SM Higgs production cross sections at √s = 13 TeV (update in CERN Report4 2016)
- Cross sections reported in CERN Report 4.
- SM Higgs cross sections and BRs in Spread sheet is available in xlsx format (update 2016.02.14)
- You can find figures at our gallery here.
Mass range and step for SM-like Higgs boson:
| Higgs Mass range | step size | # of points |
addendum |
|---|---|---|---|
| [126,130] GeV | 0.5 GeV | 8 points | |
| [120,124] GeV | 0.5 GeV | 9 points | |
| [124,126] GeV | 0.1 GeV | 20 points | + MH=125.09 GeV |
- Total 38 points for MH=[120,130] GeV.
gluon-gluon Fusion Process
- 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
| mH (GeV) | Cross Section (pb) | +QCD Scale % | -QCD Scale % | ±(PDF+αs) % | ±PDF % | ±αs % |
| 120.00 | 4.738E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 120.50 | 4.704E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 121.00 | 4.670E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 121.50 | 4.637E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 122.00 | 4.604E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 122.50 | 4.571E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 123.00 | 4.539E+01 | +7.7 | -8.2 | ±3.1 | ±1.8 | ±2.5 |
| 123.50 | 4.507E+01 | +7.7 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.00 | 4.476E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.10 | 4.470E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.20 | 4.463E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.30 | 4.457E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.40 | 4.451E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.50 | 4.445E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.60 | 4.438E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.70 | 4.432E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.80 | 4.426E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 124.90 | 4.420E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.00 | 4.414E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.09 | 4.408E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.10 | 4.408E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.20 | 4.402E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.30 | 4.396E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.40 | 4.390E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.50 | 4.383E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.60 | 4.377E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.70 | 4.371E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.80 | 4.365E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 125.90 | 4.359E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 126.00 | 4.353E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 126.50 | 4.324E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 127.00 | 4.294E+01 | +7.6 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 127.50 | 4.265E+01 | +7.5 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 128.00 | 4.236E+01 | +7.5 | -8.1 | ±3.1 | ±1.8 | ±2.5 |
| 128.50 | 4.207E+01 | +7.5 | -8.0 | ±3.1 | ±1.8 | ±2.5 |
| 129.00 | 4.179E+01 | +7.5 | -8.0 | ±3.1 | ±1.8 | ±2.5 |
| 129.50 | 4.151E+01 | +7.5 | -8.0 | ±3.1 | ±1.8 | ±2.5 |
| 130.00 | 4.123E+01 | +7.5 | -8.0 | ±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 or without constraint, i.e. μF and μR are varied independently?).
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nnlo_100 or PDF4LHC15_nnlo_30_pdfas ?
| mH (GeV) | Cross Section (pb) | +QCD Scale % | -QCD Scale % | ±(PDF+αs) % | ±PDF % | ±αs % |
| 120.00 | 3.935E+00 | +0.4 | -0.3 | ±2.1 | ||
| 120.50 | 3.919E+00 | +0.4 | -0.3 | ±2.1 | ||
| 121.00 | 3.904E+00 | +0.4 | -0.3 | ±2.1 | ||
| 121.50 | 3.888E+00 | +0.4 | -0.3 | ±2.1 | ||
| 122.00 | 3.873E+00 | +0.4 | -0.3 | ±2.1 | ||
| 122.50 | 3.858E+00 | +0.4 | -0.3 | ±2.1 | ||
| 123.00 | 3.842E+00 | +0.4 | -0.3 | ±2.1 | ||
| 123.50 | 3.827E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.00 | 3.812E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.10 | 3.809E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.20 | 3.806E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.30 | 3.803E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.40 | 3.800E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.50 | 3.797E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.60 | 3.794E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.70 | 3.791E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.80 | 3.788E+00 | +0.4 | -0.3 | ±2.1 | ||
| 124.90 | 3.785E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.00 | 3.782E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.09 | 3.779E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.10 | 3.779E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.20 | 3.776E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.30 | 3.773E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.40 | 3.770E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.50 | 3.767E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.60 | 3.764E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.70 | 3.761E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.80 | 3.758E+00 | +0.4 | -0.3 | ±2.1 | ||
| 125.90 | 3.755E+00 | +0.4 | -0.3 | ±2.1 | ||
| 126.00 | 3.752E+00 | +0.4 | -0.3 | ±2.1 | ||
| 126.50 | 3.738E+00 | +0.4 | -0.3 | ±2.1 | ||
| 127.00 | 3.723E+00 | +0.4 | -0.3 | ±2.1 | ||
| 127.50 | 3.708E+00 | +0.4 | -0.3 | ±2.1 | ||
| 128.00 | 3.694E+00 | +0.4 | -0.3 | ±2.1 | ||
| 128.50 | 3.680E+00 | +0.4 | -0.3 | ±2.1 | ||
| 129.00 | 3.665E+00 | +0.4 | -0.3 | ±2.1 | ||
| 129.50 | 3.651E+00 | +0.4 | -0.3 | ±2.1 | ||
| 130.00 | 3.637E+00 | +0.4 | -0.3 | ±2.1 |
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).
- Program: NNLO QCD (VBF@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%) (still under discussion and subject to change).
- NOT included for total cross section.
- 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 | 1.565E+00 | +0.5 | -0.6 | ±1.8 | 9.560E-01 | 6.092E-01 | ||
| 120.50 | 1.545E+00 | +0.5 | -0.7 | ±1.8 | 9.442E-01 | 6.007E-01 | ||
| 121.00 | 1.525E+00 | +0.5 | -0.7 | ±1.8 | 9.323E-01 | 5.924E-01 | ||
| 121.50 | 1.505E+00 | +0.4 | -0.7 | ±1.8 | 9.204E-01 | 5.845E-01 | ||
| 122.00 | 1.485E+00 | +0.4 | -0.7 | ±1.8 | 9.086E-01 | 5.764E-01 | ||
| 122.50 | 1.466E+00 | +0.5 | -0.8 | ±1.9 | 8.968E-01 | 5.693E-01 | ||
| 123.00 | 1.446E+00 | +0.6 | -0.7 | ±1.9 | 8.840E-01 | 5.618E-01 | ||
| 123.50 | 1.427E+00 | +0.6 | -0.7 | ±1.9 | 8.722E-01 | 5.545E-01 | ||
| 124.00 | 1.408E+00 | +0.6 | -0.6 | ±1.9 | 8.612E-01 | 5.465E-01 | ||
| 124.10 | 1.404E+00 | +0.5 | -0.6 | ±1.9 | 8.590E-01 | 5.454E-01 | ||
| 124.20 | 1.401E+00 | +0.5 | -0.6 | ±1.9 | 8.568E-01 | 5.440E-01 | ||
| 124.30 | 1.398E+00 | +0.6 | -0.7 | ±1.9 | 8.548E-01 | 5.429E-01 | ||
| 124.40 | 1.394E+00 | +0.5 | -0.7 | ±1.9 | 8.527E-01 | 5.415E-01 | ||
| 124.50 | 1.390E+00 | +0.6 | -0.6 | ±1.9 | 8.500E-01 | 5.395E-01 | ||
| 124.60 | 1.387E+00 | +0.5 | -0.7 | ±1.9 | 8.487E-01 | 5.386E-01 | ||
| 124.70 | 1.383E+00 | +0.5 | -0.7 | ±1.9 | 8.463E-01 | 5.372E-01 | ||
| 124.80 | 1.380E+00 | +0.5 | -0.8 | ±1.9 | 8.441E-01 | 5.360E-01 | ||
| 124.90 | 1.376E+00 | +0.5 | -0.7 | ±1.9 | 8.418E-01 | 5.345E-01 | ||
| 125.00 | 1.373E+00 | +0.5 | -0.7 | ±1.9 | 8.399E-01 | 5.327E-01 | ||
| 125.09 | 1.369E+00 | +0.5 | -0.7 | ±1.9 | 8.380E-01 | 5.313E-01 | ||
| 125.10 | 1.369E+00 | +0.5 | -0.7 | ±1.9 | 8.377E-01 | 5.313E-01 | ||
| 125.20 | 1.365E+00 | +0.6 | -0.7 | ±1.9 | 8.355E-01 | 5.297E-01 | ||
| 125.30 | 1.362E+00 | +0.6 | -0.7 | ±1.9 | 8.334E-01 | 5.282E-01 | ||
| 125.40 | 1.358E+00 | +0.6 | -0.7 | ±1.9 | 8.313E-01 | 5.272E-01 | ||
| 125.50 | 1.355E+00 | +0.5 | -0.7 | ±1.9 | 8.291E-01 | 5.259E-01 | ||
| 125.60 | 1.351E+00 | +0.5 | -0.6 | ±1.9 | 8.270E-01 | 5.243E-01 | ||
| 125.70 | 1.347E+00 | +0.5 | -0.6 | ±1.9 | 8.243E-01 | 5.231E-01 | ||
| 125.80 | 1.344E+00 | +0.6 | -0.7 | ±1.9 | 8.224E-01 | 5.217E-01 | ||
| 125.90 | 1.341E+00 | +0.5 | -0.8 | ±1.9 | 8.212E-01 | 5.202E-01 | ||
| 126.00 | 1.337E+00 | +0.6 | -0.8 | ±1.9 | 8.184E-01 | 5.187E-01 | ||
| 126.50 | 1.320E+00 | +0.6 | -0.7 | ±1.9 | 8.080E-01 | 5.123E-01 | ||
| 127.00 | 1.304E+00 | +0.5 | -0.7 | ±1.8 | 7.987E-01 | 5.051E-01 | ||
| 127.50 | 1.287E+00 | +0.6 | -0.7 | ±1.8 | 7.879E-01 | 4.988E-01 | ||
| 128.00 | 1.271E+00 | +0.5 | -0.7 | ±1.8 | 7.785E-01 | 4.923E-01 | ||
| 128.50 | 1.255E+00 | +0.5 | -0.7 | ±1.8 | 7.686E-01 | 4.863E-01 | ||
| 129.00 | 1.239E+00 | +0.5 | -0.7 | ±1.8 | 7.593E-01 | 4.801E-01 | ||
| 129.50 | 1.224E+00 | +0.5 | -0.7 | ±1.8 | 7.500E-01 | 4.738E-01 | ||
| 130.00 | 1.209E+00 | +0.4 | -0.7 | ±1.8 | 7.413E-01 | 4.676E-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 | 1.099E-01 | +0.6 | -0.6 | ±1.8 | 6.140E-03 | 7.042E-02 | +0.4 | -0.6 | ±1.9 | 4.300E-03 | ||||
| 120.50 | 1.086E-01 | +0.5 | -0.7 | ±1.8 | 6.120E-03 | 6.949E-02 | +0.5 | -0.6 | ±1.9 | 4.290E-03 | ||||
| 121.00 | 1.073E-01 | +0.5 | -0.7 | ±1.8 | 6.110E-03 | 6.859E-02 | +0.5 | -0.6 | ±1.9 | 4.290E-03 | ||||
| 121.50 | 1.060E-01 | +0.4 | -0.8 | ±1.8 | 6.100E-03 | 6.772E-02 | +0.5 | -0.6 | ±1.9 | 4.280E-03 | ||||
| 122.00 | 1.047E-01 | +0.3 | -0.8 | ±1.8 | 6.090E-03 | 6.683E-02 | +0.6 | -0.6 | ±1.9 | 4.270E-03 | ||||
| 122.50 | 1.034E-01 | +0.5 | -0.8 | ±1.8 | 6.070E-03 | 6.605E-02 | +0.4 | -0.7 | ±2.0 | 4.260E-03 | ||||
| 123.00 | 1.020E-01 | +0.6 | -0.7 | ±1.8 | 6.050E-03 | 6.521E-02 | +0.5 | -0.6 | ±2.0 | 4.240E-03 | ||||
| 123.50 | 1.007E-01 | +0.6 | -0.7 | ±1.8 | 6.040E-03 | 6.441E-02 | +0.5 | -0.7 | ±2.0 | 4.230E-03 | ||||
| 124.00 | 9.950E-02 | +0.6 | -0.6 | ±1.8 | 6.030E-03 | 6.354E-02 | +0.6 | -0.6 | ±2.0 | 4.230E-03 | ||||
| 124.10 | 9.926E-02 | +0.5 | -0.6 | ±1.8 | 6.030E-03 | 6.343E-02 | +0.5 | -0.7 | ±2.0 | 4.230E-03 | ||||
| 124.20 | 9.902E-02 | +0.5 | -0.6 | ±1.8 | 6.030E-03 | 6.326E-02 | +0.5 | -0.6 | ±2.0 | 4.220E-03 | ||||
| 124.30 | 9.880E-02 | +0.6 | -0.7 | ±1.8 | 6.020E-03 | 6.314E-02 | +0.5 | -0.6 | ±2.0 | 4.220E-03 | ||||
| 124.40 | 9.857E-02 | +0.6 | -0.7 | ±1.8 | 6.020E-03 | 6.299E-02 | +0.4 | -0.7 | ±2.0 | 4.220E-03 | ||||
| 124.50 | 9.828E-02 | +0.6 | -0.6 | ±1.8 | 6.020E-03 | 6.277E-02 | +0.6 | -0.6 | ±2.0 | 4.210E-03 | ||||
| 124.60 | 9.813E-02 | +0.5 | -0.7 | ±1.8 | 6.020E-03 | 6.267E-02 | +0.4 | -0.7 | ±2.0 | 4.210E-03 | ||||
| 124.70 | 9.786E-02 | +0.6 | -0.7 | ±1.8 | 6.010E-03 | 6.251E-02 | +0.4 | -0.7 | ±2.0 | 4.210E-03 | ||||
| 124.80 | 9.762E-02 | +0.6 | -0.8 | ±1.8 | 6.010E-03 | 6.238E-02 | +0.4 | -0.7 | ±2.0 | 4.210E-03 | ||||
| 124.90 | 9.738E-02 | +0.6 | -0.7 | ±1.8 | 6.010E-03 | 6.222E-02 | +0.3 | -0.7 | ±2.0 | 4.210E-03 | ||||
| 125.00 | 9.717E-02 | +0.5 | -0.7 | ±1.8 | 6.010E-03 | 6.203E-02 | +0.4 | -0.7 | ±2.0 | 4.210E-03 | ||||
| 125.09 | 9.695E-02 | +0.5 | -0.7 | ±1.8 | 6.000E-03 | 6.187E-02 | +0.4 | -0.6 | ±2.0 | 4.200E-03 | ||||
| 125.10 | 9.692E-02 | +0.6 | -0.7 | ±1.8 | 6.000E-03 | 6.187E-02 | +0.4 | -0.6 | ±2.0 | 4.210E-03 | ||||
| 125.20 | 9.668E-02 | +0.6 | -0.7 | ±1.8 | 6.000E-03 | 6.169E-02 | +0.5 | -0.6 | ±2.0 | 4.200E-03 | ||||
| 125.30 | 9.645E-02 | +0.6 | -0.8 | ±1.8 | 6.000E-03 | 6.153E-02 | +0.5 | -0.6 | ±2.0 | 4.200E-03 | ||||
| 125.40 | 9.622E-02 | +0.6 | -0.7 | ±1.8 | 6.000E-03 | 6.142E-02 | +0.5 | -0.8 | ±2.0 | 4.200E-03 | ||||
| 125.50 | 9.598E-02 | +0.6 | -0.7 | ±1.8 | 5.990E-03 | 6.128E-02 | +0.4 | -0.7 | ±2.0 | 4.200E-03 | ||||
| 125.60 | 9.575E-02 | +0.5 | -0.6 | ±1.8 | 5.990E-03 | 6.111E-02 | +0.4 | -0.7 | ±2.0 | 4.200E-03 | ||||
| 125.70 | 9.545E-02 | +0.6 | -0.6 | ±1.8 | 5.990E-03 | 6.096E-02 | +0.3 | -0.7 | ±2.0 | 4.190E-03 | ||||
| 125.80 | 9.524E-02 | +0.7 | -0.7 | ±1.8 | 5.980E-03 | 6.081E-02 | +0.4 | -0.8 | ±2.0 | 4.190E-03 | ||||
| 125.90 | 9.511E-02 | +0.6 | -0.8 | ±1.8 | 5.980E-03 | 6.065E-02 | +0.4 | -0.7 | ±2.0 | 4.190E-03 | ||||
| 126.00 | 9.481E-02 | +0.6 | -0.8 | ±1.8 | 5.980E-03 | 6.049E-02 | +0.5 | -0.7 | ±2.0 | 4.190E-03 | ||||
| 126.50 | 9.367E-02 | +0.6 | -0.7 | ±1.8 | 5.970E-03 | 5.977E-02 | +0.5 | -0.7 | ±2.0 | 4.170E-03 | ||||
| 127.00 | 9.264E-02 | +0.5 | -0.7 | ±1.8 | 5.950E-03 | 5.899E-02 | +0.5 | -0.6 | ±1.9 | 4.170E-03 | ||||
| 127.50 | 9.146E-02 | +0.6 | -0.7 | ±1.8 | 5.940E-03 | 5.830E-02 | +0.5 | -0.6 | ±1.9 | 4.160E-03 | ||||
| 128.00 | 9.042E-02 | +0.5 | -0.7 | ±1.8 | 5.930E-03 | 5.758E-02 | +0.4 | -0.6 | ±1.9 | 4.150E-03 | ||||
| 128.50 | 8.934E-02 | +0.6 | -0.7 | ±1.8 | 5.920E-03 | 5.691E-02 | +0.4 | -0.7 | ±1.9 | 4.130E-03 | ||||
| 129.00 | 8.831E-02 | +0.5 | -0.7 | ±1.8 | 5.900E-03 | 5.624E-02 | +0.4 | -0.7 | ±1.9 | 4.130E-03 | ||||
| 129.50 | 8.729E-02 | +0.5 | -0.7 | ±1.8 | 5.890E-03 | 5.554E-02 | +0.5 | -0.7 | ±1.9 | 4.120E-03 | ||||
| 130.00 | 8.634E-02 | +0.4 | -0.8 | ±1.8 | 5.880E-03 | 5.486E-02 | +0.5 | -0.6 | ±1.9 | 4.110E-03 | ||||
ZH Process
- Cross sections are calculated at NNLO QCD (VH@NNLO) and NLO EW (HAWK) accuracies.
- gg→ZH (box-diagram) occurs as a part of NNLO QCD correction and included in the total cross section.
- Calculations are the same as CERN Report 3, except photon-induced contribution (see below).
- 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 (still under discussion and subject to change).
- NOT included for total cross section.
- Included in cross sections for dedicated ZH→llH (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 % | σ(gg→ZH) (pb) |
| 120.00 | 9.939E-01 | +3.4 | -3.0 | ±1.6 | 1.299E-01 | ||
| 120.50 | 9.829E-01 | +3.4 | -3.0 | ±1.6 | 1.292E-01 | ||
| 121.00 | 9.705E-01 | +3.5 | -3.0 | ±1.6 | 1.281E-01 | ||
| 121.50 | 9.591E-01 | +3.6 | -3.0 | ±1.6 | 1.269E-01 | ||
| 122.00 | 9.485E-01 | +3.6 | -3.0 | ±1.6 | 1.271E-01 | ||
| 122.50 | 9.371E-01 | +3.6 | -3.0 | ±1.6 | 1.265E-01 | ||
| 123.00 | 9.266E-01 | +3.6 | -3.1 | ±1.6 | 1.254E-01 | ||
| 123.50 | 9.157E-01 | +3.5 | -3.1 | ±1.6 | 1.250E-01 | ||
| 124.00 | 9.051E-01 | +3.6 | -3.1 | ±1.6 | 1.242E-01 | ||
| 124.10 | 9.037E-01 | +3.7 | -3.2 | ±1.6 | 1.242E-01 | ||
| 124.20 | 9.008E-01 | +3.8 | -3.0 | ±1.6 | 1.241E-01 | ||
| 124.30 | 8.988E-01 | +3.7 | -3.1 | ±1.6 | 1.239E-01 | ||
| 124.40 | 8.964E-01 | +3.7 | -3.0 | ±1.6 | 1.236E-01 | ||
| 124.50 | 8.943E-01 | +3.8 | -3.0 | ±1.6 | 1.235E-01 | ||
| 124.60 | 8.921E-01 | +3.8 | -3.0 | ±1.6 | 1.233E-01 | ||
| 124.70 | 8.902E-01 | +3.8 | -3.1 | ±1.6 | 1.235E-01 | ||
| 124.80 | 8.884E-01 | +3.7 | -3.1 | ±1.6 | 1.230E-01 | ||
| 124.90 | 8.858E-01 | +3.9 | -3.1 | ±1.6 | 1.227E-01 | ||
| 125.00 | 8.839E-01 | +3.8 | -3.1 | ±1.6 | 1.227E-01 | ||
| 125.09 | 8.824E-01 | +3.8 | -3.0 | ±1.6 | 1.227E-01 | ||
| 125.10 | 8.820E-01 | +3.9 | -3.0 | ±1.6 | 1.226E-01 | ||
| 125.20 | 8.800E-01 | +3.8 | -3.1 | ±1.6 | 1.223E-01 | ||
| 125.30 | 8.785E-01 | +3.8 | -3.1 | ±1.6 | 1.224E-01 | ||
| 125.40 | 8.768E-01 | +3.8 | -3.1 | ±1.6 | 1.223E-01 | ||
| 125.50 | 8.744E-01 | +3.7 | -3.1 | ±1.6 | 1.221E-01 | ||
| 125.60 | 8.729E-01 | +3.8 | -3.1 | ±1.6 | 1.224E-01 | ||
| 125.70 | 8.705E-01 | +3.8 | -3.0 | ±1.6 | 1.218E-01 | ||
| 125.80 | 8.691E-01 | +3.7 | -3.2 | ±1.6 | 1.219E-01 | ||
| 125.90 | 8.669E-01 | +3.8 | -3.1 | ±1.6 | 1.218E-01 | ||
| 126.00 | 8.651E-01 | +3.8 | -3.1 | ±1.6 | 1.218E-01 | ||
| 126.50 | 8.550E-01 | +3.7 | -3.2 | ±1.6 | 1.211E-01 | ||
| 127.00 | 8.447E-01 | +3.7 | -3.2 | ±1.6 | 1.203E-01 | ||
| 127.50 | 8.350E-01 | +3.8 | -3.2 | ±1.6 | 1.197E-01 | ||
| 128.00 | 8.256E-01 | +3.9 | -3.1 | ±1.6 | 1.190E-01 | ||
| 128.50 | 8.163E-01 | +3.9 | -3.2 | ±1.6 | 1.180E-01 | ||
| 129.00 | 8.073E-01 | +3.8 | -3.2 | ±1.6 | 1.177E-01 | ||
| 129.50 | 7.978E-01 | +3.9 | -3.2 | ±1.6 | 1.171E-01 | ||
| 130.00 | 7.897E-01 | +3.9 | -3.2 | ±1.6 | 1.164E-01 |
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 | 3.363E-02 | +3.4 | -3.0 | ±1.6 | 4.380E-03 | 2.200E-04 | 1.997E-01 | +3.4 | -3.0 | ±1.6 | 2.600E-02 | 0.000E+00 | ||||
| 120.50 | 3.326E-02 | +3.4 | -3.0 | ±1.6 | 4.360E-03 | 2.200E-04 | 1.975E-01 | +3.4 | -3.0 | ±1.6 | 2.585E-02 | 0.000E+00 | ||||
| 121.00 | 3.284E-02 | +3.5 | -3.0 | ±1.6 | 4.320E-03 | 2.200E-04 | 1.950E-01 | +3.5 | -3.0 | ±1.6 | 2.564E-02 | 0.000E+00 | ||||
| 121.50 | 3.246E-02 | +3.6 | -3.0 | ±1.6 | 4.280E-03 | 2.200E-04 | 1.927E-01 | +3.6 | -3.0 | ±1.6 | 2.540E-02 | 0.000E+00 | ||||
| 122.00 | 3.210E-02 | +3.6 | -3.0 | ±1.6 | 4.290E-03 | 2.200E-04 | 1.906E-01 | +3.6 | -3.0 | ±1.6 | 2.545E-02 | 0.000E+00 | ||||
| 122.50 | 3.172E-02 | +3.6 | -3.0 | ±1.6 | 4.270E-03 | 2.200E-04 | 1.883E-01 | +3.6 | -3.0 | ±1.6 | 2.531E-02 | 0.000E+00 | ||||
| 123.00 | 3.136E-02 | +3.6 | -3.1 | ±1.6 | 4.230E-03 | 2.200E-04 | 1.862E-01 | +3.6 | -3.1 | ±1.6 | 2.510E-02 | 0.000E+00 | ||||
| 123.50 | 3.100E-02 | +3.5 | -3.1 | ±1.6 | 4.220E-03 | 2.200E-04 | 1.840E-01 | +3.5 | -3.1 | ±1.6 | 2.502E-02 | 0.000E+00 | ||||
| 124.00 | 3.064E-02 | +3.6 | -3.1 | ±1.6 | 4.190E-03 | 2.200E-04 | 1.819E-01 | +3.6 | -3.1 | ±1.6 | 2.486E-02 | 0.000E+00 | ||||
| 124.10 | 3.059E-02 | +3.7 | -3.2 | ±1.6 | 4.190E-03 | 2.200E-04 | 1.816E-01 | +3.7 | -3.2 | ±1.6 | 2.487E-02 | 0.000E+00 | ||||
| 124.20 | 3.050E-02 | +3.8 | -3.0 | ±1.6 | 4.190E-03 | 2.200E-04 | 1.810E-01 | +3.8 | -3.0 | ±1.6 | 2.482E-02 | 0.000E+00 | ||||
| 124.30 | 3.043E-02 | +3.7 | -3.1 | ±1.6 | 4.180E-03 | 2.200E-04 | 1.806E-01 | +3.7 | -3.1 | ±1.6 | 2.480E-02 | 0.000E+00 | ||||
| 124.40 | 3.035E-02 | +3.7 | -3.0 | ±1.6 | 4.170E-03 | 2.200E-04 | 1.801E-01 | +3.7 | -3.0 | ±1.6 | 2.474E-02 | 0.000E+00 | ||||
| 124.50 | 3.028E-02 | +3.8 | -3.0 | ±1.6 | 4.170E-03 | 2.200E-04 | 1.797E-01 | +3.8 | -3.0 | ±1.6 | 2.471E-02 | 0.000E+00 | ||||
| 124.60 | 3.020E-02 | +3.8 | -3.0 | ±1.6 | 4.160E-03 | 2.200E-04 | 1.793E-01 | +3.8 | -3.0 | ±1.6 | 2.467E-02 | 0.000E+00 | ||||
| 124.70 | 3.014E-02 | +3.8 | -3.1 | ±1.6 | 4.170E-03 | 2.200E-04 | 1.789E-01 | +3.8 | -3.1 | ±1.6 | 2.470E-02 | 0.000E+00 | ||||
| 124.80 | 3.008E-02 | +3.7 | -3.1 | ±1.6 | 4.150E-03 | 2.200E-04 | 1.785E-01 | +3.7 | -3.1 | ±1.6 | 2.461E-02 | 0.000E+00 | ||||
| 124.90 | 2.999E-02 | +3.9 | -3.1 | ±1.6 | 4.140E-03 | 2.200E-04 | 1.780E-01 | +3.9 | -3.1 | ±1.6 | 2.458E-02 | 0.000E+00 | ||||
| 125.00 | 2.993E-02 | +3.8 | -3.1 | ±1.6 | 4.140E-03 | 2.200E-04 | 1.776E-01 | +3.8 | -3.1 | ±1.6 | 2.457E-02 | 0.000E+00 | ||||
| 125.09 | 2.987E-02 | +3.8 | -3.0 | ±1.6 | 4.140E-03 | 2.100E-04 | 1.773E-01 | +3.8 | -3.0 | ±1.6 | 2.455E-02 | 0.000E+00 | ||||
| 125.10 | 2.986E-02 | +3.9 | -3.0 | ±1.6 | 4.140E-03 | 2.100E-04 | 1.772E-01 | +3.9 | -3.0 | ±1.6 | 2.454E-02 | 0.000E+00 | ||||
| 125.20 | 2.979E-02 | +3.8 | -3.1 | ±1.6 | 4.130E-03 | 2.100E-04 | 1.768E-01 | +3.8 | -3.1 | ±1.6 | 2.447E-02 | 0.000E+00 | ||||
| 125.30 | 2.974E-02 | +3.8 | -3.1 | ±1.6 | 4.130E-03 | 2.100E-04 | 1.765E-01 | +3.8 | -3.1 | ±1.6 | 2.448E-02 | 0.000E+00 | ||||
| 125.40 | 2.968E-02 | +3.8 | -3.1 | ±1.6 | 4.130E-03 | 2.100E-04 | 1.762E-01 | +3.8 | -3.1 | ±1.6 | 2.446E-02 | 0.000E+00 | ||||
| 125.50 | 2.960E-02 | +3.7 | -3.1 | ±1.6 | 4.120E-03 | 2.100E-04 | 1.757E-01 | +3.7 | -3.1 | ±1.6 | 2.444E-02 | 0.000E+00 | ||||
| 125.60 | 2.955E-02 | +3.8 | -3.1 | ±1.6 | 4.130E-03 | 2.100E-04 | 1.754E-01 | +3.8 | -3.1 | ±1.6 | 2.448E-02 | 0.000E+00 | ||||
| 125.70 | 2.947E-02 | +3.8 | -3.0 | ±1.6 | 4.110E-03 | 2.100E-04 | 1.749E-01 | +3.8 | -3.0 | ±1.6 | 2.436E-02 | 0.000E+00 | ||||
| 125.80 | 2.943E-02 | +3.7 | -3.2 | ±1.6 | 4.110E-03 | 2.100E-04 | 1.746E-01 | +3.7 | -3.2 | ±1.6 | 2.440E-02 | 0.000E+00 | ||||
| 125.90 | 2.935E-02 | +3.8 | -3.1 | ±1.6 | 4.110E-03 | 2.100E-04 | 1.742E-01 | +3.8 | -3.1 | ±1.6 | 2.436E-02 | 0.000E+00 | ||||
| 126.00 | 2.929E-02 | +3.8 | -3.1 | ±1.6 | 4.110E-03 | 2.100E-04 | 1.738E-01 | +3.8 | -3.1 | ±1.6 | 2.437E-02 | 0.000E+00 | ||||
| 126.50 | 2.895E-02 | +3.7 | -3.2 | ±1.6 | 4.090E-03 | 2.100E-04 | 1.718E-01 | +3.7 | -3.2 | ±1.6 | 2.423E-02 | 0.000E+00 | ||||
| 127.00 | 2.861E-02 | +3.7 | -3.2 | ±1.6 | 4.060E-03 | 2.100E-04 | 1.697E-01 | +3.7 | -3.2 | ±1.6 | 2.407E-02 | 0.000E+00 | ||||
| 127.50 | 2.827E-02 | +3.8 | -3.2 | ±1.6 | 4.040E-03 | 2.100E-04 | 1.678E-01 | +3.8 | -3.2 | ±1.6 | 2.394E-02 | 0.000E+00 | ||||
| 128.00 | 2.796E-02 | +3.9 | -3.1 | ±1.6 | 4.020E-03 | 2.100E-04 | 1.659E-01 | +3.9 | -3.1 | ±1.6 | 2.381E-02 | 0.000E+00 | ||||
| 128.50 | 2.765E-02 | +3.9 | -3.2 | ±1.6 | 3.980E-03 | 2.100E-04 | 1.640E-01 | +3.9 | -3.2 | ±1.6 | 2.362E-02 | 0.000E+00 | ||||
| 129.00 | 2.735E-02 | +3.8 | -3.2 | ±1.6 | 3.970E-03 | 2.100E-04 | 1.622E-01 | +3.8 | -3.2 | ±1.6 | 2.355E-02 | 0.000E+00 | ||||
| 129.50 | 2.703E-02 | +3.9 | -3.2 | ±1.6 | 3.950E-03 | 2.100E-04 | 1.603E-01 | +3.9 | -3.2 | ±1.6 | 2.344E-02 | 0.000E+00 | ||||
| 130.00 | 2.675E-02 | +3.9 | -3.2 | ±1.6 | 3.930E-03 | 2.100E-04 | 1.587E-01 | +3.9 | -3.2 | ±1.6 | 2.329E-02 | 0.000E+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 | 5.697E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 120.50 | 5.625E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 121.00 | 5.568E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 121.50 | 5.502E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 122.00 | 5.438E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 122.50 | 5.375E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 123.00 | 5.315E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 123.50 | 5.259E-01 | +5.9 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.00 | 5.193E-01 | +5.9 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.10 | 5.179E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.20 | 5.167E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.30 | 5.161E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 124.40 | 5.143E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.50 | 5.132E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.60 | 5.122E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 124.70 | 5.115E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 124.80 | 5.100E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 124.90 | 5.086E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.00 | 5.071E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.09 | 5.065E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.10 | 5.060E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 125.20 | 5.052E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.30 | 5.043E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.40 | 5.033E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 125.50 | 5.023E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 125.60 | 5.007E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.70 | 4.993E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.80 | 4.982E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 125.90 | 4.971E-01 | +5.9 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 126.00 | 4.964E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 126.50 | 4.909E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 127.00 | 4.851E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 127.50 | 4.799E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 128.00 | 4.742E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 128.50 | 4.689E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 129.00 | 4.639E-01 | +5.8 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
| 129.50 | 4.586E-01 | +5.8 | -9.2 | ±3.6 | ±3.0 | ±2.0 |
| 130.00 | 4.539E-01 | +5.8 | -9.3 | ±3.6 | ±3.0 | ±2.0 |
bbH Process
- The cross sections are the Santander matched numbers with 5FS (NNLO) and 4FS (NLO).
- 4FS includes Yt*Yb term (O(10%) negative correction) in addition to Yb2.
| mH (GeV) | Cross Section (pb) | +(QCD Scale+PDF+αs) % | -(QCD Scale+PDF+αs) % |
| 120.00 | 5.534E-01 | +20.3 | -24.4 |
| 120.50 | 5.471E-01 | +20.3 | -24.4 |
| 121.00 | 5.414E-01 | +20.4 | -24.3 |
| 121.50 | 5.343E-01 | +20.5 | -24.3 |
| 122.00 | 5.268E-01 | +20.4 | -24.3 |
| 122.50 | 5.200E-01 | +20.2 | -24.2 |
| 123.00 | 5.124E-01 | +21.2 | -24.1 |
| 123.50 | 5.066E-01 | +20.1 | -24.0 |
| 124.00 | 4.999E-01 | +20.1 | -24.0 |
| 124.10 | 4.985E-01 | +20.1 | -24.0 |
| 124.20 | 4.976E-01 | +20.3 | -24.1 |
| 124.30 | 4.955E-01 | +20.2 | -24.1 |
| 124.40 | 4.950E-01 | +20.3 | -24.1 |
| 124.50 | 4.930E-01 | +20.0 | -23.9 |
| 124.60 | 4.918E-01 | +20.1 | -24.0 |
| 124.70 | 4.919E-01 | +20.6 | -24.1 |
| 124.80 | 4.899E-01 | +20.2 | -24.0 |
| 124.90 | 4.891E-01 | +20.3 | -24.1 |
| 125.00 | 4.880E-01 | +20.2 | -23.9 |
| 125.09 | 4.863E-01 | +20.1 | -23.9 |
| 125.10 | 4.860E-01 | +20.5 | -23.9 |
| 125.20 | 4.850E-01 | +20.1 | -24.0 |
| 125.30 | 4.833E-01 | +20.1 | -24.0 |
| 125.40 | 4.822E-01 | +20.2 | -24.0 |
| 125.50 | 4.809E-01 | +20.1 | -23.8 |
| 125.60 | 4.792E-01 | +20.1 | -23.9 |
| 125.70 | 4.789E-01 | +20.1 | -23.9 |
| 125.80 | 4.768E-01 | +20.1 | -23.9 |
| 125.90 | 4.757E-01 | +20.2 | -24.0 |
| 126.00 | 4.760E-01 | +20.2 | -23.8 |
| 126.50 | 4.695E-01 | +20.0 | -23.7 |
| 127.00 | 4.635E-01 | +20.0 | -23.7 |
| 127.50 | 4.580E-01 | +20.0 | -23.6 |
| 128.00 | 4.513E-01 | +19.9 | -23.6 |
| 128.50 | 4.463E-01 | +19.9 | -23.5 |
| 129.00 | 4.416E-01 | +20.0 | -23.4 |
| 129.50 | 4.358E-01 | +19.9 | -23.4 |
| 130.00 | 4.304E-01 | +19.9 | -23.3 |
tH Process (t-ch)
- 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 | 7.731E-02 | +6.7 | -14.6 | ±3.7 | ±3.5 | ±1.2 | 5.086E-02 | 2.643E-02 |
| 120.50 | 7.711E-02 | +6.7 | -14.8 | ±3.7 | ±3.5 | ±1.2 | 5.071E-02 | 2.633E-02 |
| 121.00 | 7.684E-02 | +6.7 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 5.047E-02 | 2.623E-02 |
| 121.50 | 7.648E-02 | +6.6 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 5.024E-02 | 2.613E-02 |
| 122.00 | 7.614E-02 | +6.7 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 5.011E-02 | 2.602E-02 |
| 122.50 | 7.581E-02 | +6.6 | -14.6 | ±3.7 | ±3.5 | ±1.2 | 4.985E-02 | 2.590E-02 |
| 123.00 | 7.552E-02 | +6.6 | -14.8 | ±3.7 | ±3.5 | ±1.2 | 4.972E-02 | 2.584E-02 |
| 123.50 | 7.523E-02 | +6.6 | -14.9 | ±3.7 | ±3.5 | ±1.2 | 4.947E-02 | 2.575E-02 |
| 124.00 | 7.499E-02 | +6.6 | -15.1 | ±3.7 | ±3.5 | ±1.2 | 4.930E-02 | 2.560E-02 |
| 124.10 | 7.471E-02 | +6.6 | -14.6 | ±3.7 | ±3.5 | ±1.2 | 4.935E-02 | 2.559E-02 |
| 124.20 | 7.477E-02 | +6.6 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 4.925E-02 | 2.558E-02 |
| 124.30 | 7.481E-02 | +6.5 | -14.9 | ±3.7 | ±3.5 | ±1.2 | 4.915E-02 | 2.556E-02 |
| 124.40 | 7.477E-02 | +6.6 | -14.9 | ±3.7 | ±3.5 | ±1.2 | 4.918E-02 | 2.557E-02 |
| 124.50 | 7.459E-02 | +6.6 | -14.9 | ±3.7 | ±3.5 | ±1.2 | 4.914E-02 | 2.553E-02 |
| 124.60 | 7.452E-02 | +6.6 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 4.904E-02 | 2.549E-02 |
| 124.70 | 7.448E-02 | +6.6 | -14.8 | ±3.7 | ±3.5 | ±1.2 | 4.901E-02 | 2.549E-02 |
| 124.80 | 7.448E-02 | +6.6 | -14.9 | ±3.7 | ±3.5 | ±1.2 | 4.898E-02 | 2.546E-02 |
| 124.90 | 7.447E-02 | +6.6 | -15.1 | ±3.7 | ±3.6 | ±1.2 | 4.894E-02 | 2.542E-02 |
| 125.00 | 7.425E-02 | +6.5 | -14.9 | ±3.7 | ±3.5 | ±1.2 | 4.889E-02 | 2.542E-02 |
| 125.09 | 7.426E-02 | +6.5 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 4.889E-02 | 2.540E-02 |
| 125.10 | 7.426E-02 | +6.5 | -14.7 | ±3.7 | ±3.5 | ±1.2 | 4.889E-02 | 2.540E-02 |
| 125.20 | 7.432E-02 | +6.5 | -15.0 | ±3.7 | ±3.5 | ±1.2 | 4.887E-02 | 2.540E-02 |
| 125.30 | 7.430E-02 | +6.6 | -14.9 | ±3.8 | ±3.6 | ±1.2 | 4.881E-02 | 2.538E-02 |
| 125.40 | 7.414E-02 | +6.6 | -14.9 | ±3.7 | ±3.6 | ±1.2 | 4.879E-02 | 2.534E-02 |
| 125.50 | 7.407E-02 | +6.6 | -15.0 | ±3.7 | ±3.5 | ±1.2 | 4.877E-02 | 2.534E-02 |
| 125.60 | 7.409E-02 | +6.5 | -15.2 | ±3.7 | ±3.6 | ±1.2 | 4.875E-02 | 2.532E-02 |
| 125.70 | 7.401E-02 | +6.5 | -15.0 | ±3.7 | ±3.6 | ±1.2 | 4.870E-02 | 2.531E-02 |
| 125.80 | 7.390E-02 | +6.5 | -15.0 | ±3.7 | ±3.6 | ±1.2 | 4.865E-02 | 2.530E-02 |
| 125.90 | 7.370E-02 | +6.6 | -14.8 | ±3.7 | ±3.5 | ±1.2 | 4.857E-02 | 2.530E-02 |
| 126.00 | 7.375E-02 | +6.5 | -15.0 | ±3.7 | ±3.6 | ±1.2 | 4.858E-02 | 2.527E-02 |
| 126.50 | 7.353E-02 | +6.5 | -14.9 | ±3.8 | ±3.6 | ±1.2 | 4.837E-02 | 2.516E-02 |
| 127.00 | 7.329E-02 | +6.5 | -15.1 | ±3.8 | ±3.6 | ±1.2 | 4.820E-02 | 2.511E-02 |
| 127.50 | 7.304E-02 | +6.5 | -15.1 | ±3.8 | ±3.6 | ±1.2 | 4.807E-02 | 2.499E-02 |
| 128.00 | 7.277E-02 | +6.5 | -15.1 | ±3.8 | ±3.6 | ±1.2 | 4.793E-02 | 2.491E-02 |
| 128.50 | 7.244E-02 | +6.4 | -15.0 | ±3.8 | ±3.6 | ±1.2 | 4.765E-02 | 2.481E-02 |
| 129.00 | 7.223E-02 | +6.4 | -15.1 | ±3.8 | ±3.6 | ±1.2 | 4.755E-02 | 2.474E-02 |
| 129.50 | 7.203E-02 | +6.4 | -15.2 | ±3.8 | ±3.6 | ±1.2 | 4.734E-02 | 2.466E-02 |
| 130.00 | 7.184E-02 | +6.4 | -15.3 | ±3.8 | ±3.6 | ±1.2 | 4.723E-02 | 2.459E-02 |
tH Process (s-ch)
- 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 | 3.158E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 2.060E-03 | 1.095E-03 |
| 120.50 | 3.124E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 2.042E-03 | 1.083E-03 |
| 121.00 | 3.101E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 2.022E-03 | 1.073E-03 |
| 121.50 | 3.068E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 2.006E-03 | 1.063E-03 |
| 122.00 | 3.045E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 1.989E-03 | 1.052E-03 |
| 122.50 | 3.007E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 1.971E-03 | 1.043E-03 |
| 123.00 | 2.988E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.3 | 1.953E-03 | 1.033E-03 |
| 123.50 | 2.960E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.935E-03 | 1.023E-03 |
| 124.00 | 2.932E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.915E-03 | 1.014E-03 |
| 124.10 | 2.928E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.916E-03 | 1.012E-03 |
| 124.20 | 2.920E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.912E-03 | 1.010E-03 |
| 124.30 | 2.918E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.906E-03 | 1.008E-03 |
| 124.40 | 2.908E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.904E-03 | 1.006E-03 |
| 124.50 | 2.907E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.902E-03 | 1.004E-03 |
| 124.60 | 2.901E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.897E-03 | 1.003E-03 |
| 124.70 | 2.900E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.892E-03 | 1.000E-03 |
| 124.80 | 2.895E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.891E-03 | 9.980E-04 |
| 124.90 | 2.886E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.888E-03 | 9.960E-04 |
| 125.00 | 2.879E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.882E-03 | 9.960E-04 |
| 125.09 | 2.875E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.881E-03 | 9.930E-04 |
| 125.10 | 2.875E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.881E-03 | 9.930E-04 |
| 125.20 | 2.871E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.876E-03 | 9.910E-04 |
| 125.30 | 2.861E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.874E-03 | 9.890E-04 |
| 125.40 | 2.860E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.871E-03 | 9.880E-04 |
| 125.50 | 2.857E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.868E-03 | 9.870E-04 |
| 125.60 | 2.851E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.863E-03 | 9.830E-04 |
| 125.70 | 2.845E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.859E-03 | 9.820E-04 |
| 125.80 | 2.842E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.858E-03 | 9.800E-04 |
| 125.90 | 2.835E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.855E-03 | 9.790E-04 |
| 126.00 | 2.826E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.849E-03 | 9.770E-04 |
| 126.50 | 2.802E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.837E-03 | 9.670E-04 |
| 127.00 | 2.780E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.820E-03 | 9.590E-04 |
| 127.50 | 2.752E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.804E-03 | 9.500E-04 |
| 128.00 | 2.726E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.788E-03 | 9.410E-04 |
| 128.50 | 2.705E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.771E-03 | 9.330E-04 |
| 129.00 | 2.683E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.755E-03 | 9.240E-04 |
| 129.50 | 2.657E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.742E-03 | 9.160E-04 |
| 130.00 | 2.633E-03 | +2.4 | -1.8 | ±2.2 | ±2.2 | ±0.2 | 1.728E-03 | 9.080E-04 |
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