The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model
Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the fa...
Ausführliche Beschreibung
Autor*in: |
Sheng, Jin-Huan [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2021 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: International journal of theoretical physics - New York, NY : Springer Science + Business Media B.V., 1968, 60(2021), 1 vom: Jan., Seite 26-46 |
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Übergeordnetes Werk: |
volume:60 ; year:2021 ; number:1 ; month:01 ; pages:26-46 |
Links: |
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DOI / URN: |
10.1007/s10773-020-04654-3 |
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Katalog-ID: |
SPR042828376 |
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520 | |a Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. | ||
650 | 4 | |a Baryon decay |7 (dpeaa)DE-He213 | |
650 | 4 | |a Rare decay |7 (dpeaa)DE-He213 | |
650 | 4 | |a model |7 (dpeaa)DE-He213 | |
650 | 4 | |a Lepton flavour non-universality |7 (dpeaa)DE-He213 | |
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10.1007/s10773-020-04654-3 doi (DE-627)SPR042828376 (DE-599)SPRs10773-020-04654-3-e (SPR)s10773-020-04654-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sheng, Jin-Huan verfasserin aut The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. Baryon decay (dpeaa)DE-He213 Rare decay (dpeaa)DE-He213 model (dpeaa)DE-He213 Lepton flavour non-universality (dpeaa)DE-He213 Enthalten in International journal of theoretical physics New York, NY : Springer Science + Business Media B.V., 1968 60(2021), 1 vom: Jan., Seite 26-46 (DE-627)320567966 (DE-600)2016168-2 1572-9575 nnns volume:60 year:2021 number:1 month:01 pages:26-46 https://dx.doi.org/10.1007/s10773-020-04654-3 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 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_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_2188 GBV_ILN_2190 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_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_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_4393 GBV_ILN_4700 33.00 ASE AR 60 2021 1 01 26-46 |
spelling |
10.1007/s10773-020-04654-3 doi (DE-627)SPR042828376 (DE-599)SPRs10773-020-04654-3-e (SPR)s10773-020-04654-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sheng, Jin-Huan verfasserin aut The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. Baryon decay (dpeaa)DE-He213 Rare decay (dpeaa)DE-He213 model (dpeaa)DE-He213 Lepton flavour non-universality (dpeaa)DE-He213 Enthalten in International journal of theoretical physics New York, NY : Springer Science + Business Media B.V., 1968 60(2021), 1 vom: Jan., Seite 26-46 (DE-627)320567966 (DE-600)2016168-2 1572-9575 nnns volume:60 year:2021 number:1 month:01 pages:26-46 https://dx.doi.org/10.1007/s10773-020-04654-3 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 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_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_2188 GBV_ILN_2190 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_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_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_4393 GBV_ILN_4700 33.00 ASE AR 60 2021 1 01 26-46 |
allfields_unstemmed |
10.1007/s10773-020-04654-3 doi (DE-627)SPR042828376 (DE-599)SPRs10773-020-04654-3-e (SPR)s10773-020-04654-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sheng, Jin-Huan verfasserin aut The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. Baryon decay (dpeaa)DE-He213 Rare decay (dpeaa)DE-He213 model (dpeaa)DE-He213 Lepton flavour non-universality (dpeaa)DE-He213 Enthalten in International journal of theoretical physics New York, NY : Springer Science + Business Media B.V., 1968 60(2021), 1 vom: Jan., Seite 26-46 (DE-627)320567966 (DE-600)2016168-2 1572-9575 nnns volume:60 year:2021 number:1 month:01 pages:26-46 https://dx.doi.org/10.1007/s10773-020-04654-3 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 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_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_2188 GBV_ILN_2190 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_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_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_4393 GBV_ILN_4700 33.00 ASE AR 60 2021 1 01 26-46 |
allfieldsGer |
10.1007/s10773-020-04654-3 doi (DE-627)SPR042828376 (DE-599)SPRs10773-020-04654-3-e (SPR)s10773-020-04654-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sheng, Jin-Huan verfasserin aut The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. Baryon decay (dpeaa)DE-He213 Rare decay (dpeaa)DE-He213 model (dpeaa)DE-He213 Lepton flavour non-universality (dpeaa)DE-He213 Enthalten in International journal of theoretical physics New York, NY : Springer Science + Business Media B.V., 1968 60(2021), 1 vom: Jan., Seite 26-46 (DE-627)320567966 (DE-600)2016168-2 1572-9575 nnns volume:60 year:2021 number:1 month:01 pages:26-46 https://dx.doi.org/10.1007/s10773-020-04654-3 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 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_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_2188 GBV_ILN_2190 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_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_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_4393 GBV_ILN_4700 33.00 ASE AR 60 2021 1 01 26-46 |
allfieldsSound |
10.1007/s10773-020-04654-3 doi (DE-627)SPR042828376 (DE-599)SPRs10773-020-04654-3-e (SPR)s10773-020-04654-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sheng, Jin-Huan verfasserin aut The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. Baryon decay (dpeaa)DE-He213 Rare decay (dpeaa)DE-He213 model (dpeaa)DE-He213 Lepton flavour non-universality (dpeaa)DE-He213 Enthalten in International journal of theoretical physics New York, NY : Springer Science + Business Media B.V., 1968 60(2021), 1 vom: Jan., Seite 26-46 (DE-627)320567966 (DE-600)2016168-2 1572-9575 nnns volume:60 year:2021 number:1 month:01 pages:26-46 https://dx.doi.org/10.1007/s10773-020-04654-3 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 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_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_2188 GBV_ILN_2190 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_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_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_4393 GBV_ILN_4700 33.00 ASE AR 60 2021 1 01 26-46 |
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We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. 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Sheng, Jin-Huan |
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Sheng, Jin-Huan ddc 530 bkl 33.00 misc Baryon decay misc Rare decay misc model misc Lepton flavour non-universality The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model |
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530 ASE 33.00 bkl The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model Baryon decay (dpeaa)DE-He213 Rare decay (dpeaa)DE-He213 model (dpeaa)DE-He213 Lepton flavour non-universality (dpeaa)DE-He213 |
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The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model |
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analysis of b → sℓ+ℓ− in the family non-universal $z^{\prime }$ model |
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The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model |
abstract |
Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. |
abstractGer |
Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. |
abstract_unstemmed |
Abstract Motivated by recent experimental results on $ R_{K^{(*)}}$ and $\mathcal {P}^{\prime }_{5}$ in B → K(∗)ℓ+ℓ− and the latest improved measurement result in Λb →Λℓ+ℓ− processes. We will investigate the rare decay on the flavor-changing neutral current process of Λb baryon and B meson in the family non-universal $Z^{\prime }$ model, which is one of the well motivated extensions of the Standard Model. We have obtained the upper limits on the NP coupling parameters from the recent experimental measurements of the decay processes Bs → ℓ+ℓ−B → K(∗)ℓ+ℓ−, B → Xsℓ+ℓ− and Λb →Λℓ+ℓ−. Then we analyze the branching ratio, the normalized forward-backward asymmetries and a series of angular observables in the Standard Model and family non-universal $Z^{\prime }$ model. We find that the constrained NP coupling parameters have few obvious effects on the process b → sμ+μ−, nevertheless, NP coupling parameters have very large effects on the process b → sτ+τ−. In the future we expect the precision measurements of these observables will be researched by LHCb and Belle-II. |
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container_issue |
1 |
title_short |
The Analysis of b → sℓ+ℓ− in the Family Non-Universal $Z^{\prime }$ Model |
url |
https://dx.doi.org/10.1007/s10773-020-04654-3 |
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doi_str |
10.1007/s10773-020-04654-3 |
up_date |
2024-07-03T15:02:36.050Z |
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|
score |
7.399581 |