Impact of warped extra dimensions on the dipole coefficients in b → sγ transitions
We calculate the electro- and chromomagnetic dipole coefficients C7γ,8gand C˜7γ,8g$$ {\tilde{C}}_{7\gamma, 8g} $$in the context of the minimal Randall-Sundrum (RS) model with a Higgs sector localized on the IR brane using the five-dimensional (5D) approach, where the coefficients are expressed in te...
Gespeichert in:
| Hauptverfasser: | , , |
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
07 April 2016
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| In: |
Journal of high energy physics
Year: 2016, Heft: 4 |
| ISSN: | 1029-8479 |
| DOI: | 10.1007/JHEP04(2016)042 |
| Online-Zugang: | Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1007/JHEP04(2016)042
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| Verfasserangaben: | Raoul Malm, Matthias Neubert and Christoph Schmell |
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| 245 | 1 | 0 | |a Impact of warped extra dimensions on the dipole coefficients in b → sγ transitions |c Raoul Malm, Matthias Neubert and Christoph Schmell |
| 246 | 3 | 3 | |a Impact of warped extra dimensions on the dipole coefficients in b → s gamma transitions |
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| 520 | |a We calculate the electro- and chromomagnetic dipole coefficients C7γ,8gand C˜7γ,8g$$ {\tilde{C}}_{7\gamma, 8g} $$in the context of the minimal Randall-Sundrum (RS) model with a Higgs sector localized on the IR brane using the five-dimensional (5D) approach, where the coefficients are expressed in terms of integrals over 5D propagators. Since we keep the full dependence on the Yukawa matrices, the integral expressions are formally valid to all orders in v2/MKK2. In addition we relate our results to the expressions obtained in the Kaluza-Klein (KK) decomposed theory and show the consistency in both pictures analytically and numerically, which presents a non-trivial cross-check. In Feynman-’t Hooft gauge, the dominant corrections from virtual KK modes arise from the scalar parts of the W ±-boson penguin diagrams, including the contributions from the scalar component of the 5D gauge-boson field and from the charged Goldstone bosons in the Higgs sector. The size of the KK corrections depends on the parameter y*, which sets the upper bound for the anarchic 5D Yukawa matrices. We find that for y* ≳ 1 the KK corrections are proportional to y∗2. We discuss the phenomenological implications of our results for the branching ratio BrB¯→Xsγ$$ \mathrm{B}\mathrm{r}\left(\overline{B}\to {X}_s\gamma \right) $$, the time-dependent CP asymmetry SK ∗ γ, the direct CP asymmetry ACPb → sγand the CP asymmetry difference ΔACPb → sγ. We can derive a lower bound on the first KK gluon resonance of 3.8 TeV for y* = 3, requiring that at least 10% of the RS parameter space covers the experimental 2σ error margins. We further discuss the branching ratio BrB¯→Xsl+l−$$ \mathrm{B}\mathrm{r}\left(\overline{B}\to {X}_s{l}^{+}{l}^{-}\right) $$and compare our predictions for C7γ,9,10 and C˜7γ,9,10$$ {\tilde{C}}_{7\gamma, 9,10} $$with phenomenological results derived from model-independent analyses. | ||
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| 700 | 1 | |a Schmell, Christoph |d 1985- |e VerfasserIn |0 (DE-588)1063815886 |0 (DE-627)812623290 |0 (DE-576)423247808 |4 aut | |
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