Time reversal and the neutron
Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-revers...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Chupp, T. E. [verfasserIn] Cooper, R. L. [verfasserIn] Coulter, K. P. [verfasserIn] Freedman, S. J. [verfasserIn] Fujikawa, B. K. [verfasserIn] Jones, G. L. [verfasserIn] Garcia, A. [verfasserIn] Mumm, H. P. [verfasserIn] Nico, J. S. [verfasserIn] Thompson, A. K. [verfasserIn] Trull, C. [verfasserIn] Wietfeldt, F. E. [verfasserIn] Wilkerson, J. F. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975, 214(2013), 1-3 vom: 19. Feb., Seite 97-104 |
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| Übergeordnetes Werk: |
volume:214 ; year:2013 ; number:1-3 ; day:19 ; month:02 ; pages:97-104 |
| Links: |
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| DOI / URN: |
10.1007/s10751-013-0776-y |
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| Katalog-ID: |
SPR013006975 |
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| 520 | |a Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. | ||
| 650 | 4 | |a Time-reversal invariance |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neutron decay |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Beta decay |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Cooper, R. L. |e verfasserin |4 aut | |
| 700 | 1 | |a Coulter, K. P. |e verfasserin |4 aut | |
| 700 | 1 | |a Freedman, S. J. |e verfasserin |4 aut | |
| 700 | 1 | |a Fujikawa, B. K. |e verfasserin |4 aut | |
| 700 | 1 | |a Jones, G. L. |e verfasserin |4 aut | |
| 700 | 1 | |a Garcia, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Mumm, H. P. |e verfasserin |4 aut | |
| 700 | 1 | |a Nico, J. S. |e verfasserin |4 aut | |
| 700 | 1 | |a Thompson, A. K. |e verfasserin |4 aut | |
| 700 | 1 | |a Trull, C. |e verfasserin |4 aut | |
| 700 | 1 | |a Wietfeldt, F. E. |e verfasserin |4 aut | |
| 700 | 1 | |a Wilkerson, J. F. |e verfasserin |4 aut | |
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10.1007/s10751-013-0776-y doi (DE-627)SPR013006975 (SPR)s10751-013-0776-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Chupp, T. E. verfasserin aut Time reversal and the neutron 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. Time-reversal invariance (dpeaa)DE-He213 Neutron decay (dpeaa)DE-He213 Beta decay (dpeaa)DE-He213 Cooper, R. L. verfasserin aut Coulter, K. P. verfasserin aut Freedman, S. J. verfasserin aut Fujikawa, B. K. verfasserin aut Jones, G. L. verfasserin aut Garcia, A. verfasserin aut Mumm, H. P. verfasserin aut Nico, J. S. verfasserin aut Thompson, A. K. verfasserin aut Trull, C. verfasserin aut Wietfeldt, F. E. verfasserin aut Wilkerson, J. F. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 214(2013), 1-3 vom: 19. Feb., Seite 97-104 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:214 year:2013 number:1-3 day:19 month:02 pages:97-104 https://dx.doi.org/10.1007/s10751-013-0776-y 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_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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 214 2013 1-3 19 02 97-104 |
| spelling |
10.1007/s10751-013-0776-y doi (DE-627)SPR013006975 (SPR)s10751-013-0776-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Chupp, T. E. verfasserin aut Time reversal and the neutron 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. Time-reversal invariance (dpeaa)DE-He213 Neutron decay (dpeaa)DE-He213 Beta decay (dpeaa)DE-He213 Cooper, R. L. verfasserin aut Coulter, K. P. verfasserin aut Freedman, S. J. verfasserin aut Fujikawa, B. K. verfasserin aut Jones, G. L. verfasserin aut Garcia, A. verfasserin aut Mumm, H. P. verfasserin aut Nico, J. S. verfasserin aut Thompson, A. K. verfasserin aut Trull, C. verfasserin aut Wietfeldt, F. E. verfasserin aut Wilkerson, J. F. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 214(2013), 1-3 vom: 19. Feb., Seite 97-104 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:214 year:2013 number:1-3 day:19 month:02 pages:97-104 https://dx.doi.org/10.1007/s10751-013-0776-y 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_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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 214 2013 1-3 19 02 97-104 |
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10.1007/s10751-013-0776-y doi (DE-627)SPR013006975 (SPR)s10751-013-0776-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Chupp, T. E. verfasserin aut Time reversal and the neutron 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. Time-reversal invariance (dpeaa)DE-He213 Neutron decay (dpeaa)DE-He213 Beta decay (dpeaa)DE-He213 Cooper, R. L. verfasserin aut Coulter, K. P. verfasserin aut Freedman, S. J. verfasserin aut Fujikawa, B. K. verfasserin aut Jones, G. L. verfasserin aut Garcia, A. verfasserin aut Mumm, H. P. verfasserin aut Nico, J. S. verfasserin aut Thompson, A. K. verfasserin aut Trull, C. verfasserin aut Wietfeldt, F. E. verfasserin aut Wilkerson, J. F. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 214(2013), 1-3 vom: 19. Feb., Seite 97-104 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:214 year:2013 number:1-3 day:19 month:02 pages:97-104 https://dx.doi.org/10.1007/s10751-013-0776-y 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_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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 214 2013 1-3 19 02 97-104 |
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10.1007/s10751-013-0776-y doi (DE-627)SPR013006975 (SPR)s10751-013-0776-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Chupp, T. E. verfasserin aut Time reversal and the neutron 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. Time-reversal invariance (dpeaa)DE-He213 Neutron decay (dpeaa)DE-He213 Beta decay (dpeaa)DE-He213 Cooper, R. L. verfasserin aut Coulter, K. P. verfasserin aut Freedman, S. J. verfasserin aut Fujikawa, B. K. verfasserin aut Jones, G. L. verfasserin aut Garcia, A. verfasserin aut Mumm, H. P. verfasserin aut Nico, J. S. verfasserin aut Thompson, A. K. verfasserin aut Trull, C. verfasserin aut Wietfeldt, F. E. verfasserin aut Wilkerson, J. F. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 214(2013), 1-3 vom: 19. Feb., Seite 97-104 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:214 year:2013 number:1-3 day:19 month:02 pages:97-104 https://dx.doi.org/10.1007/s10751-013-0776-y 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_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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 214 2013 1-3 19 02 97-104 |
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10.1007/s10751-013-0776-y doi (DE-627)SPR013006975 (SPR)s10751-013-0776-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Chupp, T. E. verfasserin aut Time reversal and the neutron 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. Time-reversal invariance (dpeaa)DE-He213 Neutron decay (dpeaa)DE-He213 Beta decay (dpeaa)DE-He213 Cooper, R. L. verfasserin aut Coulter, K. P. verfasserin aut Freedman, S. J. verfasserin aut Fujikawa, B. K. verfasserin aut Jones, G. L. verfasserin aut Garcia, A. verfasserin aut Mumm, H. P. verfasserin aut Nico, J. S. verfasserin aut Thompson, A. K. verfasserin aut Trull, C. verfasserin aut Wietfeldt, F. E. verfasserin aut Wilkerson, J. F. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 214(2013), 1-3 vom: 19. Feb., Seite 97-104 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:214 year:2013 number:1-3 day:19 month:02 pages:97-104 https://dx.doi.org/10.1007/s10751-013-0776-y 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_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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 214 2013 1-3 19 02 97-104 |
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Enthalten in Hyperfine interactions 214(2013), 1-3 vom: 19. Feb., Seite 97-104 volume:214 year:2013 number:1-3 day:19 month:02 pages:97-104 |
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Chupp, T. E. @@aut@@ Cooper, R. L. @@aut@@ Coulter, K. P. @@aut@@ Freedman, S. J. @@aut@@ Fujikawa, B. K. @@aut@@ Jones, G. L. @@aut@@ Garcia, A. @@aut@@ Mumm, H. P. @@aut@@ Nico, J. S. @@aut@@ Thompson, A. K. @@aut@@ Trull, C. @@aut@@ Wietfeldt, F. E. @@aut@@ Wilkerson, J. F. @@aut@@ |
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Chupp, T. E. |
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Chupp, T. E. ddc 530 bkl 33.00 misc Time-reversal invariance misc Neutron decay misc Beta decay Time reversal and the neutron |
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Time reversal and the neutron |
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Time reversal and the neutron |
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Chupp, T. E. Cooper, R. L. Coulter, K. P. Freedman, S. J. Fujikawa, B. K. Jones, G. L. Garcia, A. Mumm, H. P. Nico, J. S. Thompson, A. K. Trull, C. Wietfeldt, F. E. Wilkerson, J. F. |
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time reversal and the neutron |
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Time reversal and the neutron |
| abstract |
Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. |
| abstractGer |
Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. |
| abstract_unstemmed |
Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. This result also improves constrains on certain non-VA interactions. |
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Time reversal and the neutron |
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Cooper, R. L. Coulter, K. P. Freedman, S. J. Fujikawa, B. K. Jones, G. L. Garcia, A. Mumm, H. P. Nico, J. S. Thompson, A. K. Trull, C. Wietfeldt, F. E. Wilkerson, J. F. |
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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">SPR013006975</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111000610.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201005s2013 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10751-013-0776-y</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR013006975</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10751-013-0776-y-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="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Chupp, T. E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Time reversal and the neutron</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2013</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="520" ind1=" " ind2=" "><subfield code="a">Abstract We have measured the triple correlation $D\langle\vec J_n\rangle/J_n\cdot (\vec\beta_e\times\hat p_\nu)$ with a polarized cold-neutron beam (Mumm et al., Phys Rev Lett 107:102301, 2011; Chupp et al., Phys Rev C 86:035505, 2012). A non-zero value of D can arise due to parity-even-time-reversal-odd interactions that imply CP violation. Final-state effects also contribute to D at the level of $ 10^{ − 5} $ and can be calculated with precision of 1 % or better. The D coefficient is uniquely sensitive to the imaginary part of the ratio of axial-vector and vector beta-decay amplitudes as well as to scalar and tensor interactions that could arise due to beyond-Standard-Model physics. Over 300 million proton-electron coincidence events were used in a blind analysis with the result D = [ − 0.94±1.89 (stat)±0.97(sys)]×$ 10^{ − 4} $. Assuming only vector and axial vector interactions in beta decay, our result can be interpreted as a measure of the phase of the axial-vector coupling relative to the vector coupling, $\phi_{\rm AV}= 180.012^\circ \pm 0.028^\circ$. 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J.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fujikawa, B. K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jones, G. L.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Garcia, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mumm, H. P.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Nico, J. S.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Thompson, A. K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Trull, C.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wietfeldt, F. E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wilkerson, J. 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