On the Flavor Problem in Strongly Coupled Theories - THEP Mainz

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188 Appendix C. Input Parameters Parameter Value ± Error Reference ηB 0.55 ± 0.01 [249] mBs 5.3661 GeV [245] fBs (245 ± 25) MeV [247] B bs 1 0.80 ± 0.08 [247] B bs 4 1.15 ± 0.13 [247] B bs 5 1.74 ± 0.19 [247] (mb + ms) (4.30 ± 0.08) GeV [247] 2β SM (0.0363 +0.0016 [160] s −0.0015 (∆ms/Γs)exp 26.3 ± 0.6 [250] Re (Γs 12 /M s 12 ) (−4.97 ± 0.94) · 10−3 [158] Im (Γs 12 /M s 12 ) (2.06 ± 0.57) · 10−5 [158] Table C.2: Parameters used in the Bs– ¯ Bs mixing observables. The given values for the B bs i parameters and the sums (mb +ms) are MS quantities normalized at the scale 4.2 GeV. Parameter Value ± Error Reference mK 497.6 MeV [245] fK 156.1 MeV [245] B sd 1 0.51 ± 0.02 [176, Table 2] B sd 4 1.04 ± 0.07 [176, Table 2] B sd 5 0.76 ± 09 [176, Table 2] (ms + md) (135 ± 18) MeV [247] φɛ (43.51 ± 0.05) ◦ [245] κɛ 0.92 ± 0.02 [173] (∆mK)exp 3.4833 · 10 −15 GeV [245] mt(mt) (163.8 � ± 1.3) � GeV [248] +0.07 mc(mc) 1.27 −0.11 GeV [245] Table C.3: Parameters used in the K– ¯ K mixing observables. The given values for the B sd i parameters and the sum (ms + md) correspond to the RI-MOM scheme taken at the scale 2 GeV .
Parameter Value ± Error Reference mBd 5.2795 GeV [245] fBd � (200 ± 20) MeV +0.024 1.472 [247] τBs −0.026 � ps [250] cA 0.96 ± 0.02 [169, 170] mµ 105.66 MeV [245] mτ 1.777 GeV [245] Table C.4: Parameters entering the predictions for the B → µ + µ − -meson decays. The relevant magic numbers for the renormalization group running of the Wilson coefficients in neutral meson mixing read [152] for K − ¯ K mixing ai = (0.29, 0.69, 0.79, 1.1, 0.14) b 11 i = (0.82, 0, 0, 0, 0), c 11 i = (0.016, 0, 0, 0, 0), b 44 i = (0, 0, 0, 4.4, 0), c 44 i = (0, 0, 0, 0.68, 0.0055), b 45 i = (0, 0, 0, 1.5, 0.17), c 45 i = (0, 0, 0, 0.35, 0.0062), b 54 i = (0, 0, 0, 0.18, 0), c 54 i = (0, 0, 0, 0.026, 0.016), b 55 i = (0, 0, 0, 0.061, 0.82), c 55 i = (0, 0, 0, 0.013, 0.018) . and Bs − ¯ Bs mixing ai = (0.286, 0.692, 0.787, 1.143, 0.143) b 11 i = (0.865, 0, 0, 0, 0), c 11 i = (0.017, 0, 0, 0, 0), b 44 i = (0, 0, 0, 2.87, 0), c 44 i = (0, 0, 0, 0.48, 0.005), b 45 i = (0, 0, 0, 0.961, 0.22), c 45 i = (0, 0, 0, 0.25, 0.006), b 54 i = (0, 0, 0, 0.09, 0), c 54 i = (0, 0, 0, 0.013, 0.016), b 55 i = (0, 0, 0, 0.029, 0.863), c 55 i = (0, 0, 0, 0.007, 0.019) . 189
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On the Flavor Problem in Strongly C
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UNIVERSITY OF MAINZ ABSTRACT THEORE
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Contents Acknowledgements vii Prefa
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Acknowledgements First and foremost
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x One of the most fascinating insig
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2 Chapter 1. Introduction: Problems
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10 Chapter 1. Introduction: Problem
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36 Chapter 2. The Randall Sundrum M
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92 Chapter 3. Solving the Flavor Pr
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100 Chapter 3. Solving the Flavor P
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Page 148 and 149: 138 Chapter 3. Solving the Flavor P
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Page 188 and 189: 178 Appendix A. Generating Paramete
Page 190 and 191: 180 Appendix A. Generating Paramete
Page 192 and 193: 182 Appendix B. Neutral Meson Mixin
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Page 197: C Input Parameters This appendix is
Page 202 and 203: 192 Appendix D. Higgs Potential for
Page 204 and 205: 194 Bibliography [13] S. Dimopoulos
Page 206 and 207: 196 Bibliography [43] G. Nordström
Page 208 and 209: 198 Bibliography [72] K. S. Babu,
Page 210 and 211: 200 Bibliography [104] R. Contino a
Page 212 and 213: 202 Bibliography [133] M. Baak, M.
Page 214 and 215: 204 Bibliography [160] J. Charles,
Page 216 and 217: 206 Bibliography [185] C. Csaki, G.
Page 218 and 219: 208 Bibliography [213] E. Thomson e
Page 220: 210 Bibliography [239] V. Ahrens, A
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On the Flavor Problem in Strongly Coupled Theories - THEP Mainz

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