| title_full |
$ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
| author_sort |
Day, T. B. |
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Il nuovo cimento |
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Il nuovo cimento |
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eng |
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1959 |
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614 |
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Day, T. B. Snow, G. A. Sucher, J. |
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13 |
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Elektronische Aufsätze |
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Day, T. B. |
| doi_str_mv |
10.1007/BF02732777 |
| title_sort |
$ k^{−} $,%$\bar k^0 %$ relative parity and the $ k^{−} $-d charge exchange reactionrelative parity and the $ k^{−} $-d charge exchange reaction |
| title_auth |
$ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
| abstract |
Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. © Società Italiana di Fisica 1959 |
| abstractGer |
Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. © Società Italiana di Fisica 1959 |
| abstract_unstemmed |
Summary The reaction $ K^{−} $ + d →%$\bar K^0 %$ + 2n is studied in the hope that limitations on the final states for the two neutrons due to statistics will help differentiate between even and odd relative parity of the $ K^{−} $ and%$\bar K^0 %$ mesons. The total cross-section for the reaction is calculated in the impulse approximation, and expressed in terms of the corresponding hydrogen cross-section for both even and odd parity. The calculations are carried outa) with the use of antisymmetrized plane waves for the two neutrons, andb) in the closure approximation. The ratio of the odd to even parity cross-sections is about a factor of two in either approximation. The total cross-section for odd parity in the plane wave approximation is found to be about 4 mb at a $ K^{−} $ laboratory momentum of 136 MeV/c. © Società Italiana di Fisica 1959 |
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3 |
| title_short |
$ K^{−} $,%$\bar K^0 %$ relative parity and the $ K^{−} $-d charge exchange reactionrelative parity and the $ K^{−} $-d charge exchange reaction |
| url |
https://dx.doi.org/10.1007/BF02732777 |
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Snow, G. A. Sucher, J. |
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Snow, G. A. Sucher, J. |
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| doi_str |
10.1007/BF02732777 |
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2024-07-03T22:12:29.218Z |
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1803597642957062144 |
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| score |
7.4009314 |