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1 Heavy WIMP Effective Theory |
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1 | (12) |
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1 | (3) |
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1.2 Universal Heavy WIMP Limit |
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4 | (3) |
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1.3 Motivations for Heavy WIMP Effective Theory |
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7 | (2) |
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9 | (4) |
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2 Heavy-Particle Spacetime Symmetries and Building Blocks |
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13 | (36) |
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2.1 Finite Dimensional Representations of the Lorentz Algebra |
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16 | (2) |
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2.2 Effective Field Theory and the Little Group |
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18 | (6) |
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2.2.1 Little Group Formalism |
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18 | (2) |
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2.2.2 Field Transformation Law and Lorentz Invariance |
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20 | (2) |
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2.2.3 1/M Expansion and Lagrangian Constraints |
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22 | (2) |
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2.3 Reparametrization Invariance and Invariant Operators |
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24 | (6) |
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24 | (2) |
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2.3.2 Reparametrization Invariance |
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26 | (1) |
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2.3.3 Invariant Operator Method |
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26 | (1) |
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2.3.4 Solution for Γ(υ, iD) |
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27 | (3) |
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2.4 Higher-Spin and Self-conjugate Fields |
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30 | (3) |
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2.4.1 Higher Spin Representations |
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30 | (2) |
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2.4.2 Self-conjugate Parity and CPT |
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32 | (1) |
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2.5 NRQED Example: Lagrangian |
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33 | (2) |
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2.6 NRQED Example: Relativistic Invariance |
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35 | (3) |
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35 | (2) |
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2.6.2 Invariant Operators |
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37 | (1) |
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2.7 NRQED Example: One-Photon Matching |
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38 | (2) |
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2.8 NRQED Example: Photon and Four-Fermion Sectors |
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40 | (6) |
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2.8.1 Pure Photon Operators |
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40 | (1) |
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2.8.2 Four-Fermion Operators |
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41 | (2) |
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2.8.3 Field Redefinitions and Redundant Operators |
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43 | (2) |
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2.8.4 Relativistic Lepton |
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45 | (1) |
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46 | (3) |
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3 Effective Theory at the Weak-Scale |
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49 | (28) |
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50 | (7) |
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3.1.1 Standard Model Building Blocks |
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50 | (3) |
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3.1.2 Dark Matter Building Blocks |
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53 | (1) |
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53 | (2) |
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55 | (2) |
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3.2 Multiplets and Mixtures |
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57 | (12) |
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59 | (2) |
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3.2.2 Higher-Order Example: Pure Triplet Scalar |
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61 | (2) |
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63 | (4) |
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67 | (1) |
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3.2.5 Relativistic Example: Singlet-Doublet Mixture |
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68 | (1) |
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3.3 Onshell Renormalization Scheme |
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69 | (6) |
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3.3.1 Singlet-Doublet Counterterm Lagrangian |
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69 | (1) |
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3.3.2 Propagator Corrections |
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70 | (2) |
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3.3.3 Renormalization Conditions |
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72 | (1) |
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3.3.4 Extension to Triplet-Doublet |
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73 | (2) |
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3.4 Low Energy Theory at the Weak Scale for Pure- and Mixed-State WIMPs |
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75 | (2) |
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77 | (42) |
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78 | (3) |
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4.1.1 Case I: M <~ mb <<: mw |
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78 | (2) |
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80 | (1) |
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81 | (1) |
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4.2 Multiplets and Mixtures |
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81 | (38) |
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4.2.1 Quark Matching: One-Boson Exchange |
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82 | (4) |
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4.2.2 Gluon Matching: One-Boson Exchange |
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86 | (1) |
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4.2.3 Quark Matching: Two-Boson Exchange |
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87 | (5) |
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4.2.4 Gluon Matching: Two-Boson Exchange |
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92 | (20) |
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4.2.5 Effective Theory Amplitudes and Infrared Regulator |
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112 | (1) |
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4.2.6 Extended Higgs Sector for Pure Case |
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113 | (1) |
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4.2.7 Bare Matching Coefficients |
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114 | (5) |
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5 QCD Analysis and Hadronic Matrix Elements |
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119 | (16) |
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5.1 Operator Renormalization |
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120 | (5) |
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5.1.1 Renormalization Constants |
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121 | (2) |
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5.1.2 Renormalized Matching Coefficients for Pure States |
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123 | (2) |
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5.2 Renormalization Group Evolution |
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125 | (2) |
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5.3 Threshold Matching and Low Energy Coefficients |
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127 | (3) |
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5.3.1 Heavy Quark Threshold Matching Conditions |
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128 | (1) |
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5.3.2 Low Energy Coefficients |
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129 | (1) |
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5.4 Hadronic Matrix Elements |
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130 | (5) |
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5.4.1 Scalar Matrix Elements |
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130 | (2) |
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5.4.2 Tensor Matrix Elements |
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132 | (3) |
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6 Heavy WIMP-Nucleon Scattering Cross Sections |
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135 | (12) |
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6.1 Cross Section Assembly Line |
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136 | (2) |
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6.2 Survey of Uncertainties |
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138 | (2) |
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6.3 Cross Section Predictions and Consistency Checks |
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140 | (7) |
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147 | (4) |
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Appendix A Solution to the Invariance Equation |
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151 | (6) |
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A.1 Series Solution for Γ |
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151 | (2) |
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A.2 Explicit Solution for Γ in the Spin 1/2 Theory |
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153 | (4) |
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Appendix B Integrals and Inputs for Weak Scale Matching |
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157 | (16) |
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B.1 Self Energy Integrals and Standard Model Two-Point Functions |
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157 | (4) |
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161 | (4) |
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B.3 Heavy Particle Integrals with Electroweak Polarization Tensor Insertion |
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165 | (5) |
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B.3.1 Case of Zero Heavy Fermions |
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166 | (1) |
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B.3.2 Case of One Heavy Fermion |
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167 | (3) |
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B.3.3 Case of Two Heavy Fermions |
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170 | (1) |
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170 | (3) |
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Appendix C Inputs for Analysis of QCD Effects and Hadronic Matrix Elements |
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173 | (2) |
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173 | (2) |
References |
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