1 Introduction - Caltech High Energy Physics - California Institute of ...

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12 Introduction Effective tagged sample 10000 9000 8000 7000 6000 5000 4000 3000 2000 1000 0 Jan-03 Jan-04 Jan-05 Jan-06 Jan-07 Jan-08 Jan-09 Jan-10 Jan-11 Years of data accumulation Figure 1-4. Projected time development for the size of the effective tagged sample (dashed red line) and the error on the amplitude for the sine coefficient (solid red line) for a fit to the time-dependent CP asymmetry in a B 0 → π + π − sample accumulated at a Super B Factory . Tagging efficiencies and per event errors are based on current BABAR analysis. Also shown are effective tagged samples and the error on the amplitude for the sine coefficient for LHCb (dashed blue curves) and BTeV (dotted purple curves), based on their simulations of tagging efficiencies and per event sensitivities. Figure 1-5. Projected time development for the size of the effective tagged sample ( --- )andthe correction to the effective value of alpha ( ——)as determined from a full isospin analysis of the two-body B decay modes for a Super B Factory. Tagging efficiencies and per event errors are based on current BABAR analysis. The Discovery Potential of a Super B Factory Jan-12 Jan-13 Jan-14 Jan-15 Jan-16 0.20 0.18 0.16 0.14 0.12 0.10 0.08 0.06 0.04 0.02 0.00 Error on sine amplitude
1.2 Measurement Capabilites of a Super B Factory 13 Figure 1-6. Projected time development for the size of the effective tagged sample ( --- )andthe error on the amplitude for the sine coefficient ( ——)from a fit to the time-dependent CP asymmetry in a B 0 → ρ + ρ − sample accumulated at Super B Factory. Tagging efficiencies and per event errors are based on current BABAR analysis. Figure 1-7. Projected time development for the size of the effective tagged sample ( --- )andthe error on the amplitude for the sine coefficient ( ——)from a fit to the time-dependent CP asymmetry in a B 0 → K 0 Sπ 0 γ sample accumulated at a Super B Factory. Tagging efficiencies and per event errors are based on current BABAR analysis. The Discovery Potential of a Super B Factory
Page 3 and 4: The Discovery Potential of a Super
Page 5 and 6: Contents 1 Introduction 1 1.1 Overv
Page 7 and 8: 2.17.2 Transversity amplitudes . .
Page 9 and 10: Combined Strategies for γ . . . .
Page 11 and 12: Semileptonic tags . . . . . . . . .
Page 13 and 14: Signals of New Physics . . . . . .
Page 15: 5.4.5 Warped Extra Dimensions Signa
Page 18 and 19: 2 Introduction Current plans call f
Page 20 and 21: 4 Introduction Several comments are
Page 22 and 23: 6 Introduction Table 1-1. Measureme
Page 24 and 25: 8 Introduction Table 1-4. Measureme
Page 26 and 27: 10 Introduction Measuring γ Table
Page 30 and 31: 14 Introduction 1.3 Conclusions As
Page 32 and 33: 16 REFERENCES The Discovery Potenti
Page 34 and 35: 18 Rare Decays 2.2 Present Status o
Page 36 and 37: 20 Rare Decays B → ℓνℓγ, th
Page 38 and 39: 22 Rare Decays corresponding to a p
Page 40 and 41: 24 Rare Decays worked out. Updated
Page 42 and 43: 26 Rare Decays the dilepton invaria
Page 44 and 45: 28 Rare Decays 2.3 Theoretical tool
Page 46 and 47: 30 Rare Decays to say that the resu
Page 48 and 49: 32 Rare Decays analysis of the stab
Page 50 and 51: 34 Rare Decays Table 2-3. Classific
Page 52 and 53: 36 Rare Decays 2.5 Prospects for In
Page 54 and 55: 38 Rare Decays however, that the co
Page 56 and 57: 40 Rare Decays events. Measurements
Page 58 and 59: 42 Rare Decays analyses [134, 51, 1
Page 60 and 61: 44 Rare Decays a substantial portio
Page 62 and 63: 46 Rare Decays As was analysed in [
Page 64 and 65: 48 Rare Decays Efficiency ± π 1 0
Page 66 and 67: 50 Rare Decays Total Error 0.1 0.08
Page 68 and 69: 52 Rare Decays Table 2-8. Theoretic
Page 70 and 71: 54 Rare Decays Η� Η� 1 0.8 0.
Page 72 and 73: 56 Rare Decays 2.10 Prospects for m
Page 74 and 75: 58 Rare Decays The hadronic paramet
Page 76 and 77: 60 Rare Decays 2.12 Double Radiativ
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62 Rare Decays 2.13 Experimental As
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64 Rare Decays AFB AFB FBAsym Nent
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66 Rare Decays if one aims at a num
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68 Rare Decays Most of the comments
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70 Rare Decays A FB 1 0.5 0 −0.5
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72 Rare Decays Figure 2-14. The Dal
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74 Rare Decays mK ∗ EK ∗ A0(q 2
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76 Rare Decays 2.16.2 Sensitivity t
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78 Rare Decays 2.16.3 Electron vers
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80 Rare Decays 2.17 Angular distrib
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82 Rare Decays Ð �Ð Ð � �
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84 Rare Decays Both asymmetries A (
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86 Rare Decays on ℓ = µ and assu
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88 Rare Decays 2.19 Experimental Pr
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90 Rare Decays 0.035 0.03 0.025 0.0
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92 Rare Decays • relatively good
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94 Rare Decays B(B → Xsνν) =(3.
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96 Rare Decays parametrizations wer
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98 Rare Decays 2.21 Purely Leptonic
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100 Rare Decays the scalar and pseu
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102 Rare Decays 2.22 Theoretical Pr
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104 Rare Decays spectrum starts to
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106 Rare Decays 2.23 B 0 → invisi
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108 Rare Decays Figure 2-33. From R
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110 Rare Decays data. Both this “
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112 Rare Decays 2.24.2 B → µµX
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114 Rare Decays 2.24.4 B → µµ T
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116 Rare Decays flavor-conserving o
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118 Rare Decays 2.26 Experimental P
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120 Rare Decays 2.27 Experimental A
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122 Rare Decays 2.28 Theoretical Pr
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124 Rare Decays and ˆs ≡ s/m 2 c
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126 Rare Decays Figure 2-39. The sa
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128 Rare Decays 2.28.2 Rare charm d
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130 Rare Decays [331] and B exp (D
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132 Rare Decays but the effects are
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134 Rare Decays • Rare radiative
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136 REFERENCES References [1] S. L.
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138 REFERENCES [59] Belle Collabora
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140 REFERENCES [117] G. P. Korchems
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142 REFERENCES [177] D. Melikhov an
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144 REFERENCES [234] See, for examp
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146 REFERENCES [288] A. Dedes, Mod.
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148 REFERENCES [346] BABAR Collabor
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150 REFERENCES The Discovery Potent
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152 Angles of the Unitarity Triangl
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244 REFERENCES [27] M. Grothe, Mod.
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246 REFERENCES [84] A. F. Falk et a
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248 REFERENCES [139] Belle Collabor
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250 REFERENCES [188] W. Bernreuther
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252 Semileptonic Decays and Sides o
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314 REFERENCES [25] N. Isgur, M. Wi
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316 REFERENCES [66] A. K. Leibovich
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318 REFERENCES [122] P. Ball and V.
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320 REFERENCES [182] A. I. Sanda an
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322 New Physics Physics and measure
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324 New Physics 5.2 Model-independe
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326 New Physics Rather promising, h
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328 New Physics For the Standard Mo
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330 New Physics Figure 5-2. Results
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332 New Physics These new parameter
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338 New Physics Figure 5-10. Result
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340 New Physics O9 = e2 g 2 s sαγ
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342 New Physics the Standard Model
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344 New Physics For muons we identi
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346 New Physics � 10 5 0 -5 -10 -
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348 New Physics In all cases, the w
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350 New Physics The key point is th
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352 New Physics which allows us to
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354 New Physics Extremizing this ex
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356 New Physics 0.8 0.7 0.6 0.5 0.4
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358 New Physics 12 10 8 6 4 2 0 -2
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360 New Physics 1 0.8 0.6 0.4 0.2 0
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362 New Physics g bR (L) δ m sL (R
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364 New Physics • maximal-parity:
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366 New Physics SΦKs 1 0.75 0.5 0.
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368 New Physics b s s (s b) V-A (s
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370 New Physics could increase f⊥
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372 New Physics The ratio of transv
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374 New Physics where ψ is the cc
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376 New Physics Since, a(s)eiδa(s)
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378 New Physics b B 0 ~ b A d �
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380 New Physics Table 5-5. Measured
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382 New Physics One of the strategi
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384 New Physics Table 5-10. 99% CL
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386 New Physics This is simply the
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388 New Physics scale, the insertio
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390 New Physics In the first model,
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392 New Physics ∆m( B s ) / ∆m(
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394 New Physics Table 5-12. Pattern
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396 New Physics such cases. We shou
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398 New Physics where (m2 dL(R) ˜
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400 New Physics ×Ä �×Ä �
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402 New Physics Table 5-14. Bounds
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404 New Physics Figure 5-35. Allowe
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406 New Physics Conclusions We have
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408 New Physics CP violation from
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410 New Physics are basically affec
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412 New Physics remain close to the
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414 New Physics + 4 s2 C2 7(1 − s
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416 New Physics Quarks Leptons thic
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418 New Physics Yukawa matrices (ea
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420 New Physics The effects of the
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422 New Physics functions of 1/R fo
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424 New Physics normalized AFB 0.15
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426 New Physics In addition, the lo
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428 New Physics From Eq. (5.9) we c
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430 New Physics There will also be
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432 New Physics gauge KK modes to z
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434 New Physics 5.5 Lepton Flavor V
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436 New Physics observation of τ
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438 New Physics LFV τ decays in th
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440 New Physics over these processe
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442 New Physics � � Ï Applicat
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444 New Physics Table 5-22. Experim
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446 New Physics Table 5-23. Pattern
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448 REFERENCES [26] Belle Collabora
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450 REFERENCES [78] A. J. Buras et
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452 REFERENCES [131] M. Beneke et a
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454 REFERENCES [175] R. Harnik et a
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456 REFERENCES [227] J. L. Hewett,
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458 REFERENCES [272] H. Davoudiasl,
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460 REFERENCES [316] K. Tobe, J. D.
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462 REFERENCES The Discovery Potent
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464 Workshop Participants Stefan Ch
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466 Workshop Participants David Lei
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468 Workshop Participants Abner Sof
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