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

More documents

Recommendations

Info

Bibliography 195[159] P. Benincasa, C. Boucher-Veronneau and F. Cachazo, Taming treeamplitudes in general relativity, JHEP 11 (2007) 057 [hep-th/0702032].[160] N. Arkani-Hamed and J. Kaplan, On Tree Amplitudes in Gauge Theory andGravity, JHEP 04 (2008) 076 [0801.2385].[161] Z. Bern, L. J. Dixon and D. A. Kosower, On-shell recurrence relations forone-loop QCD amplitudes, Phys. Rev. D71 (2005) 105013 [hep-th/0501240].[162] Z. Bern, L. J. Dixon and D. A. Kosower, The last of the finite loopamplitudes in QCD, Phys. Rev. D72 (2005) 125003 [hep-ph/0505055].[163] Z. Bern, L. J. Dixon and D. A. Kosower, Bootstrapping multi-parton loopamplitudes in QCD, Phys. Rev. D73 (2006) 065013 [hep-ph/0507005].[164] Z. Bern, N. E. J. Bjerrum-Bohr, D. C. Dunbar and H. Ita, Recursivecalculation of one-loop QCD integral coefficients, JHEP 11 (2005) 027[hep-ph/0507019].[165] C. F. Berger, Z. Bern, L. J. Dixon, D. Forde and D. A. Kosower, AllOne-loop Maximally Helicity Violating Gluonic Amplitudes in QCD, Phys.Rev. D75 (2007) 016006 [hep-ph/0607014].[166] Z. Bern, V. Del Duca, W. B. Kilgore and C. R. Schmidt, The infraredbehavior of one-loop QCD amplitudes at next-to-next-to-leading order, Phys.Rev. D60 (1999) 116001 [hep-ph/9903516].[167] Z. Bern, V. Del Duca and C. R. Schmidt, The infrared behavior of one-loopgluon amplitudes at next-to-next-to-leading order, Phys. Lett. B445 (1998)168–177 [hep-ph/9810409].[168] D. A. Kosower and P. Uwer, One-loop splitting amplitudes in gauge theory,Nucl. Phys. B563 (1999) 477–505 [hep-ph/9903515].[169] D. A. Kosower, All-order collinear behavior in gauge theories, Nucl. Phys.B552 (1999) 319–336 [hep-ph/9901201].
Bibliography 196[170] Z. Bern and A. G. Morgan, Massive Loop Amplitudes from Unitarity, Nucl.Phys. B467 (1996) 479–509 [hep-ph/9511336].[171] A. Brandhuber, S. McNamara, B. J. Spence and G. Travaglini, Loopamplitudes in pure Yang-Mills from generalised unitarity, JHEP 10 (2005)011 [hep-th/0506068].[172] S. D. Badger, Direct Extraction Of One Loop Rational Terms, JHEP 01(2009) 049 [0806.4600].[173] B. Feng and G. Yang, Unitarity Method with Spurious Pole, Nucl. Phys.B811 (2009) 305–352 [0806.4016].[174] A. Bredenstein, A. Denner, S. Dittmaier and S. Pozzorini, NLO QCDcorrections to top anti-top bottom anti-bottom production at the LHC: 1.quark-antiquark annihilation, JHEP 08 (2008) 108 [0807.1248].[175] A. Bredenstein, A. Denner, S. Dittmaier and S. Pozzorini, NLO QCDcorrections to pp → t anti-t b anti-b + X at the LHC, Phys. Rev. Lett. 103(2009) 012002 [0905.0110].[176] A. Bredenstein, A. Denner, S. Dittmaier and S. Pozzorini, NLO QCDcorrections to top anti-top bottom anti-bottom production at the LHC: 2. fullhadronic results, JHEP 03 (2010) 021 [1001.4006].[177] T. Binoth et. al., Next-to-leading order QCD corrections to pp → bbbb + X atthe LHC: the quark induced case, Phys. Lett. B685 (2010) 293–296[0910.4379].[178] C. F. Berger et. al., One-Loop Multi-Parton Amplitudes with a Vector Bosonfor the LHC, 0808.0941.[179] C. F. Berger et. al., Precise Predictions for W + 3 Jet Production at HadronColliders, Phys. Rev. Lett. 102 (2009) 222001 [0902.2760].
Page 7 and 8:
Contentsvii1.4.1 Effective Lagrangi
Page 9 and 10:
Contentsix4 One-loop Higgs plus fou
Page 11:
ContentsxiB.2 Box Integral Function
Page 18 and 19:
1.1. The Standard Model of Particle
Page 20:
Page 23 and 24:
Page 25 and 26:
Page 27 and 28:
1.2. Electroweak Symmetry Breaking
Page 29 and 30:
Page 31 and 32:
Page 33 and 34:
1.3. Higgs searches at colliders 18
Page 35 and 36:
Page 37 and 38:
Page 39 and 40:
1.4. Effective coupling between glu
Page 41 and 42:
1.4. Effective coupling between glu
Page 43 and 44:
1.5. Higgs plus two jets: Its pheno
Page 45 and 46:
1.5. Higgs plus two jets: Its pheno
Page 47 and 48:
2.1. Unitarity 32of two tree level
Page 49 and 50:
2.2. Quadruple cuts 34the rational
Page 51 and 52:
2.2. Quadruple cuts 360000000111111
Page 53 and 54:
2.2. Quadruple cuts 38We now must s
Page 55 and 56:
2.3. Forde’s Laurent expansion me
Page 57 and 58:
Page 59 and 60:
Page 61 and 62:
2.4. Spinor integration 46Here we h
Page 63 and 64:
2.4. Spinor integration 48The expli
Page 65 and 66:
2.4. Spinor integration 50with F z
Page 67 and 68:
2.5. MHV rules and BCFW recursion r
Page 69 and 70:
2.5. MHV rules and BCFW recursion r
Page 71 and 72:
2.6. The unitarity-bootstrap 56Next
Page 73 and 74:
2.6. The unitarity-bootstrap 58Figu
Page 75 and 76:
2.6. The unitarity-bootstrap 60of o
Page 77 and 78:
2.6. The unitarity-bootstrap 62rati
Page 79 and 80:
2.6. The unitarity-bootstrap 64Afte
Page 81 and 82:
2.8. Recent progress: One-loop auto
Page 83 and 84:
2.9. Summary 68cluding the recent c
Page 85 and 86:
3.2. The cut-constructible parts 70
Page 87 and 88:
eplacemen3.2. The cut-constructible
Page 89 and 90:
Page 91 and 92:
Page 93 and 94:
Page 95 and 96:
Page 97 and 98:
Page 99 and 100:
Page 101 and 102:
Page 103 and 104:
Page 105 and 106:
Page 107 and 108:
Page 109 and 110:
Page 111 and 112:
Page 113 and 114:
3.3. The rational pieces 98m−1∑
Page 115 and 116:
3.3. The rational pieces 100+m−1
Page 117 and 118:
3.3. The rational pieces 102+R(4 +
Page 119 and 120:
3.3. The rational pieces 104The cal
Page 121 and 122:
3.4. Cross Checks and Limits 1063.4
Page 123 and 124:
3.4. Cross Checks and Limits 108The
Page 125 and 126:
3.4. Cross Checks and Limits 110The
Page 127 and 128:
3.4. Cross Checks and Limits 112−
Page 129 and 130:
3.5. Summary 114The rational terms
Page 131 and 132:
Chapter 4One-loop Higgs plus four-g
Page 133 and 134:
4.2. Cut-Constructible Contribution
Page 135 and 136:
Page 137 and 138:
Page 139 and 140:
4.3. Rational Terms 124contains two
Page 141 and 142:
4.4. Higgs plus four gluon amplitud
Page 143 and 144:
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 and 196: B.2. Box Integral Functions 180L 2
Page 197 and 198: Bibliography 182[10] R. Feynman, Ma
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: Bibliography 194[148] R. Boels and
Page 213 and 214: Bibliography 198anti-t + 2 jets at
Page 215: Bibliography 200[214] C. Anastasiou
show all

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

Create successful ePaper yourself

Delete template?

Save as template?