Hadronic production of a Higgs boson in association with two jets at ...

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Bibliography[1] R. K. Ellis and S. Veseli, Strong radiative corrections to W b anti-bproduction in p anti-p collisions, Phys. Rev. D60 (1999) 011501[hep-ph/9810489].[2] J. M. Campbell and R. K. Ellis, An update on vector boson pair productionat hadron colliders, Phys. Rev. D60 (1999) 113006 [hep-ph/9905386].[3] J. M. Campbell and R. K. Ellis, Radiative corrections to Z b anti-bproduction, Phys. Rev. D62 (2000) 114012 [hep-ph/0006304].[4] J. M. Campbell, R. K. Ellis and F. Tramontano, Single top production anddecay at next-to-leading order, Phys. Rev. D70 (2004) 094012[hep-ph/0408158].[5] J. M. Campbell, R. K. Ellis, F. Maltoni and S. Willenbrock, Production of aZ boson and two jets with one heavy- quark tag, Phys. Rev. D73 (2006)054007 [hep-ph/0510362].[6] M. Peskin and D. Schroeder, An Introduction to Quantum Field Theory,Westview Press (1995).[7] R. K. Ellis, W. J. Stirling and B. R. Webber, QCD and Collider Physics,Cambridge University Press (1996).[8] R. Feynman, Space-time approach to quantum electrodynamics, Phys. Rev 76(1949) 769.[9] R. Feynman, The theory of positrons, Phys. Rev 76 (1949) 749.181
Bibliography 182[10] R. Feynman, Mathematical formulation of the quantum theory ofelectromagnetic interaction, Phys. Rev 80 (1950) 440.[11] S. Tomonaga, On a relativistically invariant formulation of the quantumtheory of wave fields, Progress of Theoretical Physics 1 (1946) 27.[12] J. Schwinger, On quantum-electrodynamics and the magnetic moment of theelectron, Phys. Rev. 73 (1948) 416.[13] J. Schwinger, Quantum-electrodynamics 1. a covariant formulation, Phys.Rev. 74 (1948) 1439.[14] C. Yang and R. Mills Phys. Rev. 96 (1954) 191.[15] S. Bethke, in Proc. QCD94 Conference, Montpellier, July 1984 , Nucl. Phys.B (Proc. Suppl.) 39BC (1995) 198.[16] G. Passarino and M. Veltman, , Nucl. Phys. B B160 (1979) 151.[17] G. ’t Hooft and M. Veltman Nucl. Phys. B44 (1972) 189.[18] F. Bloch and A. Nordsieck, Note on the radiation field of the electron, Phys.Rev 52 (1937) 54–59.[19] T. Kinoshita, Mass singularities of Feynmann amplitudes, J. Math. Phys 3(1962) 650–677.[20] T. D. Lee and M. Nauenberg, Degenerate systems and mass singularities,Phys. Rev. 133 (1964) B1549–B1562.[21] R. K. Ellis, H. Georgi, M. Machacek, H. D. Politzer and G. G. Ross,Perturbation Theory and the Parton Model in QCD, Nucl. Phys. B152(1979) 285.[22] A. D. Martin, W. J. Stirling, R. S. Thorne and G. Watt, Parton distributionsfor the LHC, Eur. Phys. J. C63 (2009) 189–285 [0901.0002].[23] P. M. Nadolsky et. al., Implications of CTEQ global analysis for colliderobservables, Phys. Rev. D78 (2008) 013004 [0802.0007].
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Contentsvii1.4.1 Effective Lagrangi
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Contentsix4 One-loop Higgs plus fou
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ContentsxiB.2 Box Integral Function
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1.1. The Standard Model of Particle
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1.2. Electroweak Symmetry Breaking
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1.3. Higgs searches at colliders 18
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1.4. Effective coupling between glu
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1.4. Effective coupling between glu
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1.5. Higgs plus two jets: Its pheno
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1.5. Higgs plus two jets: Its pheno
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2.1. Unitarity 32of two tree level
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2.2. Quadruple cuts 34the rational
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2.2. Quadruple cuts 360000000111111
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2.2. Quadruple cuts 38We now must s
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2.3. Forde’s Laurent expansion me
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2.4. Spinor integration 46Here we h
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2.4. Spinor integration 48The expli
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2.4. Spinor integration 50with F z
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2.5. MHV rules and BCFW recursion r
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2.5. MHV rules and BCFW recursion r
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2.6. The unitarity-bootstrap 56Next
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2.6. The unitarity-bootstrap 58Figu
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2.6. The unitarity-bootstrap 60of o
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2.6. The unitarity-bootstrap 62rati
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2.6. The unitarity-bootstrap 64Afte
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2.8. Recent progress: One-loop auto
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2.9. Summary 68cluding the recent c
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3.2. The cut-constructible parts 70
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eplacemen3.2. The cut-constructible
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3.3. The rational pieces 98m−1∑
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3.3. The rational pieces 100+m−1
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3.3. The rational pieces 102+R(4 +
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3.3. The rational pieces 104The cal
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3.4. Cross Checks and Limits 1063.4
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3.4. Cross Checks and Limits 108The
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3.4. Cross Checks and Limits 110The
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3.4. Cross Checks and Limits 112−
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3.5. Summary 114The rational terms
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Chapter 4One-loop Higgs plus four-g
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4.2. Cut-Constructible Contribution
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4.3. Rational Terms 124contains two
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4.4. Higgs plus four gluon amplitud
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4.4. Higgs plus four gluon amplitud
Page 145 and 146: 4.6. Summary 130p µ 2 = (+0.344450
Page 147 and 148: Chapter 5The φqqgg- NMHV amplitude
Page 149 and 150: 5.1. Introduction 134Figure 5.1: Sa
Page 151 and 152: 5.1. Introduction 136H amplitude φ
Page 153 and 154: 5.2. One-loop results 138A L 4 (φ,
Page 155 and 156: 5.2. One-loop results 140with K 1 =
Page 157 and 158: 5.2. One-loop results 142Relation f
Page 159 and 160: 5.2. One-loop results 144+ 1s 123[
Page 161 and 162: 5.4. Summary 146(φ, 1 −¯q , 2 +
Page 163 and 164: 6.2. Improvements from the semi-num
Page 165 and 166: 6.4. Tevatron results 150The W mass
Page 167 and 168: 6.4. Tevatron results 152m H [GeV]
Page 169 and 170: 6.5. LHC results 154Eq. (6.11) and
Page 171 and 172: 6.5. LHC results 156m H [GeV] 120 1
Page 173 and 174: 6.5. LHC results 158Figure 6.3: The
Page 175 and 176: 6.5. LHC results 160of describing T
Page 177 and 178: 6.5. LHC results 162Figure 6.6: p T
Page 179 and 180: 6.6. Summary 164at LO and the effec
Page 181 and 182: 6.6. Summary 166of Higgs masses, 15
Page 183 and 184: Chapter 7. Conclusions 168one can d
Page 185 and 186: Appendix ASpinor Helicity Formalism
Page 187 and 188: A.1. Spinor Helicity Formalism nota
Page 189 and 190: A.3. Pure QCD amplitudes 174Further
Page 191 and 192: Appendix BOne-loop Basis IntegralsI
Page 193 and 194: B.2. Box Integral Functions 178boxe
Page 195: B.2. Box Integral Functions 180L 2
Page 199 and 200: Bibliography 184[36] M. Bahr et. al
Page 201 and 202: Bibliography 186[63] M. Shifman, A.
Page 203 and 204: Bibliography 188[85] R. V. Harlande
Page 205 and 206: Bibliography 190[104] R. K. Ellis,
Page 207 and 208: Bibliography 192[125] G. Ossola, C.
Page 209 and 210: Bibliography 194[148] R. Boels and
Page 211 and 212: Bibliography 196[170] Z. Bern and A
Page 213 and 214: Bibliography 198anti-t + 2 jets at
Page 215: Bibliography 200[214] C. Anastasiou
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