SM Higgs production cross sections at √s = 8 TeV (update in CERN Report4 2016)
- Cross sections reported in CERN Report 4. See here and here here for previous numbers in CERN Report 3.
- Higgs cross sections and BRs in Spread sheet are available in xlsx format
- You can find figures at our gallery here.
Mass range and step for SM-like Higgs boson:
- Total 38 points for MH=[120,130] GeV.
gluon-gluon Fusion Process
N3LO QCD cross sections supercede those of NNLO+NNLL QCD
N3LO
- Cross sections are calculated by Zürich group at N3LO QCD and NLO EW accuracies [Anastasiou:2016cez].
- QCD scales: μ=μF=μR=MH/2 varied in the range of [MH/4,MH].
- Theory uncertainty:
- "±Theory" uncertainty is interpreted as a flat 100% confidence level.
- "TH Gaussian" uncertainty is interpreted as a one-sigma range. It is estimated by max{+TH,-TH}/sqrt{3} as discussed in CERN Report 4 ggF section.
- "TH Gaussian" uncertainty should be used for the construction of the workspace in the current LHC-HCG prescription
.
- PDF set: PDF4LHC15_nnlo_100
NNLO+NNLL
- Cross sections are calculated with dFG program at NNLO+NNLL QCD and NLO EW accuracies.
- Calculations are the same as CERN Report 3 (i.e. top, bottom and charm quark effects are taken into account), except it is in NWA (CPS in CERN Report 3).
- Program: dFG
- QCD scales: μ=μF=μR=MH, uncertainty estimated in the range 1/2 < μ/MH < 2 with 1/2 < μF/μR < 2 constraint.
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nnlo_30
| |
N3LO |
|
NNLO+NNLL |
| mH (GeV) |
Cross Section (pb) |
+Theory % |
-Theory % |
TH Gaussian % |
±(PDF+αs) % |
±PDF % |
±αs % |
|
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
| 120.00 |
2.322E+01 |
+4.5 |
-7.1 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
2.107E+01 |
+7.5 |
-8.1 |
±3.2 |
±1.8 |
±2.6 |
| 120.50 |
2.303E+01 |
+4.5 |
-7.0 |
±4.1 |
±3.2 |
±1.9 |
±2.7 |
|
2.090E+01 |
+7.5 |
-8.1 |
±3.2 |
±1.8 |
±2.6 |
| 121.00 |
2.285E+01 |
+4.5 |
-7.0 |
±4.1 |
±3.2 |
±1.9 |
±2.7 |
|
2.073E+01 |
+7.4 |
-8.1 |
±3.2 |
±1.8 |
±2.6 |
| 121.50 |
2.266E+01 |
+4.5 |
-7.0 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
2.057E+01 |
+7.4 |
-8.1 |
±3.2 |
±1.8 |
±2.6 |
| 122.00 |
2.248E+01 |
+4.5 |
-7.0 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
2.041E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 122.50 |
2.230E+01 |
+4.5 |
-7.0 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
2.024E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 123.00 |
2.212E+01 |
+4.5 |
-7.0 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
2.009E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 123.50 |
2.194E+01 |
+4.5 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.993E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.00 |
2.177E+01 |
+4.5 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.977E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.10 |
2.173E+01 |
+4.5 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.974E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.20 |
2.170E+01 |
+4.5 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.971E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.30 |
2.166E+01 |
+4.5 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.968E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.40 |
2.163E+01 |
+4.5 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.965E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.50 |
2.159E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.962E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.60 |
2.156E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.959E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.70 |
2.153E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.956E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.80 |
2.149E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.953E+01 |
+7.4 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 124.90 |
2.146E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.950E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.00 |
2.142E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.947E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.09 |
2.139E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.944E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.10 |
2.139E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.944E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.20 |
2.136E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.941E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.30 |
2.132E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.938E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.40 |
2.129E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.935E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.50 |
2.126E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.932E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.60 |
2.122E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.929E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.70 |
2.119E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.926E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.80 |
2.116E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.923E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 125.90 |
2.112E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.920E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 126.00 |
2.109E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.917E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 126.50 |
2.092E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
1.902E+01 |
+7.3 |
-8.0 |
±3.1 |
±1.8 |
±2.6 |
| 127.00 |
2.076E+01 |
+4.4 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.887E+01 |
+7.3 |
-7.9 |
±3.1 |
±1.8 |
±2.6 |
| 127.50 |
2.060E+01 |
+4.4 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.873E+01 |
+7.3 |
-7.9 |
±3.1 |
±1.8 |
±2.6 |
| 128.00 |
2.044E+01 |
+4.4 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.859E+01 |
+7.3 |
-7.9 |
±3.1 |
±1.8 |
±2.6 |
| 128.50 |
2.028E+01 |
+4.4 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.845E+01 |
+7.3 |
-7.9 |
±3.1 |
±1.8 |
±2.5 |
| 129.00 |
2.013E+01 |
+4.4 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.831E+01 |
+7.3 |
-7.9 |
±3.1 |
±1.8 |
±2.5 |
| 129.50 |
1.998E+01 |
+4.4 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.817E+01 |
+7.2 |
-7.9 |
±3.1 |
±1.8 |
±2.5 |
| 130.00 |
1.982E+01 |
+4.3 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
1.803E+01 |
+7.2 |
-7.9 |
±3.1 |
±1.8 |
±2.5 |
VBF Process
- Cross sections are calculated at (approx.) NNLO QCD and NLO EW accuracies.
- Calculations are the same as CERN Report 3, except it is in NWA (CPS in CERN Report 3).
- Program: NNLO QCD (VBF@NNLO) and NLO EW (HAWK).
- QCD scales: μ=μF=μR=MW, uncertainty estimated in the range 1/2 < μ/MW < 2 (keeping μF=μR).
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nnlo_100 (QCD corrections) and NNPDF2.3QED (EW corrections + photon PDF)
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
| 120.00 |
1.676E+00 |
+0.3 |
-0.3 |
±2.2 |
±2.1 |
±0.4 |
| 120.50 |
1.668E+00 |
+0.3 |
-0.3 |
±2.2 |
±2.1 |
±0.4 |
| 121.00 |
1.661E+00 |
+0.3 |
-0.3 |
±2.2 |
±2.1 |
±0.4 |
| 121.50 |
1.653E+00 |
+0.3 |
-0.3 |
±2.2 |
±2.1 |
±0.4 |
| 122.00 |
1.645E+00 |
+0.3 |
-0.3 |
±2.2 |
±2.1 |
±0.4 |
| 122.50 |
1.638E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 123.00 |
1.631E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 123.50 |
1.623E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.00 |
1.616E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.10 |
1.614E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.20 |
1.613E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.30 |
1.611E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.40 |
1.610E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.50 |
1.609E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.60 |
1.607E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.70 |
1.606E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.80 |
1.604E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.90 |
1.603E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.00 |
1.601E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.09 |
1.600E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.10 |
1.600E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.20 |
1.598E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.30 |
1.597E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.40 |
1.596E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.50 |
1.594E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.60 |
1.593E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.70 |
1.591E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.80 |
1.590E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.90 |
1.588E+00 |
+0.3 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 126.00 |
1.587E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 126.50 |
1.580E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 127.00 |
1.573E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 127.50 |
1.566E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 128.00 |
1.559E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 128.50 |
1.552E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 129.00 |
1.545E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 129.50 |
1.538E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 130.00 |
1.531E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
WH Process
- Cross sections are calculated at NNLO QCD and NLO EW accuracies.
- Calculations are the same as CERN Report 3, except photon-induced contribution (see below).
- Total cross section is calculated from WH→lνH cross section by subtracting photon-induced cross section, and then scaled via BR(W→lν)=0.108535 in NLO EW accuracy.
- Program: NNLO QCD (VH@NNLO) and NLO EW (HAWK).
- QCD scales: μ=μF=μR=MVH=(pV+pH)2 for QCD part and μ=μF=μR=MVH+MH for EW part. Uncertainty is estimated in the range 1/3 < μ/MVH < 3 (μF and μR are varied independently).
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nnlo_mc (QCD part) and NNPDF2.3QED (EW part).
- Photon-induced contribution of O(5%)
- NOT included for total cross section (agrees with CERN Report 3 numbers within 1%).
- Included in cross sections for dedicated WH→lνH (l=e,μ or τ) process (we strongly recommend to use these numbers for dedicated analyses).
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
W+H (pb) |
W-H (pb) |
| 120.00 |
8.054E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
5.091E-01 |
2.963E-01 |
| 120.50 |
7.943E-01 |
+0.5 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
5.023E-01 |
2.920E-01 |
| 121.00 |
7.832E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.953E-01 |
2.878E-01 |
| 121.50 |
7.724E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.887E-01 |
2.837E-01 |
| 122.00 |
7.620E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.821E-01 |
2.799E-01 |
| 122.50 |
7.518E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.758E-01 |
2.760E-01 |
| 123.00 |
7.414E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.694E-01 |
2.720E-01 |
| 123.50 |
7.314E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.632E-01 |
2.682E-01 |
| 124.00 |
7.218E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.570E-01 |
2.648E-01 |
| 124.10 |
7.198E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.559E-01 |
2.639E-01 |
| 124.20 |
7.180E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.548E-01 |
2.632E-01 |
| 124.30 |
7.163E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.537E-01 |
2.626E-01 |
| 124.40 |
7.146E-01 |
+0.5 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.528E-01 |
2.619E-01 |
| 124.50 |
7.124E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.514E-01 |
2.610E-01 |
| 124.60 |
7.104E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.500E-01 |
2.604E-01 |
| 124.70 |
7.082E-01 |
+0.7 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.486E-01 |
2.595E-01 |
| 124.80 |
7.065E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.477E-01 |
2.588E-01 |
| 124.90 |
7.046E-01 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
4.466E-01 |
2.580E-01 |
| 125.00 |
7.026E-01 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
4.454E-01 |
2.572E-01 |
| 125.09 |
7.009E-01 |
+0.7 |
-0.8 |
±2.0 |
±1.9 |
±0.7 |
4.443E-01 |
2.566E-01 |
| 125.10 |
7.009E-01 |
+0.6 |
-0.8 |
±2.0 |
±1.9 |
±0.7 |
4.443E-01 |
2.566E-01 |
| 125.20 |
6.989E-01 |
+0.7 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.429E-01 |
2.560E-01 |
| 125.30 |
6.969E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.416E-01 |
2.553E-01 |
| 125.40 |
6.950E-01 |
+0.7 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.404E-01 |
2.546E-01 |
| 125.50 |
6.930E-01 |
+0.7 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.391E-01 |
2.538E-01 |
| 125.60 |
6.912E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.381E-01 |
2.531E-01 |
| 125.70 |
6.895E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.371E-01 |
2.525E-01 |
| 125.80 |
6.875E-01 |
+0.7 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.358E-01 |
2.517E-01 |
| 125.90 |
6.859E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.348E-01 |
2.511E-01 |
| 126.00 |
6.840E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.336E-01 |
2.504E-01 |
| 126.50 |
6.749E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.277E-01 |
2.472E-01 |
| 127.00 |
6.660E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.223E-01 |
2.437E-01 |
| 127.50 |
6.572E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.167E-01 |
2.405E-01 |
| 128.00 |
6.488E-01 |
+0.6 |
-0.8 |
±2.1 |
±1.9 |
±0.7 |
4.116E-01 |
2.373E-01 |
| 128.50 |
6.402E-01 |
+0.6 |
-0.9 |
±2.1 |
±1.9 |
±0.7 |
4.063E-01 |
2.338E-01 |
| 129.00 |
6.319E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
4.010E-01 |
2.309E-01 |
| 129.50 |
6.236E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.959E-01 |
2.277E-01 |
| 130.00 |
6.154E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.908E-01 |
2.245E-01 |
WH→lνH (l=e,μ or τ) Process
| |
W+H→l+νH |
W-H→l-νH |
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
σγ |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
σγ |
| 120.00 |
5.646E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.21E-03 |
3.288E-02 |
+0.5 |
-0.9 |
±2.2 |
±2.1 |
±0.6 |
7.20E-04 |
| 120.50 |
5.573E-02 |
+0.5 |
-0.9 |
±2.0 |
±1.8 |
±0.7 |
1.21E-03 |
3.241E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.20E-04 |
| 121.00 |
5.497E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.21E-03 |
3.196E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.20E-04 |
| 121.50 |
5.424E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.20E-03 |
3.151E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.20E-04 |
| 122.00 |
5.352E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.20E-03 |
3.109E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.10E-04 |
| 122.50 |
5.284E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.20E-03 |
3.067E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.10E-04 |
| 123.00 |
5.214E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.19E-03 |
3.023E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.10E-04 |
| 123.50 |
5.146E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.19E-03 |
2.981E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.00 |
5.079E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
1.19E-03 |
2.944E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.10 |
5.067E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
1.19E-03 |
2.934E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.20 |
5.054E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.927E-02 |
+0.5 |
-0.9 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.30 |
5.042E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.920E-02 |
+0.5 |
-0.9 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.40 |
5.032E-02 |
+0.5 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.912E-02 |
+0.5 |
-0.9 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.50 |
5.017E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.903E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.60 |
5.002E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.896E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.70 |
4.987E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.887E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.80 |
4.977E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.879E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 124.90 |
4.965E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.870E-02 |
+0.6 |
-0.8 |
±2.1 |
±2.1 |
±0.6 |
7.00E-04 |
| 125.00 |
4.952E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.862E-02 |
+0.6 |
-0.8 |
±2.1 |
±2.1 |
±0.6 |
7.00E-04 |
| 125.09 |
4.940E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.855E-02 |
+0.6 |
-0.7 |
±2.1 |
±2.1 |
±0.6 |
7.00E-04 |
| 125.10 |
4.940E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.855E-02 |
+0.6 |
-0.7 |
±2.1 |
±2.1 |
±0.6 |
7.00E-04 |
| 125.20 |
4.925E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.848E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 125.30 |
4.911E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.841E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
7.00E-04 |
| 125.40 |
4.898E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.832E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 125.50 |
4.884E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.824E-02 |
+0.6 |
-0.7 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 125.60 |
4.873E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
1.18E-03 |
2.816E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 125.70 |
4.861E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.7 |
1.17E-03 |
2.809E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 125.80 |
4.847E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.17E-03 |
2.801E-02 |
+0.6 |
-0.7 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 125.90 |
4.836E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.7 |
1.17E-03 |
2.794E-02 |
+0.6 |
-0.7 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 126.00 |
4.823E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.7 |
1.17E-03 |
2.787E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 126.50 |
4.759E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.17E-03 |
2.752E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 127.00 |
4.700E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.7 |
1.17E-03 |
2.714E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 127.50 |
4.639E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.16E-03 |
2.679E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.90E-04 |
| 128.00 |
4.583E-02 |
+0.6 |
-0.8 |
±2.0 |
±1.8 |
±0.7 |
1.16E-03 |
2.643E-02 |
+0.6 |
-0.9 |
±2.2 |
±2.1 |
±0.6 |
6.80E-04 |
| 128.50 |
4.526E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.8 |
±0.7 |
1.16E-03 |
2.606E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.80E-04 |
| 129.00 |
4.467E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
1.15E-03 |
2.574E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.80E-04 |
| 129.50 |
4.412E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
1.15E-03 |
2.539E-02 |
+0.5 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.80E-04 |
| 130.00 |
4.357E-02 |
+0.6 |
-1.0 |
±2.0 |
±1.9 |
±0.7 |
1.15E-03 |
2.505E-02 |
+0.6 |
-0.8 |
±2.2 |
±2.1 |
±0.6 |
6.80E-04 |
ZH Process
- Cross sections are calculated at NNLO QCD and NLO EW accuracies.
- Calculations are the same as CERN Report 3, except photon-induced contribution (see below).
- Total cross section is calculated from ZH→llH,ννH cross sections by subtracting photon-induced cross section, and then scaled via BR(Z→ll)=0.0335962 and BR(Z→νν)=0.201030 in NLO EW accuracy.
- gg→ZH (box-diagram) occurs as a part of NNLO QCD correction and included in the total cross section.
- ZH cross section went up by +1~2%, due to +22~16% for √s = 7-14 TeV, due to increase in gg→ZH for NLO+NLL QCD corrections (NLO in CERN Report 3).
- Program: NNLO QCD (VH@NNLO) and NLO EW (HAWK).
- QCD scales: μ=μF=μR=MVH=(pV+pH)2 for QCD part and μ=μF=μR=MVH+MH for EW part. Uncertainty is estimated in the range 1/3 < μ/MVH < 3 (μF and μR are varied independently).
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nnlo_mc (QCD part) and NNPDF2.3QED (EW part).
- Photon-induced contribution of O(1%) or below
- NOT included for total cross section (agrees with CERN Report 3 numbers).
- Included in cross sections for dedicated ZH→llH,ννH (l=e,μ or τ) processes (we strongly recommend to use these numbers for dedicated analyses).
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
σ(gg→ZH) (pb) |
| 120.00 |
4.767E-01 |
+2.6 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
4.175E-02 |
| 120.50 |
4.705E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
4.148E-02 |
| 121.00 |
4.648E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
4.123E-02 |
| 121.50 |
4.591E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
4.096E-02 |
| 122.00 |
4.534E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
4.086E-02 |
| 122.50 |
4.479E-01 |
+2.7 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
4.059E-02 |
| 123.00 |
4.421E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
4.031E-02 |
| 123.50 |
4.366E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
4.004E-02 |
| 124.00 |
4.314E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.994E-02 |
| 124.10 |
4.303E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.977E-02 |
| 124.20 |
4.292E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.974E-02 |
| 124.30 |
4.282E-01 |
+2.7 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.974E-02 |
| 124.40 |
4.273E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.969E-02 |
| 124.50 |
4.261E-01 |
+2.7 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.967E-02 |
| 124.60 |
4.250E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.964E-02 |
| 124.70 |
4.238E-01 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.947E-02 |
| 124.80 |
4.228E-01 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.944E-02 |
| 124.90 |
4.217E-01 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.942E-02 |
| 125.00 |
4.208E-01 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.942E-02 |
| 125.09 |
4.199E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.942E-02 |
| 125.10 |
4.199E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.942E-02 |
| 125.20 |
4.187E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.937E-02 |
| 125.30 |
4.176E-01 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.934E-02 |
| 125.40 |
4.166E-01 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
3.917E-02 |
| 125.50 |
4.157E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.914E-02 |
| 125.60 |
4.148E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
3.914E-02 |
| 125.70 |
4.136E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
3.912E-02 |
| 125.80 |
4.128E-01 |
+2.7 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.909E-02 |
| 125.90 |
4.119E-01 |
+2.8 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.909E-02 |
| 126.00 |
4.107E-01 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
3.905E-02 |
| 126.50 |
4.056E-01 |
+2.9 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
3.877E-02 |
| 127.00 |
4.008E-01 |
+2.9 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
3.852E-02 |
| 127.50 |
3.961E-01 |
+2.8 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.828E-02 |
| 128.00 |
3.914E-01 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.818E-02 |
| 128.50 |
3.863E-01 |
+3.0 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
3.788E-02 |
| 129.00 |
3.818E-01 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.765E-02 |
| 129.50 |
3.773E-01 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.738E-02 |
| 130.00 |
3.726E-01 |
+3.0 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
3.708E-02 |
ZH→llH, ννH (l=e,μ or τ) Process
| |
ZH→l+l-H |
ZH→ννH |
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
gg→ZH (pb) |
σγ |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
gg→ZH (pb) |
σγ |
| 120.00 |
1.606E-02 |
+2.6 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.41E-03 |
4.00E-05 |
9.581E-02 |
+2.6 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
8.35E-03 |
0.00E+00 |
| 120.50 |
1.585E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
1.40E-03 |
4.00E-05 |
9.456E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
8.30E-03 |
0.00E+00 |
| 121.00 |
1.566E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
1.39E-03 |
4.00E-05 |
9.341E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
8.26E-03 |
0.00E+00 |
| 121.50 |
1.547E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
1.38E-03 |
4.00E-05 |
9.227E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.5 |
±0.8 |
8.21E-03 |
0.00E+00 |
| 122.00 |
1.528E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.38E-03 |
4.00E-05 |
9.112E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
8.17E-03 |
0.00E+00 |
| 122.50 |
1.509E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.37E-03 |
4.00E-05 |
9.001E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
8.12E-03 |
0.00E+00 |
| 123.00 |
1.490E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.36E-03 |
4.00E-05 |
8.885E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
8.07E-03 |
0.00E+00 |
| 123.50 |
1.471E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.35E-03 |
4.00E-05 |
8.774E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
8.02E-03 |
0.00E+00 |
| 124.00 |
1.454E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.35E-03 |
4.00E-05 |
8.669E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.98E-03 |
0.00E+00 |
| 124.10 |
1.450E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.34E-03 |
4.00E-05 |
8.647E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.97E-03 |
0.00E+00 |
| 124.20 |
1.446E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.34E-03 |
4.00E-05 |
8.627E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.96E-03 |
0.00E+00 |
| 124.30 |
1.443E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.34E-03 |
4.00E-05 |
8.607E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.96E-03 |
0.00E+00 |
| 124.40 |
1.440E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.34E-03 |
4.00E-05 |
8.587E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.94E-03 |
0.00E+00 |
| 124.50 |
1.436E-02 |
+2.7 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.34E-03 |
4.00E-05 |
8.565E-02 |
+2.7 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.93E-03 |
0.00E+00 |
| 124.60 |
1.432E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.34E-03 |
4.00E-05 |
8.542E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.92E-03 |
0.00E+00 |
| 124.70 |
1.428E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.519E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.91E-03 |
0.00E+00 |
| 124.80 |
1.425E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.497E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.90E-03 |
0.00E+00 |
| 124.90 |
1.421E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.476E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.89E-03 |
0.00E+00 |
| 125.00 |
1.418E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.456E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.89E-03 |
0.00E+00 |
| 125.09 |
1.415E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.440E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.89E-03 |
0.00E+00 |
| 125.10 |
1.415E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.440E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.89E-03 |
0.00E+00 |
| 125.20 |
1.411E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.416E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.87E-03 |
0.00E+00 |
| 125.30 |
1.407E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.33E-03 |
4.00E-05 |
8.394E-02 |
+2.9 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.86E-03 |
0.00E+00 |
| 125.40 |
1.404E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
1.32E-03 |
4.00E-05 |
8.373E-02 |
+2.8 |
-2.4 |
±1.7 |
±1.5 |
±0.8 |
7.85E-03 |
0.00E+00 |
| 125.50 |
1.401E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.32E-03 |
4.00E-05 |
8.356E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.84E-03 |
0.00E+00 |
| 125.60 |
1.398E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
1.32E-03 |
4.00E-05 |
8.336E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.8 |
7.84E-03 |
0.00E+00 |
| 125.70 |
1.394E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
1.32E-03 |
4.00E-05 |
8.313E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
7.83E-03 |
0.00E+00 |
| 125.80 |
1.391E-02 |
+2.7 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.32E-03 |
4.00E-05 |
8.298E-02 |
+2.7 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.82E-03 |
0.00E+00 |
| 125.90 |
1.388E-02 |
+2.8 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.32E-03 |
4.00E-05 |
8.279E-02 |
+2.8 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.82E-03 |
0.00E+00 |
| 126.00 |
1.384E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
1.32E-03 |
4.00E-05 |
8.254E-02 |
+2.8 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
7.80E-03 |
0.00E+00 |
| 126.50 |
1.367E-02 |
+2.9 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
1.31E-03 |
4.00E-05 |
8.153E-02 |
+2.9 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
7.75E-03 |
0.00E+00 |
| 127.00 |
1.351E-02 |
+2.9 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
1.30E-03 |
4.00E-05 |
8.054E-02 |
+2.9 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
7.71E-03 |
0.00E+00 |
| 127.50 |
1.335E-02 |
+2.8 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.29E-03 |
4.00E-05 |
7.960E-02 |
+2.8 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.67E-03 |
0.00E+00 |
| 128.00 |
1.319E-02 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.29E-03 |
4.00E-05 |
7.867E-02 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.63E-03 |
0.00E+00 |
| 128.50 |
1.302E-02 |
+3.0 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
1.28E-03 |
4.00E-05 |
7.763E-02 |
+3.0 |
-2.5 |
±1.7 |
±1.5 |
±0.7 |
7.57E-03 |
0.00E+00 |
| 129.00 |
1.287E-02 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.27E-03 |
4.00E-05 |
7.675E-02 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.54E-03 |
0.00E+00 |
| 129.50 |
1.272E-02 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.26E-03 |
4.00E-05 |
7.582E-02 |
+2.9 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.49E-03 |
0.00E+00 |
| 130.00 |
1.256E-02 |
+3.0 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
1.25E-03 |
4.00E-05 |
7.490E-02 |
+3.0 |
-2.6 |
±1.7 |
±1.5 |
±0.7 |
7.43E-03 |
0.00E+00 |
ttH Process
- Cross sections are calculated at NLO QCD and NLO EW accuracies.
- Calculations are the same as CERN Report 3, except NLO EW corrections are adopted now.
- Program: MadGraph5_aMC@NLO (Sherpa+OpenLoops as cross ceck)
- QCD scales: μ=μF=μR=Mtop+MH/2, uncertainty estimated in the range 1/2 < μ/(Mtop+MH/2) < 2 (with 1/2 < μF/μR < 2 constraint).
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nlo_30_pdfas
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
| 120.00 |
1.501E-01 |
+4.1 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 120.50 |
1.485E-01 |
+4.1 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 121.00 |
1.465E-01 |
+4.1 |
-9.3 |
±4.3 |
±3.7 |
±2.1 |
| 121.50 |
1.447E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 122.00 |
1.431E-01 |
+4.1 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 122.50 |
1.413E-01 |
+4.1 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 123.00 |
1.395E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 123.50 |
1.379E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.00 |
1.363E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.10 |
1.361E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.20 |
1.355E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.30 |
1.352E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.40 |
1.349E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.50 |
1.346E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.60 |
1.343E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.70 |
1.339E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.80 |
1.336E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 124.90 |
1.334E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.00 |
1.330E-01 |
+4.1 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.09 |
1.326E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.10 |
1.327E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.20 |
1.324E-01 |
+4.1 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.30 |
1.321E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.40 |
1.316E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.50 |
1.314E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.60 |
1.310E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.70 |
1.306E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.80 |
1.305E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 125.90 |
1.302E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 126.00 |
1.299E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 126.50 |
1.282E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 127.00 |
1.266E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 127.50 |
1.253E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 128.00 |
1.237E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 128.50 |
1.224E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 129.00 |
1.208E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 129.50 |
1.194E-01 |
+3.9 |
-9.2 |
±4.3 |
±3.7 |
±2.1 |
| 130.00 |
1.181E-01 |
+4.0 |
-9.2 |
±4.3 |
±3.7 |
±2.2 |
bbH Process
- The cross sections are the Santander matched numbers with 5FS (NNLO) and 4FS (NLO). No EW corrections.
- Program: SusHi for 5FS and dedicated version of MadGraph5_aMC@NLO for 4FS.
- QCD scales:
- 5FS: μF=MH/4, μR=MH,
- 4FS: μF=μR=(MH+2Mb)/4,
- scale with 7-point variation by a factor of 2 in both cases.
- Uncertainties
- 5FS: Linearly added scale + (PDF⊕αs) + Mb + μb (PDF and αs uncertainties are added in quadrature).
- 4FS: Only scale uncertainties (as they are the dominant ones) and no PDF uncertainties are included.
- PDF set
- 5FS: Dedicated sets produced with APFEL are used which are generated from the PDF4LHC15_nnlo_100 sets taken below the Mb-threshold and evolved upwards, while generating a b-PDF set at high scale.
- 4FS: PDF4LHC15_nlo_nf4_100
| mH (GeV) |
Cross Section (pb) |
+(QCD Scale+PDF+αs) % |
-(QCD Scale+PDF+αs) % |
| 120.00 |
2.315E-01 |
+20.8 |
-22.8 |
| 120.50 |
2.289E-01 |
+20.8 |
-22.8 |
| 121.00 |
2.250E-01 |
+20.7 |
-22.7 |
| 121.50 |
2.224E-01 |
+20.8 |
-22.7 |
| 122.00 |
2.190E-01 |
+20.6 |
-22.6 |
| 122.50 |
2.161E-01 |
+20.7 |
-22.5 |
| 123.00 |
2.132E-01 |
+20.7 |
-22.5 |
| 123.50 |
2.104E-01 |
+20.7 |
-22.4 |
| 124.00 |
2.071E-01 |
+20.6 |
-22.4 |
| 124.10 |
2.069E-01 |
+20.7 |
-22.4 |
| 124.20 |
2.062E-01 |
+20.6 |
-22.5 |
| 124.30 |
2.056E-01 |
+20.7 |
-22.6 |
| 124.40 |
2.052E-01 |
+20.8 |
-22.6 |
| 124.50 |
2.045E-01 |
+20.6 |
-22.4 |
| 124.60 |
2.043E-01 |
+20.7 |
-22.5 |
| 124.70 |
2.036E-01 |
+20.7 |
-22.5 |
| 124.80 |
2.028E-01 |
+20.6 |
-22.5 |
| 124.90 |
2.024E-01 |
+20.7 |
-22.5 |
| 125.00 |
2.021E-01 |
+20.7 |
-22.3 |
| 125.09 |
2.015E-01 |
+20.6 |
-22.4 |
| 125.10 |
2.008E-01 |
+20.6 |
-22.3 |
| 125.20 |
2.008E-01 |
+20.7 |
-22.4 |
| 125.30 |
2.005E-01 |
+20.7 |
-22.4 |
| 125.40 |
1.998E-01 |
+20.7 |
-22.5 |
| 125.50 |
1.993E-01 |
+20.6 |
-22.3 |
| 125.60 |
1.993E-01 |
+20.6 |
-22.3 |
| 125.70 |
1.988E-01 |
+20.7 |
-22.4 |
| 125.80 |
1.982E-01 |
+20.7 |
-22.4 |
| 125.90 |
1.974E-01 |
+20.8 |
-22.5 |
| 126.00 |
1.968E-01 |
+20.6 |
-22.3 |
| 126.50 |
1.936E-01 |
+20.6 |
-22.1 |
| 127.00 |
1.914E-01 |
+20.5 |
-22.2 |
| 127.50 |
1.882E-01 |
+20.4 |
-22.1 |
| 128.00 |
1.864E-01 |
+20.4 |
-22.1 |
| 128.50 |
1.833E-01 |
+20.3 |
-22.0 |
| 129.00 |
1.811E-01 |
+20.3 |
-22.0 |
| 129.50 |
1.786E-01 |
+20.4 |
-22.0 |
| 130.00 |
1.763E-01 |
+20.3 |
-21.9 |
tH Process
t-ch (qb→tHq)
- Cross sections are calculated at NLO QCD accuracy (no NLO EW correction) in 5FS.
- Program: MadGraph5_aMC@NLO
- QCD scales: μ=μF=μR=(Mtop+MH)/4, uncertainty estimated in the range 1/2 < μ/{(Mtop+MH)/4} < 2 (with 1/2 < μF/μR < 2 constraint).
- Flavour scheme (FS) dependence (4FS - 5FS envelope) included in the scale uncertainty. No PU uncertainty assigned.
- PDF set:
- PDF4LHC15_nlo_30_pdfas (5FS)
- PDF4LHC15_nlo_nf4_100 (4FS central set), used to compute the combined scale+FS uncertainty in tH t-channel.
| mH (GeV) |
Cross Section (pb) |
+(QCD Scale + FS) % |
-(QCD Scale + FS) % |
±(PDF+αs) % |
±PDF % |
±αs % |
tH (pb) |
tbarH (pb) |
| 120.00 |
1.959E-02 |
+7.4 |
-16.0 |
±4.6 |
±4.4 |
±1.4 |
1.337E-02 |
6.220E-03 |
| 120.50 |
1.949E-02 |
+7.4 |
-16.0 |
±4.6 |
±4.4 |
±1.4 |
1.330E-02 |
6.190E-03 |
| 121.00 |
1.938E-02 |
+7.4 |
-16.0 |
±4.6 |
±4.4 |
±1.4 |
1.325E-02 |
6.160E-03 |
| 121.50 |
1.929E-02 |
+7.4 |
-16.1 |
±4.6 |
±4.4 |
±1.4 |
1.315E-02 |
6.130E-03 |
| 122.00 |
1.921E-02 |
+7.4 |
-16.1 |
±4.6 |
±4.4 |
±1.4 |
1.310E-02 |
6.110E-03 |
| 122.50 |
1.911E-02 |
+7.4 |
-16.3 |
±4.6 |
±4.4 |
±1.4 |
1.302E-02 |
6.080E-03 |
| 123.00 |
1.902E-02 |
+7.3 |
-16.3 |
±4.6 |
±4.4 |
±1.4 |
1.299E-02 |
6.050E-03 |
| 123.50 |
1.892E-02 |
+7.3 |
-16.2 |
±4.6 |
±4.4 |
±1.4 |
1.293E-02 |
6.030E-03 |
| 124.00 |
1.887E-02 |
+7.3 |
-16.4 |
±4.6 |
±4.4 |
±1.4 |
1.286E-02 |
5.990E-03 |
| 124.10 |
1.882E-02 |
+7.3 |
-16.3 |
±4.6 |
±4.4 |
±1.4 |
1.284E-02 |
5.990E-03 |
| 124.20 |
1.881E-02 |
+7.3 |
-16.4 |
±4.6 |
±4.4 |
±1.4 |
1.285E-02 |
6.000E-03 |
| 124.30 |
1.878E-02 |
+7.3 |
-16.4 |
±4.6 |
±4.4 |
±1.4 |
1.284E-02 |
5.990E-03 |
| 124.40 |
1.876E-02 |
+7.3 |
-16.3 |
±4.6 |
±4.4 |
±1.4 |
1.282E-02 |
5.970E-03 |
| 124.50 |
1.878E-02 |
+7.2 |
-16.4 |
±4.6 |
±4.4 |
±1.4 |
1.281E-02 |
5.970E-03 |
| 124.60 |
1.875E-02 |
+7.3 |
-16.4 |
±4.6 |
±4.4 |
±1.4 |
1.278E-02 |
5.970E-03 |
| 124.70 |
1.875E-02 |
+7.3 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.278E-02 |
5.960E-03 |
| 124.80 |
1.871E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.276E-02 |
5.950E-03 |
| 124.90 |
1.870E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.277E-02 |
5.950E-03 |
| 125.00 |
1.869E-02 |
+7.3 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.273E-02 |
5.950E-03 |
| 125.09 |
1.866E-02 |
+7.3 |
-16.6 |
±4.6 |
±4.4 |
±1.4 |
1.272E-02 |
5.950E-03 |
| 125.10 |
1.866E-02 |
+7.3 |
-16.6 |
±4.6 |
±4.4 |
±1.4 |
1.272E-02 |
5.950E-03 |
| 125.20 |
1.866E-02 |
+7.3 |
-16.6 |
±4.6 |
±4.4 |
±1.4 |
1.274E-02 |
5.940E-03 |
| 125.30 |
1.864E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.270E-02 |
5.920E-03 |
| 125.40 |
1.862E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.269E-02 |
5.930E-03 |
| 125.50 |
1.862E-02 |
+7.2 |
-16.6 |
±4.6 |
±4.4 |
±1.4 |
1.268E-02 |
5.920E-03 |
| 125.60 |
1.857E-02 |
+7.2 |
-16.6 |
±4.6 |
±4.4 |
±1.4 |
1.266E-02 |
5.920E-03 |
| 125.70 |
1.855E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.266E-02 |
5.910E-03 |
| 125.80 |
1.856E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.264E-02 |
5.900E-03 |
| 125.90 |
1.854E-02 |
+7.2 |
-16.5 |
±4.6 |
±4.4 |
±1.4 |
1.265E-02 |
5.900E-03 |
| 126.00 |
1.852E-02 |
+7.2 |
-16.6 |
±4.7 |
±4.4 |
±1.4 |
1.262E-02 |
5.900E-03 |
| 126.50 |
1.844E-02 |
+7.2 |
-16.8 |
±4.7 |
±4.4 |
±1.4 |
1.256E-02 |
5.870E-03 |
| 127.00 |
1.836E-02 |
+7.2 |
-16.4 |
±4.7 |
±4.4 |
±1.4 |
1.249E-02 |
5.850E-03 |
| 127.50 |
1.828E-02 |
+7.1 |
-16.8 |
±4.7 |
±4.4 |
±1.4 |
1.245E-02 |
5.820E-03 |
| 128.00 |
1.820E-02 |
+7.1 |
-16.8 |
±4.7 |
±4.4 |
±1.4 |
1.242E-02 |
5.790E-03 |
| 128.50 |
1.813E-02 |
+7.1 |
-16.8 |
±4.7 |
±4.5 |
±1.4 |
1.236E-02 |
5.790E-03 |
| 129.00 |
1.804E-02 |
+7.1 |
-16.8 |
±4.7 |
±4.5 |
±1.4 |
1.230E-02 |
5.750E-03 |
| 129.50 |
1.796E-02 |
+7.1 |
-16.8 |
±4.7 |
±4.5 |
±1.4 |
1.226E-02 |
5.720E-03 |
| 130.00 |
1.787E-02 |
+7.1 |
-16.9 |
±4.7 |
±4.5 |
±1.4 |
1.219E-02 |
5.710E-03 |
s-ch (qq→tHb)
- Cross sections are calculated at NLO QCD accuracy (no NLO EW correction) in 5FS.
- Program: MadGraph5_aMC@NLO
- QCD scales: μ=μF=μR=(Mtop+MH)/2, uncertainty estimated in the range 1/2 < μ/{(Mtop+MH)/2} < 2 (with 1/2 < μF/μR < 2 constraint).
- No additional THU nor PU uncertainties assigned.
- PDF set:
- PDF4LHC15_nlo_30_pdfas (5FS)
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
tH (pb) |
tbarH (pb) |
| 120.00 |
1.339E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.1 |
9.130E-04 |
4.260E-04 |
| 120.50 |
1.326E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
9.030E-04 |
4.220E-04 |
| 121.00 |
1.313E-03 |
+2.8 |
-2.3 |
±2.8 |
±2.8 |
±0.0 |
8.950E-04 |
4.180E-04 |
| 121.50 |
1.301E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.870E-04 |
4.130E-04 |
| 122.00 |
1.287E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.780E-04 |
4.090E-04 |
| 122.50 |
1.274E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.700E-04 |
4.050E-04 |
| 123.00 |
1.263E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.620E-04 |
4.010E-04 |
| 123.50 |
1.251E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.540E-04 |
3.970E-04 |
| 124.00 |
1.238E-03 |
+2.7 |
-2.3 |
±2.8 |
±2.8 |
±0.0 |
8.450E-04 |
3.930E-04 |
| 124.10 |
1.235E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.430E-04 |
3.920E-04 |
| 124.20 |
1.233E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.420E-04 |
3.910E-04 |
| 124.30 |
1.232E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.410E-04 |
3.900E-04 |
| 124.40 |
1.228E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.390E-04 |
3.900E-04 |
| 124.50 |
1.225E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.380E-04 |
3.880E-04 |
| 124.60 |
1.224E-03 |
+2.7 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.360E-04 |
3.880E-04 |
| 124.70 |
1.221E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.340E-04 |
3.870E-04 |
| 124.80 |
1.219E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.320E-04 |
3.860E-04 |
| 124.90 |
1.216E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.310E-04 |
3.850E-04 |
| 125.00 |
1.214E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.290E-04 |
3.850E-04 |
| 125.09 |
1.211E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.280E-04 |
3.840E-04 |
| 125.10 |
1.211E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.280E-04 |
3.840E-04 |
| 125.20 |
1.209E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.270E-04 |
3.830E-04 |
| 125.30 |
1.208E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.250E-04 |
3.830E-04 |
| 125.40 |
1.204E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.240E-04 |
3.810E-04 |
| 125.50 |
1.202E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.220E-04 |
3.810E-04 |
| 125.60 |
1.200E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.200E-04 |
3.800E-04 |
| 125.70 |
1.198E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.180E-04 |
3.790E-04 |
| 125.80 |
1.195E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.170E-04 |
3.790E-04 |
| 125.90 |
1.193E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.150E-04 |
3.780E-04 |
| 126.00 |
1.191E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.140E-04 |
3.770E-04 |
| 126.50 |
1.179E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
8.060E-04 |
3.730E-04 |
| 127.00 |
1.167E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
7.980E-04 |
3.700E-04 |
| 127.50 |
1.158E-03 |
+2.7 |
-2.3 |
±2.8 |
±2.8 |
±0.0 |
7.910E-04 |
3.660E-04 |
| 128.00 |
1.146E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
7.840E-04 |
3.630E-04 |
| 128.50 |
1.134E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
7.770E-04 |
3.590E-04 |
| 129.00 |
1.126E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
7.700E-04 |
3.560E-04 |
| 129.50 |
1.115E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
7.630E-04 |
3.520E-04 |
| 130.00 |
1.103E-03 |
+2.8 |
-2.4 |
±2.8 |
±2.8 |
±0.0 |
7.550E-04 |
3.480E-04 |
W-associated (gb→tHW)
- Cross sections are calculated at NLO QCD accuracy (no NLO EW correction) in 5FS
- With DR2 (Diagram Removal plus interference) described in [Demartin:2016axk]
- σ(tHW-) = σ(tbarHW+) = (σ(tHW-)+σ(tbarHW+))/2
- Program: MadGraph5_aMC@NLO
- QCD scales: μ=μF=μR=(Mtop+MH+MW)/2, uncertainty estimated in the range 1/2 < μ/{(Mtop+MH+MW)/2} < 2 (with 1/2 < μF/μR < 2 constraint).
- PDF set:
- PDF4LHC15_nlo_30_pdfas (5FS)
| mH (GeV) |
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
| 125.00 |
3.51E-03 |
+4.3 |
-5.7 |
±7.9 |
±7.6 |
±1.9 |
--
ReiTanaka - 2016-03-01
This topic: LHCPhysics
> LHCHXSWG > CERNYellowReportPageAt8TeV
Topic revision: r20 - 2017-01-27 - ReiTanaka
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