A dynamical calculation of the weak axial vector currentF/D ratio
Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2.
Gespeichert in:
| Autor*in: |
Diu, B. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1966 |
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| Schlagwörter: |
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| Anmerkung: |
© Società Italiana di Fisica 1966 |
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| Übergeordnetes Werk: |
Enthalten in: Il nuovo cimento - [S.l.] : Italian Physical Society, 1965, 42(1966), 3 vom: Apr., Seite 649-655 |
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| Übergeordnetes Werk: |
volume:42 ; year:1966 ; number:3 ; month:04 ; pages:649-655 |
| Links: |
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| DOI / URN: |
10.1007/BF02720542 |
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| Katalog-ID: |
SPR020614195 |
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| 100 | 1 | |a Diu, B. |e verfasserin |4 aut | |
| 245 | 1 | 2 | |a A dynamical calculation of the weak axial vector currentF/D ratio |
| 264 | 1 | |c 1966 | |
| 336 | |a Text |b txt |2 rdacontent | ||
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| 500 | |a © Società Italiana di Fisica 1966 | ||
| 520 | |a Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. | ||
| 650 | 4 | |a Dynamical Calculation |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Vector Current |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Pseudoscalar Meson |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Inhomogeneous Term |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Baryon Octet |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Van Royen, R. P. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Il nuovo cimento |d [S.l.] : Italian Physical Society, 1965 |g 42(1966), 3 vom: Apr., Seite 649-655 |w (DE-627)627248667 |w (DE-600)2556213-7 |x 1826-9869 |7 nnns |
| 773 | 1 | 8 | |g volume:42 |g year:1966 |g number:3 |g month:04 |g pages:649-655 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/BF02720542 |z lizenzpflichtig |3 Volltext |
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1966 |
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1966 |
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10.1007/BF02720542 doi (DE-627)SPR020614195 (SPR)BF02720542-e DE-627 ger DE-627 rakwb eng Diu, B. verfasserin aut A dynamical calculation of the weak axial vector currentF/D ratio 1966 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1966 Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. Dynamical Calculation (dpeaa)DE-He213 Vector Current (dpeaa)DE-He213 Pseudoscalar Meson (dpeaa)DE-He213 Inhomogeneous Term (dpeaa)DE-He213 Baryon Octet (dpeaa)DE-He213 Van Royen, R. P. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 42(1966), 3 vom: Apr., Seite 649-655 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:42 year:1966 number:3 month:04 pages:649-655 https://dx.doi.org/10.1007/BF02720542 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 42 1966 3 04 649-655 |
| spelling |
10.1007/BF02720542 doi (DE-627)SPR020614195 (SPR)BF02720542-e DE-627 ger DE-627 rakwb eng Diu, B. verfasserin aut A dynamical calculation of the weak axial vector currentF/D ratio 1966 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1966 Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. Dynamical Calculation (dpeaa)DE-He213 Vector Current (dpeaa)DE-He213 Pseudoscalar Meson (dpeaa)DE-He213 Inhomogeneous Term (dpeaa)DE-He213 Baryon Octet (dpeaa)DE-He213 Van Royen, R. P. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 42(1966), 3 vom: Apr., Seite 649-655 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:42 year:1966 number:3 month:04 pages:649-655 https://dx.doi.org/10.1007/BF02720542 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 42 1966 3 04 649-655 |
| allfields_unstemmed |
10.1007/BF02720542 doi (DE-627)SPR020614195 (SPR)BF02720542-e DE-627 ger DE-627 rakwb eng Diu, B. verfasserin aut A dynamical calculation of the weak axial vector currentF/D ratio 1966 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1966 Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. Dynamical Calculation (dpeaa)DE-He213 Vector Current (dpeaa)DE-He213 Pseudoscalar Meson (dpeaa)DE-He213 Inhomogeneous Term (dpeaa)DE-He213 Baryon Octet (dpeaa)DE-He213 Van Royen, R. P. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 42(1966), 3 vom: Apr., Seite 649-655 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:42 year:1966 number:3 month:04 pages:649-655 https://dx.doi.org/10.1007/BF02720542 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 42 1966 3 04 649-655 |
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10.1007/BF02720542 doi (DE-627)SPR020614195 (SPR)BF02720542-e DE-627 ger DE-627 rakwb eng Diu, B. verfasserin aut A dynamical calculation of the weak axial vector currentF/D ratio 1966 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1966 Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. Dynamical Calculation (dpeaa)DE-He213 Vector Current (dpeaa)DE-He213 Pseudoscalar Meson (dpeaa)DE-He213 Inhomogeneous Term (dpeaa)DE-He213 Baryon Octet (dpeaa)DE-He213 Van Royen, R. P. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 42(1966), 3 vom: Apr., Seite 649-655 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:42 year:1966 number:3 month:04 pages:649-655 https://dx.doi.org/10.1007/BF02720542 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 42 1966 3 04 649-655 |
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10.1007/BF02720542 doi (DE-627)SPR020614195 (SPR)BF02720542-e DE-627 ger DE-627 rakwb eng Diu, B. verfasserin aut A dynamical calculation of the weak axial vector currentF/D ratio 1966 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1966 Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. Dynamical Calculation (dpeaa)DE-He213 Vector Current (dpeaa)DE-He213 Pseudoscalar Meson (dpeaa)DE-He213 Inhomogeneous Term (dpeaa)DE-He213 Baryon Octet (dpeaa)DE-He213 Van Royen, R. P. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 42(1966), 3 vom: Apr., Seite 649-655 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:42 year:1966 number:3 month:04 pages:649-655 https://dx.doi.org/10.1007/BF02720542 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 42 1966 3 04 649-655 |
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English |
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Enthalten in Il nuovo cimento 42(1966), 3 vom: Apr., Seite 649-655 volume:42 year:1966 number:3 month:04 pages:649-655 |
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Enthalten in Il nuovo cimento 42(1966), 3 vom: Apr., Seite 649-655 volume:42 year:1966 number:3 month:04 pages:649-655 |
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Dynamical Calculation Vector Current Pseudoscalar Meson Inhomogeneous Term Baryon Octet |
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Il nuovo cimento |
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Diu, B. @@aut@@ Van Royen, R. P. @@aut@@ |
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1966-04-01T00:00:00Z |
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Diu, B. misc Dynamical Calculation misc Vector Current misc Pseudoscalar Meson misc Inhomogeneous Term misc Baryon Octet A dynamical calculation of the weak axial vector currentF/D ratio |
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A dynamical calculation of the weak axial vector currentF/D ratio Dynamical Calculation (dpeaa)DE-He213 Vector Current (dpeaa)DE-He213 Pseudoscalar Meson (dpeaa)DE-He213 Inhomogeneous Term (dpeaa)DE-He213 Baryon Octet (dpeaa)DE-He213 |
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dynamical calculation of the weak axial vector currentf/d ratio |
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A dynamical calculation of the weak axial vector currentF/D ratio |
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Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. © Società Italiana di Fisica 1966 |
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Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. © Società Italiana di Fisica 1966 |
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Summary The Dashen-Frautschi perturbation technique is applied to the weak axial vector current of baryons, with the result that it transforms like an octet member and that itsF/D ratio is approximately 1/2. © Società Italiana di Fisica 1966 |
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A dynamical calculation of the weak axial vector currentF/D ratio |
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