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

More documents

Recommendations

Info

3.2. The cut-constructible parts 73++−−+−++−−++−+−−+−−+ − +− +(a) (b) (c)+−−+−+−−−−−+++++−+−+(d) (e) (f)Figure 3.2: As in the four-mass case three-mass boxes do not contribute to φ-MHVamplitudes. External particles are either; positive helicity gluons (solid black lines)of which there can be an arbitrary number at any vertex, negative helicity gluons(shown in green) of which there can be only two and one φ (dashed black line). Ineach configuration (a) − (f) we find that whichever way we distribute the helicitieswe have at least one zero tree-level amplitude (highlighted by the red boxes).
3.2. The cut-constructible parts 74++−+−−+−−−++−++−(a) (b) (c)−+−+−+++−++−−− + −−− +− +− +(d) (e) (f)+−−+−−−+ − +−++++−+(g) (h) (i)Figure 3.3: As in the four- and three-mass cases two-mass hard boxes do not contributeto φ-MHV amplitudes. Here for simplicity we suppress helicities which areunfixed (i.e. ±, ∓). A new feature for the two-mass boxes which does not happenfor three- and four-mass is the zeroing of diagrams with two adjacent MHV (MHV)three point amplitudes. These are highlighted by the blue boxes.
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:
1.3. Higgs searches at colliders 20
Page 37 and 38: 1.3. Higgs searches at colliders 22
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 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: eplacemen3.2. The cut-constructible
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 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 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
show all

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

You also want an ePaper? Increase the reach of your titles

Delete template?

Save as template?