SM Higgs production cross sections at √s = 13 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 |
5.222E+01 |
+4.7 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
4.738E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 120.50 |
5.184E+01 |
+4.7 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
4.704E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 121.00 |
5.146E+01 |
+4.6 |
-6.9 |
±4.0 |
±3.2 |
±1.9 |
±2.6 |
|
4.670E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 121.50 |
5.108E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.637E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 122.00 |
5.071E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.604E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 122.50 |
5.035E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.571E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 123.00 |
4.998E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.539E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
| 123.50 |
4.963E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.507E+01 |
+7.7 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.00 |
4.927E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.476E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.10 |
4.920E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.470E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.20 |
4.913E+01 |
+4.6 |
-6.8 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.463E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.30 |
4.906E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.457E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.40 |
4.899E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.451E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.50 |
4.892E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.445E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.60 |
4.885E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.438E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.70 |
4.878E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.432E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.80 |
4.871E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.426E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 124.90 |
4.864E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.420E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.00 |
4.858E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.414E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.09 |
4.852E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.408E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.10 |
4.851E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.408E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.20 |
4.844E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.402E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.30 |
4.837E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.396E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.40 |
4.830E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.390E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.50 |
4.823E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.383E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.60 |
4.816E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.377E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.70 |
4.810E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.371E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.80 |
4.803E+01 |
+4.6 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.365E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 125.90 |
4.796E+01 |
+4.5 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.359E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 126.00 |
4.789E+01 |
+4.5 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.353E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 126.50 |
4.756E+01 |
+4.5 |
-6.7 |
±3.9 |
±3.2 |
±1.9 |
±2.6 |
|
4.324E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 127.00 |
4.723E+01 |
+4.5 |
-6.7 |
±3.8 |
±3.2 |
±1.9 |
±2.6 |
|
4.294E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 127.50 |
4.690E+01 |
+4.5 |
-6.6 |
±3.8 |
±3.2 |
±1.9 |
±2.6 |
|
4.265E+01 |
+7.5 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 128.00 |
4.658E+01 |
+4.5 |
-6.6 |
±3.8 |
±3.2 |
±1.9 |
±2.6 |
|
4.236E+01 |
+7.5 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
| 128.50 |
4.625E+01 |
+4.5 |
-6.6 |
±3.8 |
±3.2 |
±1.9 |
±2.6 |
|
4.207E+01 |
+7.5 |
-8.0 |
±3.1 |
±1.8 |
±2.5 |
| 129.00 |
4.594E+01 |
+4.5 |
-6.6 |
±3.8 |
±3.2 |
±1.9 |
±2.6 |
|
4.179E+01 |
+7.5 |
-8.0 |
±3.1 |
±1.8 |
±2.5 |
| 129.50 |
4.562E+01 |
+4.5 |
-6.6 |
±3.8 |
±3.2 |
±1.9 |
±2.6 |
|
4.151E+01 |
+7.5 |
-8.0 |
±3.1 |
±1.8 |
±2.5 |
| 130.00 |
4.531E+01 |
+4.5 |
-6.6 |
±3.8 |
±3.2 |
±1.8 |
±2.6 |
|
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).
- 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 |
3.935E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 120.50 |
3.919E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 121.00 |
3.904E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 121.50 |
3.888E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 122.00 |
3.873E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 122.50 |
3.858E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 123.00 |
3.842E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 123.50 |
3.827E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.00 |
3.812E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.10 |
3.809E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.20 |
3.806E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.30 |
3.803E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.40 |
3.800E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.50 |
3.797E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.60 |
3.794E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.70 |
3.791E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.80 |
3.788E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 124.90 |
3.785E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.00 |
3.782E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.09 |
3.779E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.10 |
3.779E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.20 |
3.776E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.30 |
3.773E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.40 |
3.770E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.50 |
3.767E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.60 |
3.764E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.70 |
3.761E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.80 |
3.758E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 125.90 |
3.755E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 126.00 |
3.752E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 126.50 |
3.738E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 127.00 |
3.723E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 127.50 |
3.708E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 128.00 |
3.694E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 128.50 |
3.680E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 129.00 |
3.665E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 129.50 |
3.651E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
| 130.00 |
3.637E+00 |
+0.4 |
-0.3 |
±2.1 |
±2.1 |
±0.5 |
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 |
1.565E+00 |
+0.5 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
9.558E-01 |
6.092E-01 |
| 120.50 |
1.545E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
9.439E-01 |
6.007E-01 |
| 121.00 |
1.524E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
9.320E-01 |
5.925E-01 |
| 121.50 |
1.505E+00 |
+0.4 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
9.201E-01 |
5.845E-01 |
| 122.00 |
1.486E+00 |
+0.4 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
9.091E-01 |
5.765E-01 |
| 122.50 |
1.466E+00 |
+0.5 |
-0.8 |
±1.9 |
±1.7 |
±0.9 |
8.971E-01 |
5.693E-01 |
| 123.00 |
1.446E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.843E-01 |
5.618E-01 |
| 123.50 |
1.427E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.725E-01 |
5.544E-01 |
| 124.00 |
1.408E+00 |
+0.6 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
8.611E-01 |
5.466E-01 |
| 124.10 |
1.405E+00 |
+0.5 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
8.591E-01 |
5.455E-01 |
| 124.20 |
1.401E+00 |
+0.5 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
8.569E-01 |
5.439E-01 |
| 124.30 |
1.398E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.548E-01 |
5.429E-01 |
| 124.40 |
1.394E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.527E-01 |
5.415E-01 |
| 124.50 |
1.390E+00 |
+0.6 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
8.500E-01 |
5.395E-01 |
| 124.60 |
1.387E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.487E-01 |
5.386E-01 |
| 124.70 |
1.383E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.462E-01 |
5.372E-01 |
| 124.80 |
1.380E+00 |
+0.5 |
-0.8 |
±1.9 |
±1.7 |
±0.9 |
8.442E-01 |
5.360E-01 |
| 124.90 |
1.376E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.419E-01 |
5.345E-01 |
| 125.00 |
1.373E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.400E-01 |
5.328E-01 |
| 125.09 |
1.369E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.380E-01 |
5.313E-01 |
| 125.10 |
1.369E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.377E-01 |
5.313E-01 |
| 125.20 |
1.365E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.355E-01 |
5.298E-01 |
| 125.30 |
1.362E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.334E-01 |
5.282E-01 |
| 125.40 |
1.358E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.313E-01 |
5.272E-01 |
| 125.50 |
1.355E+00 |
+0.5 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.291E-01 |
5.259E-01 |
| 125.60 |
1.351E+00 |
+0.5 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
8.270E-01 |
5.243E-01 |
| 125.70 |
1.347E+00 |
+0.5 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
8.243E-01 |
5.230E-01 |
| 125.80 |
1.344E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.224E-01 |
5.217E-01 |
| 125.90 |
1.341E+00 |
+0.5 |
-0.8 |
±1.9 |
±1.7 |
±0.9 |
8.211E-01 |
5.202E-01 |
| 126.00 |
1.337E+00 |
+0.6 |
-0.8 |
±1.9 |
±1.7 |
±0.9 |
8.184E-01 |
5.187E-01 |
| 126.50 |
1.320E+00 |
+0.6 |
-0.7 |
±1.9 |
±1.7 |
±0.9 |
8.080E-01 |
5.123E-01 |
| 127.00 |
1.304E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.987E-01 |
5.051E-01 |
| 127.50 |
1.287E+00 |
+0.6 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.879E-01 |
4.988E-01 |
| 128.00 |
1.271E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.785E-01 |
4.924E-01 |
| 128.50 |
1.255E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.687E-01 |
4.862E-01 |
| 129.00 |
1.239E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.593E-01 |
4.801E-01 |
| 129.50 |
1.224E+00 |
+0.5 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.501E-01 |
4.738E-01 |
| 130.00 |
1.209E+00 |
+0.4 |
-0.7 |
±1.8 |
±1.7 |
±0.9 |
7.414E-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 |
1.069E-01 |
+0.6 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.16E-03 |
6.817E-02 |
+0.4 |
-0.6 |
±1.9 |
±1.7 |
±0.9 |
2.05E-03 |
| 120.50 |
1.056E-01 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.15E-03 |
6.725E-02 |
+0.5 |
-0.6 |
±1.9 |
±1.7 |
±0.8 |
2.05E-03 |
| 121.00 |
1.043E-01 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.15E-03 |
6.635E-02 |
+0.5 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
2.04E-03 |
| 121.50 |
1.030E-01 |
+0.4 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.14E-03 |
6.548E-02 |
+0.5 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
2.04E-03 |
| 122.00 |
1.018E-01 |
+0.3 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.13E-03 |
6.460E-02 |
+0.6 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
2.03E-03 |
| 122.50 |
1.005E-01 |
+0.5 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.13E-03 |
6.382E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.03E-03 |
| 123.00 |
9.910E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.12E-03 |
6.299E-02 |
+0.5 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.02E-03 |
| 123.50 |
9.781E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.11E-03 |
6.219E-02 |
+0.5 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.02E-03 |
| 124.00 |
9.657E-02 |
+0.6 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.11E-03 |
6.133E-02 |
+0.6 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.10 |
9.634E-02 |
+0.5 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.122E-02 |
+0.5 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.20 |
9.610E-02 |
+0.5 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.104E-02 |
+0.5 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.30 |
9.588E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.093E-02 |
+0.5 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.40 |
9.565E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.078E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.50 |
9.536E-02 |
+0.6 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.057E-02 |
+0.6 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.60 |
9.521E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.047E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.70 |
9.494E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.10E-03 |
6.031E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.80 |
9.471E-02 |
+0.6 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
6.018E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 124.90 |
9.447E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
6.002E-02 |
+0.3 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.01E-03 |
| 125.00 |
9.426E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.983E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.09 |
9.404E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.967E-02 |
+0.4 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.10 |
9.401E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.966E-02 |
+0.4 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.20 |
9.377E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.950E-02 |
+0.5 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.30 |
9.354E-02 |
+0.6 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.933E-02 |
+0.5 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.40 |
9.331E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.922E-02 |
+0.5 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.50 |
9.308E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.09E-03 |
5.908E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.60 |
9.284E-02 |
+0.5 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.08E-03 |
5.891E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.70 |
9.254E-02 |
+0.6 |
-0.6 |
±1.8 |
±1.6 |
±0.9 |
3.08E-03 |
5.876E-02 |
+0.3 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.80 |
9.234E-02 |
+0.7 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.08E-03 |
5.862E-02 |
+0.4 |
-0.8 |
±2.0 |
±1.8 |
±0.8 |
2.00E-03 |
| 125.90 |
9.220E-02 |
+0.6 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.08E-03 |
5.845E-02 |
+0.4 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
1.99E-03 |
| 126.00 |
9.191E-02 |
+0.6 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.08E-03 |
5.829E-02 |
+0.5 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
1.99E-03 |
| 126.50 |
9.077E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.07E-03 |
5.759E-02 |
+0.5 |
-0.7 |
±2.0 |
±1.8 |
±0.8 |
1.99E-03 |
| 127.00 |
8.975E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.06E-03 |
5.680E-02 |
+0.5 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
1.98E-03 |
| 127.50 |
8.858E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.06E-03 |
5.612E-02 |
+0.5 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
1.98E-03 |
| 128.00 |
8.754E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.05E-03 |
5.541E-02 |
+0.4 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
1.97E-03 |
| 128.50 |
8.647E-02 |
+0.6 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.04E-03 |
5.474E-02 |
+0.4 |
-0.7 |
±1.9 |
±1.8 |
±0.8 |
1.97E-03 |
| 129.00 |
8.545E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.04E-03 |
5.407E-02 |
+0.4 |
-0.7 |
±1.9 |
±1.8 |
±0.8 |
1.96E-03 |
| 129.50 |
8.444E-02 |
+0.5 |
-0.7 |
±1.8 |
±1.6 |
±0.9 |
3.03E-03 |
5.338E-02 |
+0.5 |
-0.7 |
±1.9 |
±1.8 |
±0.8 |
1.96E-03 |
| 130.00 |
8.349E-02 |
+0.4 |
-0.8 |
±1.8 |
±1.6 |
±0.9 |
3.02E-03 |
5.270E-02 |
+0.5 |
-0.6 |
±1.9 |
±1.8 |
±0.8 |
1.95E-03 |
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 |
9.939E-01 |
+3.4 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
1.299E-01 |
| 120.50 |
9.829E-01 |
+3.4 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
1.292E-01 |
| 121.00 |
9.705E-01 |
+3.5 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
1.281E-01 |
| 121.50 |
9.591E-01 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
1.269E-01 |
| 122.00 |
9.485E-01 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
1.271E-01 |
| 122.50 |
9.371E-01 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.265E-01 |
| 123.00 |
9.266E-01 |
+3.6 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.254E-01 |
| 123.50 |
9.157E-01 |
+3.5 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.250E-01 |
| 124.00 |
9.051E-01 |
+3.6 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.242E-01 |
| 124.10 |
9.037E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.242E-01 |
| 124.20 |
9.008E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.241E-01 |
| 124.30 |
8.988E-01 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.239E-01 |
| 124.40 |
8.964E-01 |
+3.7 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.236E-01 |
| 124.50 |
8.943E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.235E-01 |
| 124.60 |
8.923E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.233E-01 |
| 124.70 |
8.902E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.235E-01 |
| 124.80 |
8.884E-01 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.230E-01 |
| 124.90 |
8.858E-01 |
+3.9 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.227E-01 |
| 125.00 |
8.839E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.227E-01 |
| 125.09 |
8.824E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.227E-01 |
| 125.10 |
8.819E-01 |
+3.9 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.226E-01 |
| 125.20 |
8.800E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.223E-01 |
| 125.30 |
8.783E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.224E-01 |
| 125.40 |
8.767E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.223E-01 |
| 125.50 |
8.744E-01 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.221E-01 |
| 125.60 |
8.728E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.224E-01 |
| 125.70 |
8.703E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
1.218E-01 |
| 125.80 |
8.690E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.219E-01 |
| 125.90 |
8.668E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.218E-01 |
| 126.00 |
8.649E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.218E-01 |
| 126.50 |
8.549E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.211E-01 |
| 127.00 |
8.446E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.203E-01 |
| 127.50 |
8.350E-01 |
+3.8 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.197E-01 |
| 128.00 |
8.255E-01 |
+3.9 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
1.190E-01 |
| 128.50 |
8.161E-01 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.180E-01 |
| 129.00 |
8.073E-01 |
+3.8 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.177E-01 |
| 129.50 |
7.980E-01 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
1.171E-01 |
| 130.00 |
7.899E-01 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
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 |
3.352E-02 |
+3.4 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
4.38E-03 |
1.10E-04 |
1.997E-01 |
+3.4 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
2.600E-02 |
0.00E+00 |
| 120.50 |
3.315E-02 |
+3.4 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
4.36E-03 |
1.10E-04 |
1.975E-01 |
+3.4 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
2.585E-02 |
0.00E+00 |
| 121.00 |
3.273E-02 |
+3.5 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
4.32E-03 |
1.10E-04 |
1.950E-01 |
+3.5 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
2.564E-02 |
0.00E+00 |
| 121.50 |
3.235E-02 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
4.28E-03 |
1.10E-04 |
1.927E-01 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
2.540E-02 |
0.00E+00 |
| 122.00 |
3.199E-02 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
4.29E-03 |
1.10E-04 |
1.906E-01 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±1.0 |
2.545E-02 |
0.00E+00 |
| 122.50 |
3.161E-02 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.27E-03 |
1.10E-04 |
1.883E-01 |
+3.6 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.531E-02 |
0.00E+00 |
| 123.00 |
3.125E-02 |
+3.6 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.23E-03 |
1.10E-04 |
1.862E-01 |
+3.6 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.510E-02 |
0.00E+00 |
| 123.50 |
3.089E-02 |
+3.5 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.22E-03 |
1.10E-04 |
1.840E-01 |
+3.5 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.502E-02 |
0.00E+00 |
| 124.00 |
3.053E-02 |
+3.6 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.19E-03 |
1.10E-04 |
1.819E-01 |
+3.6 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.486E-02 |
0.00E+00 |
| 124.10 |
3.048E-02 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
4.19E-03 |
1.10E-04 |
1.816E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.487E-02 |
0.00E+00 |
| 124.20 |
3.039E-02 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.19E-03 |
1.10E-04 |
1.810E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.482E-02 |
0.00E+00 |
| 124.30 |
3.032E-02 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.18E-03 |
1.10E-04 |
1.806E-01 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.480E-02 |
0.00E+00 |
| 124.40 |
3.024E-02 |
+3.7 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.17E-03 |
1.10E-04 |
1.801E-01 |
+3.7 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.474E-02 |
0.00E+00 |
| 124.50 |
3.017E-02 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.17E-03 |
1.10E-04 |
1.797E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.471E-02 |
0.00E+00 |
| 124.60 |
3.010E-02 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.16E-03 |
1.10E-04 |
1.793E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.467E-02 |
0.00E+00 |
| 124.70 |
3.003E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.17E-03 |
1.10E-04 |
1.789E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.470E-02 |
0.00E+00 |
| 124.80 |
2.997E-02 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.15E-03 |
1.10E-04 |
1.785E-01 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.461E-02 |
0.00E+00 |
| 124.90 |
2.988E-02 |
+3.9 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.14E-03 |
1.10E-04 |
1.780E-01 |
+3.9 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.458E-02 |
0.00E+00 |
| 125.00 |
2.982E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.14E-03 |
1.10E-04 |
1.776E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.457E-02 |
0.00E+00 |
| 125.09 |
2.977E-02 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.14E-03 |
1.10E-04 |
1.773E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.455E-02 |
0.00E+00 |
| 125.10 |
2.975E-02 |
+3.9 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.14E-03 |
1.10E-04 |
1.772E-01 |
+3.9 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.454E-02 |
0.00E+00 |
| 125.20 |
2.969E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.13E-03 |
1.10E-04 |
1.768E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.447E-02 |
0.00E+00 |
| 125.30 |
2.963E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.13E-03 |
1.10E-04 |
1.765E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.448E-02 |
0.00E+00 |
| 125.40 |
2.957E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.13E-03 |
1.10E-04 |
1.762E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.446E-02 |
0.00E+00 |
| 125.50 |
2.950E-02 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.12E-03 |
1.10E-04 |
1.757E-01 |
+3.7 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.444E-02 |
0.00E+00 |
| 125.60 |
2.944E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.13E-03 |
1.10E-04 |
1.754E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.448E-02 |
0.00E+00 |
| 125.70 |
2.936E-02 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
4.11E-03 |
1.10E-04 |
1.749E-01 |
+3.8 |
-3.0 |
±1.6 |
±1.3 |
±0.9 |
2.436E-02 |
0.00E+00 |
| 125.80 |
2.932E-02 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
4.11E-03 |
1.10E-04 |
1.746E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.440E-02 |
0.00E+00 |
| 125.90 |
2.924E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.11E-03 |
1.10E-04 |
1.742E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.436E-02 |
0.00E+00 |
| 126.00 |
2.918E-02 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.11E-03 |
1.10E-04 |
1.738E-01 |
+3.8 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.437E-02 |
0.00E+00 |
| 126.50 |
2.884E-02 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
4.09E-03 |
1.10E-04 |
1.718E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.423E-02 |
0.00E+00 |
| 127.00 |
2.850E-02 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
4.06E-03 |
1.10E-04 |
1.697E-01 |
+3.7 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.407E-02 |
0.00E+00 |
| 127.50 |
2.817E-02 |
+3.8 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
4.04E-03 |
1.10E-04 |
1.678E-01 |
+3.8 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.394E-02 |
0.00E+00 |
| 128.00 |
2.785E-02 |
+3.9 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
4.02E-03 |
1.10E-04 |
1.659E-01 |
+3.9 |
-3.1 |
±1.6 |
±1.3 |
±0.9 |
2.381E-02 |
0.00E+00 |
| 128.50 |
2.754E-02 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
3.98E-03 |
1.10E-04 |
1.640E-01 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.362E-02 |
0.00E+00 |
| 129.00 |
2.724E-02 |
+3.8 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
3.97E-03 |
1.00E-04 |
1.622E-01 |
+3.8 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.355E-02 |
0.00E+00 |
| 129.50 |
2.693E-02 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
3.95E-03 |
1.00E-04 |
1.603E-01 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.344E-02 |
0.00E+00 |
| 130.00 |
2.665E-02 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
3.93E-03 |
1.00E-04 |
1.587E-01 |
+3.9 |
-3.2 |
±1.6 |
±1.3 |
±0.9 |
2.329E-02 |
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 |
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). 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 |
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 |
--
ReiTanaka - 2016-03-01
This topic: LHCPhysics
> LHCHXSWG > CERNYellowReportPageAt13TeV
Topic revision: r20 - 2016-12-08 - MarcoPieri
Copyright &© 2008-2021 by the contributing authors. All material on this collaboration platform is the property of the contributing authors.