SM Higgs production cross sections at √s = 7 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 |
1.831E+01 |
+4.5 |
-7.1 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.661E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 120.50 |
1.816E+01 |
+4.5 |
-7.1 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.647E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 121.00 |
1.800E+01 |
+4.5 |
-7.1 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.634E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 121.50 |
1.785E+01 |
+4.5 |
-7.1 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.620E+01 |
+7.4 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 122.00 |
1.771E+01 |
+4.5 |
-7.1 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.607E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 122.50 |
1.756E+01 |
+4.5 |
-7.0 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.594E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 123.00 |
1.741E+01 |
+4.5 |
-7.0 |
±4.1 |
±3.3 |
±1.9 |
±2.7 |
|
1.581E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 123.50 |
1.727E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.568E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.00 |
1.713E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.556E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.10 |
1.710E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.553E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.20 |
1.707E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.551E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.30 |
1.704E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.548E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.40 |
1.702E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.546E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.50 |
1.699E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.543E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.60 |
1.696E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.541E+01 |
+7.3 |
-8.0 |
±3.2 |
±1.8 |
±2.6 |
| 124.70 |
1.693E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.538E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 124.80 |
1.690E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.536E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 124.90 |
1.688E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.533E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.00 |
1.685E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.531E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.09 |
1.682E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.529E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.10 |
1.682E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.528E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.20 |
1.679E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.526E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.30 |
1.677E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.523E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.40 |
1.674E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.521E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.50 |
1.671E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.519E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.60 |
1.668E+01 |
+4.4 |
-7.0 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.516E+01 |
+7.3 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.70 |
1.666E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.514E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.80 |
1.663E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.511E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 125.90 |
1.660E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.509E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 126.00 |
1.658E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.507E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 126.50 |
1.644E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.495E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 127.00 |
1.631E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.483E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 127.50 |
1.618E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.471E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 128.00 |
1.605E+01 |
+4.4 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.460E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 128.50 |
1.592E+01 |
+4.3 |
-6.9 |
±4.0 |
±3.3 |
±1.9 |
±2.7 |
|
1.448E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 129.00 |
1.580E+01 |
+4.3 |
-6.8 |
±3.9 |
±3.3 |
±1.9 |
±2.7 |
|
1.437E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 129.50 |
1.567E+01 |
+4.3 |
-6.8 |
±3.9 |
±3.3 |
±1.9 |
±2.7 |
|
1.426E+01 |
+7.2 |
-7.9 |
±3.2 |
±1.8 |
±2.6 |
| 130.00 |
1.555E+01 |
+4.3 |
-6.8 |
±3.9 |
±3.3 |
±1.9 |
±2.7 |
|
1.415E+01 |
+7.1 |
-7.8 |
±3.2 |
±1.8 |
±2.6 |
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 |
1.302E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 120.50 |
1.296E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 121.00 |
1.289E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 121.50 |
1.283E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 122.00 |
1.277E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 122.50 |
1.271E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 123.00 |
1.265E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 123.50 |
1.259E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.00 |
1.253E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.10 |
1.252E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.20 |
1.251E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.30 |
1.250E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.40 |
1.249E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.50 |
1.247E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.60 |
1.246E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.70 |
1.245E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.80 |
1.244E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 124.90 |
1.243E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.00 |
1.241E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.09 |
1.240E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.10 |
1.240E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.20 |
1.239E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.30 |
1.238E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.40 |
1.237E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.50 |
1.236E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.60 |
1.235E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.70 |
1.233E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.80 |
1.232E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 125.90 |
1.231E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 126.00 |
1.230E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 126.50 |
1.224E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 127.00 |
1.218E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 127.50 |
1.213E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 128.00 |
1.207E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 128.50 |
1.201E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 129.00 |
1.196E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 129.50 |
1.190E+00 |
+0.2 |
-0.2 |
±2.2 |
±2.1 |
±0.4 |
| 130.00 |
1.185E+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 |
6.625E-01 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
4.233E-01 |
2.392E-01 |
| 120.50 |
6.532E-01 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
4.176E-01 |
2.357E-01 |
| 121.00 |
6.439E-01 |
+0.7 |
-0.9 |
±2.0 |
±2.0 |
±0.6 |
4.116E-01 |
2.324E-01 |
| 121.50 |
6.349E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
4.059E-01 |
2.291E-01 |
| 122.00 |
6.264E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
4.006E-01 |
2.258E-01 |
| 122.50 |
6.180E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.954E-01 |
2.226E-01 |
| 123.00 |
6.097E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.900E-01 |
2.197E-01 |
| 123.50 |
6.012E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.846E-01 |
2.166E-01 |
| 124.00 |
5.931E-01 |
+0.6 |
-0.8 |
±2.1 |
±2.0 |
±0.7 |
3.795E-01 |
2.136E-01 |
| 124.10 |
5.915E-01 |
+0.6 |
-0.8 |
±2.1 |
±2.0 |
±0.7 |
3.785E-01 |
2.130E-01 |
| 124.20 |
5.899E-01 |
+0.6 |
-0.8 |
±2.1 |
±2.0 |
±0.7 |
3.774E-01 |
2.125E-01 |
| 124.30 |
5.883E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.766E-01 |
2.117E-01 |
| 124.40 |
5.867E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.756E-01 |
2.111E-01 |
| 124.50 |
5.853E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.746E-01 |
2.107E-01 |
| 124.60 |
5.838E-01 |
+0.6 |
-1.0 |
±2.1 |
±2.0 |
±0.7 |
3.738E-01 |
2.100E-01 |
| 124.70 |
5.820E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.726E-01 |
2.094E-01 |
| 124.80 |
5.804E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.716E-01 |
2.088E-01 |
| 124.90 |
5.788E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.706E-01 |
2.082E-01 |
| 125.00 |
5.771E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.696E-01 |
2.076E-01 |
| 125.09 |
5.756E-01 |
+0.7 |
-0.8 |
±2.1 |
±2.0 |
±0.7 |
3.685E-01 |
2.070E-01 |
| 125.10 |
5.756E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.686E-01 |
2.069E-01 |
| 125.20 |
5.740E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.677E-01 |
2.063E-01 |
| 125.30 |
5.725E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.667E-01 |
2.058E-01 |
| 125.40 |
5.708E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.656E-01 |
2.052E-01 |
| 125.50 |
5.694E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.648E-01 |
2.046E-01 |
| 125.60 |
5.679E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.638E-01 |
2.041E-01 |
| 125.70 |
5.665E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.629E-01 |
2.035E-01 |
| 125.80 |
5.650E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.619E-01 |
2.031E-01 |
| 125.90 |
5.633E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.608E-01 |
2.025E-01 |
| 126.00 |
5.618E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.599E-01 |
2.019E-01 |
| 126.50 |
5.542E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.551E-01 |
1.991E-01 |
| 127.00 |
5.469E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.505E-01 |
1.964E-01 |
| 127.50 |
5.395E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.7 |
3.459E-01 |
1.937E-01 |
| 128.00 |
5.323E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.414E-01 |
1.909E-01 |
| 128.50 |
5.253E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.368E-01 |
1.884E-01 |
| 129.00 |
5.182E-01 |
+0.7 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.324E-01 |
1.857E-01 |
| 129.50 |
5.116E-01 |
+0.6 |
-1.0 |
±2.1 |
±2.0 |
±0.6 |
3.283E-01 |
1.834E-01 |
| 130.00 |
5.046E-01 |
+0.6 |
-0.9 |
±2.1 |
±2.0 |
±0.6 |
3.240E-01 |
1.807E-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 |
4.685E-02 |
+0.6 |
-0.9 |
±1.9 |
±1.8 |
±0.6 |
9.10E-04 |
2.648E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.20E-04 |
| 120.50 |
4.622E-02 |
+0.6 |
-1.0 |
±1.9 |
±1.8 |
±0.6 |
9.00E-04 |
2.610E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.20E-04 |
| 121.00 |
4.557E-02 |
+0.7 |
-0.9 |
±1.9 |
±1.9 |
±0.6 |
9.00E-04 |
2.574E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.20E-04 |
| 121.50 |
4.495E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
9.00E-04 |
2.538E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.20E-04 |
| 122.00 |
4.438E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
9.00E-04 |
2.503E-02 |
+0.7 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.20E-04 |
| 122.50 |
4.380E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.90E-04 |
2.468E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.20E-04 |
| 123.00 |
4.322E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.90E-04 |
2.435E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 123.50 |
4.263E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.90E-04 |
2.402E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.00 |
4.207E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.369E-02 |
+0.5 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.10 |
4.196E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.363E-02 |
+0.5 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.20 |
4.184E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.357E-02 |
+0.5 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.30 |
4.175E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.349E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.40 |
4.165E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.342E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.50 |
4.154E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.338E-02 |
+0.5 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.60 |
4.145E-02 |
+0.6 |
-1.0 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.330E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.70 |
4.132E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.324E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.80 |
4.121E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.317E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 124.90 |
4.110E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.311E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.00 |
4.099E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.304E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.09 |
4.088E-02 |
+0.7 |
-0.8 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.298E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.10 |
4.089E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.297E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.20 |
4.079E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.290E-02 |
+0.7 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.30 |
4.068E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.285E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.40 |
4.056E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.278E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.50 |
4.047E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.80E-04 |
2.272E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.60 |
4.036E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.266E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.2 |
±0.6 |
5.10E-04 |
| 125.70 |
4.026E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.259E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.2 |
±0.6 |
5.00E-04 |
| 125.80 |
4.015E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.254E-02 |
+0.6 |
-0.8 |
±2.3 |
±2.3 |
±0.6 |
5.00E-04 |
| 125.90 |
4.003E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.248E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.3 |
±0.6 |
5.00E-04 |
| 126.00 |
3.993E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.241E-02 |
+0.7 |
-0.8 |
±2.3 |
±2.3 |
±0.6 |
5.00E-04 |
| 126.50 |
3.941E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.211E-02 |
+0.6 |
-0.9 |
±2.3 |
±2.3 |
±0.6 |
5.00E-04 |
| 127.00 |
3.891E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.70E-04 |
2.182E-02 |
+0.6 |
-1.0 |
±2.3 |
±2.3 |
±0.6 |
5.00E-04 |
| 127.50 |
3.840E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.7 |
8.60E-04 |
2.152E-02 |
+0.6 |
-0.9 |
±2.4 |
±2.3 |
±0.6 |
5.00E-04 |
| 128.00 |
3.791E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.60E-04 |
2.122E-02 |
+0.7 |
-0.9 |
±2.4 |
±2.3 |
±0.6 |
5.00E-04 |
| 128.50 |
3.742E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.60E-04 |
2.094E-02 |
+0.7 |
-0.9 |
±2.4 |
±2.3 |
±0.6 |
4.90E-04 |
| 129.00 |
3.694E-02 |
+0.7 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.60E-04 |
2.065E-02 |
+0.6 |
-0.9 |
±2.4 |
±2.3 |
±0.6 |
4.90E-04 |
| 129.50 |
3.648E-02 |
+0.6 |
-1.0 |
±2.0 |
±1.9 |
±0.6 |
8.50E-04 |
2.039E-02 |
+0.6 |
-0.9 |
±2.4 |
±2.3 |
±0.6 |
4.90E-04 |
| 130.00 |
3.601E-02 |
+0.6 |
-0.9 |
±2.0 |
±1.9 |
±0.6 |
8.50E-04 |
2.010E-02 |
+0.7 |
-0.9 |
±2.4 |
±2.3 |
±0.6 |
4.90E-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 |
3.851E-01 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
2.961E-02 |
| 120.50 |
3.803E-01 |
+2.4 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
2.938E-02 |
| 121.00 |
3.755E-01 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
2.931E-02 |
| 121.50 |
3.705E-01 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
2.909E-02 |
| 122.00 |
3.657E-01 |
+2.6 |
-2.1 |
±1.7 |
±1.6 |
±0.7 |
2.896E-02 |
| 122.50 |
3.612E-01 |
+2.6 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
2.876E-02 |
| 123.00 |
3.563E-01 |
+2.7 |
-2.1 |
±1.7 |
±1.6 |
±0.7 |
2.851E-02 |
| 123.50 |
3.518E-01 |
+2.6 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
2.841E-02 |
| 124.00 |
3.478E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.839E-02 |
| 124.10 |
3.470E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.822E-02 |
| 124.20 |
3.461E-01 |
+2.5 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.822E-02 |
| 124.30 |
3.452E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.817E-02 |
| 124.40 |
3.444E-01 |
+2.5 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.817E-02 |
| 124.50 |
3.434E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.814E-02 |
| 124.60 |
3.426E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.814E-02 |
| 124.70 |
3.417E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.809E-02 |
| 124.80 |
3.408E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.792E-02 |
| 124.90 |
3.401E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.792E-02 |
| 125.00 |
3.392E-01 |
+2.6 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
2.789E-02 |
| 125.09 |
3.384E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.792E-02 |
| 125.10 |
3.383E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.789E-02 |
| 125.20 |
3.375E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.789E-02 |
| 125.30 |
3.366E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.787E-02 |
| 125.40 |
3.357E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.784E-02 |
| 125.50 |
3.348E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.782E-02 |
| 125.60 |
3.339E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.782E-02 |
| 125.70 |
3.333E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.782E-02 |
| 125.80 |
3.325E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.779E-02 |
| 125.90 |
3.315E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.762E-02 |
| 126.00 |
3.307E-01 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.760E-02 |
| 126.50 |
3.265E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.752E-02 |
| 127.00 |
3.225E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.730E-02 |
| 127.50 |
3.185E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.722E-02 |
| 128.00 |
3.146E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.697E-02 |
| 128.50 |
3.109E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.690E-02 |
| 129.00 |
3.071E-01 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
2.665E-02 |
| 129.50 |
3.033E-01 |
+2.7 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
2.645E-02 |
| 130.00 |
2.996E-01 |
+2.7 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
2.635E-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 |
1.297E-02 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
1.00E-03 |
3.00E-05 |
7.740E-02 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
5.92E-03 |
0.00E+00 |
| 120.50 |
1.281E-02 |
+2.4 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
9.90E-04 |
3.00E-05 |
7.643E-02 |
+2.4 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
5.89E-03 |
0.00E+00 |
| 121.00 |
1.265E-02 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
9.90E-04 |
3.00E-05 |
7.546E-02 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
5.86E-03 |
0.00E+00 |
| 121.50 |
1.248E-02 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
9.80E-04 |
3.00E-05 |
7.448E-02 |
+2.5 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
5.83E-03 |
0.00E+00 |
| 122.00 |
1.232E-02 |
+2.6 |
-2.1 |
±1.7 |
±1.6 |
±0.7 |
9.80E-04 |
3.00E-05 |
7.351E-02 |
+2.6 |
-2.1 |
±1.7 |
±1.6 |
±0.7 |
5.78E-03 |
0.00E+00 |
| 122.50 |
1.217E-02 |
+2.6 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
9.70E-04 |
3.00E-05 |
7.259E-02 |
+2.6 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
5.76E-03 |
0.00E+00 |
| 123.00 |
1.200E-02 |
+2.7 |
-2.1 |
±1.7 |
±1.6 |
±0.7 |
9.60E-04 |
3.00E-05 |
7.162E-02 |
+2.7 |
-2.1 |
±1.7 |
±1.6 |
±0.7 |
5.72E-03 |
0.00E+00 |
| 123.50 |
1.185E-02 |
+2.6 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
9.60E-04 |
3.00E-05 |
7.073E-02 |
+2.6 |
-2.2 |
±1.7 |
±1.6 |
±0.7 |
5.68E-03 |
0.00E+00 |
| 124.00 |
1.172E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.60E-04 |
3.00E-05 |
6.990E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.67E-03 |
0.00E+00 |
| 124.10 |
1.169E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.973E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.66E-03 |
0.00E+00 |
| 124.20 |
1.166E-02 |
+2.5 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.958E-02 |
+2.5 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.66E-03 |
0.00E+00 |
| 124.30 |
1.163E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.937E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.64E-03 |
0.00E+00 |
| 124.40 |
1.160E-02 |
+2.5 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.923E-02 |
+2.5 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.64E-03 |
0.00E+00 |
| 124.50 |
1.157E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.901E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.63E-03 |
0.00E+00 |
| 124.60 |
1.154E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.888E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.63E-03 |
0.00E+00 |
| 124.70 |
1.151E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.50E-04 |
3.00E-05 |
6.869E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.61E-03 |
0.00E+00 |
| 124.80 |
1.148E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.850E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.60E-03 |
0.00E+00 |
| 124.90 |
1.146E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.835E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.60E-03 |
0.00E+00 |
| 125.00 |
1.143E-02 |
+2.6 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.818E-02 |
+2.6 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
5.59E-03 |
0.00E+00 |
| 125.09 |
1.140E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.802E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.60E-03 |
0.00E+00 |
| 125.10 |
1.140E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.800E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.59E-03 |
0.00E+00 |
| 125.20 |
1.137E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.782E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.59E-03 |
0.00E+00 |
| 125.30 |
1.134E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.765E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.58E-03 |
0.00E+00 |
| 125.40 |
1.131E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.749E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.57E-03 |
0.00E+00 |
| 125.50 |
1.128E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.728E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.56E-03 |
0.00E+00 |
| 125.60 |
1.125E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.713E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.56E-03 |
0.00E+00 |
| 125.70 |
1.123E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.697E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.56E-03 |
0.00E+00 |
| 125.80 |
1.120E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.40E-04 |
3.00E-05 |
6.683E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.55E-03 |
0.00E+00 |
| 125.90 |
1.117E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.30E-04 |
3.00E-05 |
6.662E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.54E-03 |
0.00E+00 |
| 126.00 |
1.114E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.30E-04 |
3.00E-05 |
6.648E-02 |
+2.6 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.53E-03 |
0.00E+00 |
| 126.50 |
1.100E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.30E-04 |
3.00E-05 |
6.562E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.50E-03 |
0.00E+00 |
| 127.00 |
1.087E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.20E-04 |
3.00E-05 |
6.482E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.47E-03 |
0.00E+00 |
| 127.50 |
1.073E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.20E-04 |
3.00E-05 |
6.403E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.44E-03 |
0.00E+00 |
| 128.00 |
1.060E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.10E-04 |
3.00E-05 |
6.324E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.40E-03 |
0.00E+00 |
| 128.50 |
1.048E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.10E-04 |
3.00E-05 |
6.248E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.37E-03 |
0.00E+00 |
| 129.00 |
1.035E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
9.00E-04 |
3.00E-05 |
6.172E-02 |
+2.7 |
-2.3 |
±1.7 |
±1.6 |
±0.7 |
5.33E-03 |
0.00E+00 |
| 129.50 |
1.022E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
8.90E-04 |
3.00E-05 |
6.097E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
5.31E-03 |
0.00E+00 |
| 130.00 |
1.010E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
8.90E-04 |
3.00E-05 |
6.022E-02 |
+2.7 |
-2.4 |
±1.7 |
±1.6 |
±0.7 |
5.27E-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 |
1.005E-01 |
+3.6 |
-9.3 |
±4.5 |
±3.9 |
±2.2 |
| 120.50 |
9.936E-02 |
+3.6 |
-9.3 |
±4.5 |
±3.9 |
±2.2 |
| 121.00 |
9.800E-02 |
+3.6 |
-9.3 |
±4.5 |
±3.9 |
±2.2 |
| 121.50 |
9.679E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 122.00 |
9.572E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 122.50 |
9.455E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 123.00 |
9.335E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 123.50 |
9.216E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.00 |
9.107E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.10 |
9.084E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.20 |
9.060E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.30 |
9.042E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.40 |
9.018E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.50 |
9.007E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.60 |
8.972E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.70 |
8.957E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.80 |
8.930E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 124.90 |
8.912E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.00 |
8.878E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.09 |
8.864E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.10 |
8.873E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.20 |
8.841E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.30 |
8.825E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.40 |
8.794E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.50 |
8.783E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.60 |
8.761E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.70 |
8.742E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.80 |
8.714E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 125.90 |
8.703E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 126.00 |
8.674E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 126.50 |
8.571E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 127.00 |
8.477E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 127.50 |
8.369E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 128.00 |
8.262E-02 |
+3.5 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 128.50 |
8.167E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 129.00 |
8.073E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 129.50 |
7.973E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±2.2 |
| 130.00 |
7.882E-02 |
+3.4 |
-9.2 |
±4.5 |
±3.9 |
±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 |
1.782E-01 |
+21.0 |
-22.8 |
| 120.50 |
1.762E-01 |
+21.0 |
-22.8 |
| 121.00 |
1.735E-01 |
+20.9 |
-22.7 |
| 121.50 |
1.710E-01 |
+20.9 |
-22.7 |
| 122.00 |
1.688E-01 |
+20.9 |
-22.7 |
| 122.50 |
1.663E-01 |
+20.8 |
-22.6 |
| 123.00 |
1.634E-01 |
+20.7 |
-22.5 |
| 123.50 |
1.619E-01 |
+20.7 |
-22.5 |
| 124.00 |
1.597E-01 |
+20.8 |
-22.6 |
| 124.10 |
1.591E-01 |
+20.8 |
-22.6 |
| 124.20 |
1.586E-01 |
+20.8 |
-22.6 |
| 124.30 |
1.583E-01 |
+20.8 |
-22.7 |
| 124.40 |
1.579E-01 |
+20.9 |
-22.7 |
| 124.50 |
1.573E-01 |
+20.7 |
-22.5 |
| 124.60 |
1.572E-01 |
+20.8 |
-22.5 |
| 124.70 |
1.564E-01 |
+20.8 |
-22.5 |
| 124.80 |
1.557E-01 |
+20.8 |
-22.6 |
| 124.90 |
1.555E-01 |
+20.8 |
-22.6 |
| 125.00 |
1.552E-01 |
+20.7 |
-22.4 |
| 125.09 |
1.545E-01 |
+20.7 |
-22.5 |
| 125.10 |
1.547E-01 |
+20.8 |
-22.5 |
| 125.20 |
1.543E-01 |
+20.8 |
-22.5 |
| 125.30 |
1.538E-01 |
+20.8 |
-22.5 |
| 125.40 |
1.532E-01 |
+20.8 |
-22.6 |
| 125.50 |
1.527E-01 |
+20.7 |
-22.4 |
| 125.60 |
1.524E-01 |
+20.6 |
-22.4 |
| 125.70 |
1.521E-01 |
+20.7 |
-22.5 |
| 125.80 |
1.514E-01 |
+20.7 |
-22.5 |
| 125.90 |
1.510E-01 |
+20.8 |
-22.5 |
| 126.00 |
1.508E-01 |
+20.7 |
-22.3 |
| 126.50 |
1.486E-01 |
+20.6 |
-22.3 |
| 127.00 |
1.467E-01 |
+20.6 |
-22.3 |
| 127.50 |
1.446E-01 |
+20.5 |
-22.2 |
| 128.00 |
1.425E-01 |
+20.4 |
-22.2 |
| 128.50 |
1.406E-01 |
+20.4 |
-22.2 |
| 129.00 |
1.389E-01 |
+20.4 |
-22.1 |
| 129.50 |
1.370E-01 |
+20.4 |
-22.1 |
| 130.00 |
1.351E-01 |
+20.3 |
-22.1 |
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 |
1.289E-02 |
+7.6 |
-16.6 |
±4.9 |
±4.7 |
±1.5 |
8.880E-03 |
4.000E-03 |
| 120.50 |
1.281E-02 |
+7.5 |
-16.5 |
±4.9 |
±4.7 |
±1.5 |
8.830E-03 |
3.970E-03 |
| 121.00 |
1.273E-02 |
+7.6 |
-16.5 |
±4.9 |
±4.7 |
±1.5 |
8.780E-03 |
3.950E-03 |
| 121.50 |
1.267E-02 |
+7.5 |
-16.6 |
±4.9 |
±4.7 |
±1.5 |
8.730E-03 |
3.930E-03 |
| 122.00 |
1.260E-02 |
+7.5 |
-16.6 |
±4.9 |
±4.7 |
±1.5 |
8.690E-03 |
3.920E-03 |
| 122.50 |
1.254E-02 |
+7.5 |
-16.8 |
±4.9 |
±4.7 |
±1.5 |
8.630E-03 |
3.890E-03 |
| 123.00 |
1.247E-02 |
+7.5 |
-16.7 |
±4.9 |
±4.7 |
±1.5 |
8.600E-03 |
3.880E-03 |
| 123.50 |
1.241E-02 |
+7.4 |
-16.8 |
±4.9 |
±4.7 |
±1.5 |
8.550E-03 |
3.860E-03 |
| 124.00 |
1.236E-02 |
+7.4 |
-17.0 |
±4.9 |
±4.7 |
±1.5 |
8.510E-03 |
3.840E-03 |
| 124.10 |
1.235E-02 |
+7.4 |
-16.9 |
±4.9 |
±4.7 |
±1.5 |
8.510E-03 |
3.840E-03 |
| 124.20 |
1.235E-02 |
+7.4 |
-17.0 |
±4.9 |
±4.7 |
±1.5 |
8.500E-03 |
3.830E-03 |
| 124.30 |
1.233E-02 |
+7.4 |
-17.0 |
±4.9 |
±4.7 |
±1.5 |
8.500E-03 |
3.830E-03 |
| 124.40 |
1.231E-02 |
+7.4 |
-17.0 |
±4.9 |
±4.7 |
±1.5 |
8.500E-03 |
3.830E-03 |
| 124.50 |
1.228E-02 |
+7.4 |
-16.9 |
±4.9 |
±4.7 |
±1.5 |
8.460E-03 |
3.820E-03 |
| 124.60 |
1.228E-02 |
+7.4 |
-16.8 |
±4.9 |
±4.7 |
±1.5 |
8.470E-03 |
3.820E-03 |
| 124.70 |
1.226E-02 |
+7.4 |
-16.8 |
±4.9 |
±4.7 |
±1.5 |
8.470E-03 |
3.810E-03 |
| 124.80 |
1.225E-02 |
+7.4 |
-16.8 |
±4.9 |
±4.7 |
±1.5 |
8.440E-03 |
3.810E-03 |
| 124.90 |
1.223E-02 |
+7.4 |
-16.8 |
±4.9 |
±4.7 |
±1.5 |
8.430E-03 |
3.800E-03 |
| 125.00 |
1.226E-02 |
+7.3 |
-17.2 |
±4.9 |
±4.7 |
±1.5 |
8.430E-03 |
3.800E-03 |
| 125.09 |
1.223E-02 |
+7.4 |
-17.0 |
±5.0 |
±4.7 |
±1.5 |
8.420E-03 |
3.800E-03 |
| 125.10 |
1.223E-02 |
+7.4 |
-17.0 |
±5.0 |
±4.7 |
±1.5 |
8.420E-03 |
3.800E-03 |
| 125.20 |
1.222E-02 |
+7.3 |
-16.9 |
±5.0 |
±4.7 |
±1.5 |
8.410E-03 |
3.800E-03 |
| 125.30 |
1.221E-02 |
+7.4 |
-16.9 |
±5.0 |
±4.7 |
±1.5 |
8.410E-03 |
3.790E-03 |
| 125.40 |
1.217E-02 |
+7.4 |
-16.8 |
±5.0 |
±4.7 |
±1.5 |
8.400E-03 |
3.790E-03 |
| 125.50 |
1.219E-02 |
+7.4 |
-17.0 |
±5.0 |
±4.7 |
±1.5 |
8.400E-03 |
3.790E-03 |
| 125.60 |
1.218E-02 |
+7.3 |
-17.1 |
±5.0 |
±4.7 |
±1.5 |
8.390E-03 |
3.780E-03 |
| 125.70 |
1.216E-02 |
+7.3 |
-17.0 |
±5.0 |
±4.7 |
±1.5 |
8.380E-03 |
3.780E-03 |
| 125.80 |
1.214E-02 |
+7.4 |
-16.8 |
±5.0 |
±4.7 |
±1.5 |
8.360E-03 |
3.780E-03 |
| 125.90 |
1.213E-02 |
+7.3 |
-17.0 |
±5.0 |
±4.7 |
±1.5 |
8.350E-03 |
3.770E-03 |
| 126.00 |
1.213E-02 |
+7.3 |
-17.0 |
±5.0 |
±4.7 |
±1.5 |
8.340E-03 |
3.770E-03 |
| 126.50 |
1.207E-02 |
+7.3 |
-17.1 |
±5.0 |
±4.7 |
±1.5 |
8.320E-03 |
3.750E-03 |
| 127.00 |
1.199E-02 |
+7.3 |
-17.1 |
±5.0 |
±4.7 |
±1.5 |
8.270E-03 |
3.740E-03 |
| 127.50 |
1.197E-02 |
+7.3 |
-17.1 |
±5.0 |
±4.7 |
±1.5 |
8.240E-03 |
3.720E-03 |
| 128.00 |
1.190E-02 |
+7.2 |
-17.2 |
±5.0 |
±4.7 |
±1.5 |
8.200E-03 |
3.700E-03 |
| 128.50 |
1.185E-02 |
+7.2 |
-17.5 |
±5.0 |
±4.8 |
±1.5 |
8.160E-03 |
3.690E-03 |
| 129.00 |
1.178E-02 |
+7.3 |
-17.2 |
±5.0 |
±4.8 |
±1.5 |
8.120E-03 |
3.670E-03 |
| 129.50 |
1.174E-02 |
+7.2 |
-17.4 |
±5.0 |
±4.8 |
±1.5 |
8.080E-03 |
3.660E-03 |
| 130.00 |
1.167E-02 |
+7.2 |
-17.4 |
±5.0 |
±4.8 |
±1.5 |
8.040E-03 |
3.650E-03 |
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 |
1.028E-03 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
7.090E-04 |
3.190E-04 |
| 120.50 |
1.018E-03 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
7.030E-04 |
3.150E-04 |
| 121.00 |
1.008E-03 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.960E-04 |
3.110E-04 |
| 121.50 |
1.000E-03 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.890E-04 |
3.090E-04 |
| 122.00 |
9.870E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.820E-04 |
3.050E-04 |
| 122.50 |
9.780E-04 |
+2.8 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.760E-04 |
3.020E-04 |
| 123.00 |
9.690E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.690E-04 |
2.990E-04 |
| 123.50 |
9.600E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.630E-04 |
2.960E-04 |
| 124.00 |
9.490E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.550E-04 |
2.930E-04 |
| 124.10 |
9.470E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.540E-04 |
2.920E-04 |
| 124.20 |
9.430E-04 |
+2.8 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.530E-04 |
2.910E-04 |
| 124.30 |
9.430E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.520E-04 |
2.910E-04 |
| 124.40 |
9.410E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.510E-04 |
2.900E-04 |
| 124.50 |
9.390E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.500E-04 |
2.900E-04 |
| 124.60 |
9.370E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.480E-04 |
2.890E-04 |
| 124.70 |
9.350E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.470E-04 |
2.880E-04 |
| 124.80 |
9.340E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.450E-04 |
2.880E-04 |
| 124.90 |
9.330E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.440E-04 |
2.870E-04 |
| 125.00 |
9.300E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.420E-04 |
2.870E-04 |
| 125.09 |
9.290E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.420E-04 |
2.860E-04 |
| 125.10 |
9.290E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.420E-04 |
2.860E-04 |
| 125.20 |
9.250E-04 |
+2.8 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.410E-04 |
2.850E-04 |
| 125.30 |
9.250E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.400E-04 |
2.850E-04 |
| 125.40 |
9.220E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.380E-04 |
2.840E-04 |
| 125.50 |
9.210E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.380E-04 |
2.840E-04 |
| 125.60 |
9.190E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.360E-04 |
2.830E-04 |
| 125.70 |
9.170E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.340E-04 |
2.830E-04 |
| 125.80 |
9.160E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.330E-04 |
2.820E-04 |
| 125.90 |
9.140E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.320E-04 |
2.810E-04 |
| 126.00 |
9.120E-04 |
+2.9 |
-2.5 |
±3.0 |
±3.0 |
±0.0 |
6.300E-04 |
2.800E-04 |
| 126.50 |
9.030E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.250E-04 |
2.780E-04 |
| 127.00 |
8.940E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.190E-04 |
2.750E-04 |
| 127.50 |
8.850E-04 |
+2.9 |
-2.6 |
±3.0 |
±3.0 |
±0.0 |
6.130E-04 |
2.720E-04 |
| 128.00 |
8.750E-04 |
+2.9 |
-2.5 |
±3.1 |
±3.1 |
±0.0 |
6.070E-04 |
2.700E-04 |
| 128.50 |
8.690E-04 |
+2.9 |
-2.6 |
±3.1 |
±3.1 |
±0.0 |
6.010E-04 |
2.670E-04 |
| 129.00 |
8.600E-04 |
+2.9 |
-2.6 |
±3.1 |
±3.1 |
±0.0 |
5.950E-04 |
2.640E-04 |
| 129.50 |
8.520E-04 |
+2.9 |
-2.6 |
±3.1 |
±3.1 |
±0.0 |
5.890E-04 |
2.620E-04 |
| 130.00 |
8.430E-04 |
+2.9 |
-2.6 |
±3.1 |
±3.1 |
±0.0 |
5.850E-04 |
2.590E-04 |
--
ReiTanaka - 2016-03-01
This topic: LHCPhysics
> LHCHXSWG > CERNYellowReportPageAt7TeV
Topic revision: r18 - 2016-07-02 - ReiTanaka
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