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LHCPhysics Web>LHCHXSWG>CERNYellowReportPageBSMAt8TeV (2023-11-13, TatsuyaMasubuchi) EditAttachPDFBSM Higgs production cross sections at √s = 8 TeV (update in CERN Report4 2016)
- Cross sections reported in CERN Report 4. See here and here here for previous numbers in CERN Report 3.
- Higgs cross sections and BRs in Spread sheet are available in xlsx format
- You can find figures at our gallery here.
BSM Higgs-boson production cross section calculation
- Please check Proposal on how to provide reference "Higgs" cross sections for BSM applications
- Full mass scan should be provided for major Higgs production processes:
- Major process: ggF, VBF, WH (also separate W+H and W-H), ZH (also gg→ZH)
- Associated Higgs with heavy quark: ttH, bbH
- Associated Higgs with single top-quark: tH (bq→tHq', bg→WtH, qq→btH)
- Higgs width should be set to zero (NWA).
- Separate electroweak correction should be provided.
- For relevant processes, and if possible, the contributions proportional to different Higgs couplings should be given separately, together with the corresponding uncertainties.
- All other external parameters should be chosen as in the corresponding best SM predictions as well as the evaluation of the uncertainties.
- SM width: At each mass point, the corresponding Higgs widths calculated in the SM with the same characteristics above should be provided.
- Examples on how to use these predictions in specific cases are provided.
Mass range and step for BSM Higgs boson:
| Higgs Mass range | step size | # of points | addendum |
|---|---|---|---|
| [10,150] GeV | 5 GeV | 29 points | |
| [150,500] GeV | 10 GeV | 35 points | + MH=125.09 GeV |
| [500,3000] GeV | 50 GeV | 50 points |
- Total 115 points for MH=[10,3000] GeV.
- Lower mass limit might depend on stability of the code at low Bjorken-x. To be assessed.
gluon-gluon Fusion Process
- Cross sections are calculated with dFG program at NNLO+NNLL QCD (only) accuracy. Separate NLO EW correction factors 1+δEW are also given for MH=[100,2500]GeV.
- This is an interim recommendation, will be updated when new N3LO QCD numbers became available.
- 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 % | 1+δEW |
| 10.00 | 4.614E+03 | +47.9 | -37.3 | ±6.5 | ±5.9 | ±2.7 | 0.0000 |
| 15.00 | 2.701E+03 | +33.6 | -27.7 | ±5.1 | ±4.2 | ±2.8 | 0.0000 |
| 20.00 | 1.261E+03 | +24.9 | -21.2 | ±4.4 | ±3.2 | ±2.9 | 0.0000 |
| 25.00 | 6.676E+02 | +20.3 | -17.1 | ±4.1 | ±2.7 | ±3.0 | 0.0000 |
| 30.00 | 4.009E+02 | +18.1 | -14.8 | ±4.0 | ±2.5 | ±3.0 | 0.0000 |
| 35.00 | 2.664E+02 | +15.9 | -13.4 | ±3.8 | ±2.4 | ±3.0 | 0.0000 |
| 40.00 | 1.911E+02 | +14.2 | -12.6 | ±3.8 | ±2.2 | ±3.0 | 0.0000 |
| 45.00 | 1.450E+02 | +13.0 | -11.9 | ±3.7 | ±2.2 | ±3.0 | 0.0000 |
| 50.00 | 1.147E+02 | +12.0 | -11.3 | ±3.6 | ±2.1 | ±3.0 | 0.0000 |
| 55.00 | 9.365E+01 | +11.2 | -10.8 | ±3.6 | ±2.0 | ±2.9 | 0.0000 |
| 60.00 | 7.827E+01 | +10.6 | -10.4 | ±3.5 | ±2.0 | ±2.9 | 0.0000 |
| 65.00 | 6.661E+01 | +10.1 | -10.1 | ±3.5 | ±2.0 | ±2.8 | 0.0000 |
| 70.00 | 5.752E+01 | +9.7 | -9.8 | ±3.4 | ±2.0 | ±2.8 | 0.0000 |
| 75.00 | 5.025E+01 | +9.3 | -9.5 | ±3.4 | ±1.9 | ±2.8 | 0.0000 |
| 80.00 | 4.431E+01 | +9.0 | -9.3 | ±3.3 | ±1.9 | ±2.7 | 0.0000 |
| 85.00 | 3.940E+01 | +8.7 | -9.1 | ±3.3 | ±1.9 | ±2.7 | 0.0000 |
| 90.00 | 3.526E+01 | +8.5 | -8.9 | ±3.3 | ±1.9 | ±2.7 | 0.0000 |
| 95.00 | 3.175E+01 | +8.3 | -8.7 | ±3.3 | ±1.9 | ±2.7 | 0.0000 |
| 100.00 | 2.873E+01 | +8.1 | -8.6 | ±3.2 | ±1.9 | ±2.6 | 1.0418 |
| 105.00 | 2.611E+01 | +7.9 | -8.4 | ±3.2 | ±1.8 | ±2.6 | 1.0436 |
| 110.00 | 2.383E+01 | +7.7 | -8.3 | ±3.2 | ±1.8 | ±2.6 | 1.0455 |
| 115.00 | 2.184E+01 | +7.6 | -8.2 | ±3.2 | ±1.8 | ±2.6 | 1.0474 |
| 120.00 | 2.008E+01 | +7.5 | -8.1 | ±3.2 | ±1.8 | ±2.6 | 1.0494 |
| 125.00 | 1.851E+01 | +7.3 | -8.0 | ±3.1 | ±1.8 | ±2.6 | 1.0514 |
| 130.00 | 1.712E+01 | +7.2 | -7.9 | ±3.1 | ±1.8 | ±2.5 | 1.0534 |
| 135.00 | 1.587E+01 | +7.1 | -7.8 | ±3.1 | ±1.8 | ±2.5 | 1.0553 |
| 140.00 | 1.475E+01 | +7.0 | -7.7 | ±3.1 | ±1.8 | ±2.5 | 1.0571 |
| 145.00 | 1.375E+01 | +6.9 | -7.6 | ±3.1 | ±1.8 | ±2.5 | 1.0587 |
| 150.00 | 1.284E+01 | +6.8 | -7.5 | ±3.1 | ±1.8 | ±2.5 | 1.0598 |
| 160.00 | 1.127E+01 | +6.6 | -7.4 | ±3.1 | ±1.8 | ±2.5 | 1.0486 |
| 170.00 | 9.961E+00 | +6.5 | -7.3 | ±3.1 | ±1.8 | ±2.5 | 1.0206 |
| 180.00 | 8.866E+00 | +6.4 | -7.1 | ±3.1 | ±1.8 | ±2.5 | 1.0053 |
| 190.00 | 7.945E+00 | +6.2 | -7.0 | ±3.1 | ±1.8 | ±2.5 | 0.9872 |
| 200.00 | 7.163E+00 | +6.1 | -6.9 | ±3.1 | ±1.9 | ±2.5 | 0.9793 |
| 210.00 | 6.492E+00 | +6.0 | -6.8 | ±3.1 | ±1.9 | ±2.5 | 0.9761 |
| 220.00 | 5.919E+00 | +6.0 | -6.7 | ±3.1 | ±1.9 | ±2.5 | 0.9749 |
| 230.00 | 5.426E+00 | +5.9 | -6.6 | ±3.1 | ±1.9 | ±2.5 | 0.9749 |
| 240.00 | 5.000E+00 | +5.9 | -6.6 | ±3.2 | ±2.0 | ±2.5 | 0.9755 |
| 250.00 | 4.632E+00 | +5.8 | -6.5 | ±3.2 | ±2.0 | ±2.5 | 0.9762 |
| 260.00 | 4.314E+00 | +5.8 | -6.4 | ±3.2 | ±2.0 | ±2.5 | 0.9772 |
| 270.00 | 4.040E+00 | +5.8 | -6.3 | ±3.2 | ±2.0 | ±2.5 | 0.9783 |
| 280.00 | 3.807E+00 | +5.8 | -6.3 | ±3.2 | ±2.1 | ±2.5 | 0.9795 |
| 290.00 | 3.608E+00 | +5.8 | -6.2 | ±3.2 | ±2.1 | ±2.5 | 0.9805 |
| 300.00 | 3.444E+00 | +5.8 | -6.2 | ±3.3 | ±2.1 | ±2.5 | 0.9813 |
| 310.00 | 3.314E+00 | +5.8 | -6.1 | ±3.3 | ±2.2 | ±2.5 | 0.9819 |
| 320.00 | 3.222E+00 | +5.8 | -6.0 | ±3.3 | ±2.2 | ±2.5 | 0.9820 |
| 330.00 | 3.175E+00 | +5.8 | -5.9 | ±3.4 | ±2.3 | ±2.5 | 0.9813 |
| 340.00 | 3.200E+00 | +5.9 | -5.9 | ±3.4 | ±2.3 | ±2.5 | 0.9779 |
| 350.00 | 3.409E+00 | +5.9 | -5.8 | ±3.4 | ±2.3 | ±2.5 | 0.9595 |
| 360.00 | 3.503E+00 | +5.9 | -5.8 | ±3.5 | ±2.4 | ±2.5 | 0.9608 |
| 370.00 | 3.470E+00 | +5.9 | -5.7 | ±3.5 | ±2.4 | ±2.5 | 0.9642 |
| 380.00 | 3.357E+00 | +5.9 | -5.6 | ±3.6 | ±2.5 | ±2.5 | 0.9677 |
| 390.00 | 3.198E+00 | +5.9 | -5.6 | ±3.6 | ±2.5 | ±2.5 | 0.9713 |
| 400.00 | 3.011E+00 | +5.9 | -5.5 | ±3.6 | ±2.6 | ±2.6 | 0.9741 |
| 410.00 | 2.812E+00 | +5.9 | -5.5 | ±3.7 | ±2.6 | ±2.6 | 0.9771 |
| 420.00 | 2.609E+00 | +5.9 | -5.4 | ±3.7 | ±2.7 | ±2.6 | 0.9802 |
| 430.00 | 2.411E+00 | +5.9 | -5.4 | ±3.8 | ±2.8 | ±2.6 | 0.9830 |
| 440.00 | 2.220E+00 | +5.9 | -5.4 | ±3.8 | ±2.8 | ±2.6 | 0.9853 |
| 450.00 | 2.038E+00 | +5.9 | -5.3 | ±3.9 | ±2.9 | ±2.6 | 0.9878 |
| 460.00 | 1.868E+00 | +5.9 | -5.3 | ±3.9 | ±2.9 | ±2.6 | 0.9900 |
| 470.00 | 1.709E+00 | +5.9 | -5.3 | ±4.0 | ±3.0 | ±2.6 | 0.9921 |
| 480.00 | 1.562E+00 | +5.9 | -5.3 | ±4.0 | ±3.1 | ±2.6 | 0.9940 |
| 490.00 | 1.426E+00 | +5.9 | -5.2 | ±4.1 | ±3.1 | ±2.7 | 0.9961 |
| 500.00 | 1.301E+00 | +5.9 | -5.2 | ±4.2 | ±3.2 | ±2.7 | 0.9981 |
| 550.00 | 8.236E-01 | +5.9 | -5.1 | ±4.4 | ±3.5 | ±2.7 | 1.0069 |
| 600.00 | 5.241E-01 | +6.0 | -5.1 | ±4.8 | ±3.8 | ±2.8 | 1.0152 |
| 650.00 | 3.377E-01 | +6.0 | -5.1 | ±5.1 | ±4.2 | ±2.9 | 1.0226 |
| 700.00 | 2.207E-01 | +6.1 | -5.2 | ±5.4 | ±4.5 | ±3.0 | 1.0301 |
| 750.00 | 1.464E-01 | +6.1 | -5.2 | ±5.8 | ±4.9 | ±3.1 | 1.0377 |
| 800.00 | 9.849E-02 | +6.2 | -5.2 | ±6.1 | ±5.3 | ±3.1 | 1.0454 |
| 850.00 | 6.713E-02 | +6.3 | -5.3 | ±6.5 | ±5.6 | ±3.2 | 1.0532 |
| 900.00 | 4.634E-02 | +6.3 | -5.4 | ±6.9 | ±6.0 | ±3.3 | 1.0610 |
| 950.00 | 3.237E-02 | +6.4 | -5.4 | ±7.3 | ±6.4 | ±3.4 | 1.0695 |
| 1000.00 | 2.285E-02 | +6.5 | -5.5 | ±7.7 | ±6.8 | ±3.5 | 1.0783 |
| 1050.00 | 1.628E-02 | +6.6 | -5.6 | ±8.1 | ±7.2 | ±3.6 | 1.0890 |
| 1100.00 | 1.172E-02 | +6.7 | -5.6 | ±8.5 | ±7.6 | ±3.8 | 1.1004 |
| 1150.00 | 8.507E-03 | +6.7 | -5.7 | ±8.9 | ±8.0 | ±3.9 | 1.1122 |
| 1200.00 | 6.222E-03 | +6.8 | -5.8 | ±9.3 | ±8.4 | ±4.0 | 1.1242 |
| 1250.00 | 4.587E-03 | +6.9 | -5.8 | ±9.8 | ±8.9 | ±4.1 | 1.1364 |
| 1300.00 | 3.402E-03 | +7.0 | -5.9 | ±10.2 | ±9.3 | ±4.2 | 1.1475 |
| 1350.00 | 2.540E-03 | +7.1 | -6.0 | ±10.7 | ±9.7 | ±4.4 | 1.1586 |
| 1400.00 | 1.909E-03 | +7.3 | -6.1 | ±11.1 | ±10.2 | ±4.5 | 1.1700 |
| 1450.00 | 1.442E-03 | +7.4 | -6.2 | ±11.6 | ±10.7 | ±4.6 | 1.1816 |
| 1500.00 | 1.095E-03 | +7.6 | -6.2 | ±12.1 | ±11.1 | ±4.8 | 1.1937 |
| 1550.00 | 8.349E-04 | +7.7 | -6.3 | ±12.6 | ±11.6 | ±4.9 | 1.2069 |
| 1600.00 | 6.400E-04 | +7.8 | -6.4 | ±13.2 | ±12.1 | ±5.1 | 1.2206 |
| 1650.00 | 4.925E-04 | +7.9 | -6.5 | ±13.7 | ±12.7 | ±5.3 | 1.2347 |
| 1700.00 | 3.805E-04 | +7.9 | -6.6 | ±14.3 | ±13.2 | ±5.4 | 1.2493 |
| 1750.00 | 2.951E-04 | +8.0 | -3.6 | ±15.0 | ±8.3 | ±12.4 | 1.2644 |
| 1800.00 | 2.297E-04 | +8.0 | -4.3 | ±15.0 | ±9.9 | ±11.3 | 1.2798 |
| 1850.00 | 1.793E-04 | +8.1 | -4.9 | ±15.3 | ±11.4 | ±10.3 | 1.2955 |
| 1900.00 | 1.404E-04 | +8.1 | -5.4 | ±15.9 | ±12.8 | ±9.5 | 1.3117 |
| 1950.00 | 1.103E-04 | +8.2 | -5.9 | ±16.6 | ±14.0 | ±8.8 | 1.3283 |
| 2000.00 | 8.685E-05 | +8.2 | -6.3 | ±17.4 | ±15.2 | ±8.3 | 1.3453 |
| 2050.00 | 6.857E-05 | +8.2 | -6.7 | ±18.2 | ±16.4 | ±8.0 | 1.3627 |
| 2100.00 | 5.422E-05 | +8.3 | -7.1 | ±19.1 | ±17.5 | ±7.7 | 1.3806 |
| 2150.00 | 4.311E-05 | +8.3 | -7.4 | ±20.0 | ±18.5 | ±7.6 | 1.3989 |
| 2200.00 | 3.419E-05 | +8.4 | -7.6 | ±20.8 | ±19.4 | ±7.5 | 1.4176 |
| 2250.00 | 2.722E-05 | +8.4 | -7.9 | ±21.7 | ±20.4 | ±7.6 | 1.4367 |
| 2300.00 | 2.173E-05 | +8.4 | -8.1 | ±22.6 | ±21.2 | ±7.7 | 1.4563 |
| 2350.00 | 1.737E-05 | +8.5 | -8.2 | ±23.5 | ±22.1 | ±7.9 | 1.4763 |
| 2400.00 | 1.390E-05 | +8.5 | -8.4 | ±24.4 | ±23.0 | ±8.2 | 1.4968 |
| 2450.00 | 1.113E-05 | +8.6 | -8.5 | ±25.3 | ±23.8 | ±8.5 | 1.5177 |
| 2500.00 | 8.936E-06 | +8.6 | -8.6 | ±26.2 | ±24.6 | ±8.8 | 1.5390 |
| 2550.00 | 7.190E-06 | +8.6 | -8.6 | ±27.1 | ±25.5 | ±9.1 | 0.0000 |
| 2600.00 | 5.771E-06 | +8.7 | -8.7 | ±28.0 | ±26.3 | ±9.5 | 0.0000 |
| 2650.00 | 4.665E-06 | +8.7 | -8.7 | ±28.9 | ±27.2 | ±9.8 | 0.0000 |
| 2700.00 | 3.753E-06 | +8.8 | -8.8 | ±29.9 | ±28.1 | ±10.2 | 0.0000 |
| 2750.00 | 3.028E-06 | +8.8 | -8.8 | ±30.8 | ±29.0 | ±10.5 | 0.0000 |
| 2800.00 | 2.455E-06 | +8.8 | -8.8 | ±31.8 | ±30.0 | ±10.7 | 0.0000 |
| 2850.00 | 1.979E-06 | +8.9 | -8.9 | ±32.9 | ±31.0 | ±10.9 | 0.0000 |
| 2900.00 | 1.604E-06 | +8.9 | -8.9 | ±34.0 | ±32.1 | ±11.0 | 0.0000 |
| 2950.00 | 1.298E-06 | +9.0 | -9.0 | ±35.1 | ±33.3 | ±11.1 | 0.0000 |
| 3000.00 | 1.048E-06 | +9.0 | -9.0 | ±36.2 | ±34.5 | ±11.1 | 0.0000 |
VBF Process
- Cross sections are calculated at (approx.) NNLO QCD accuracy.
- Calculations are the same as CERN Report 3, except it is in NWA (CPS in CERN Report 3).
- Program: NNLO QCD (VBF@NNLO)
- QCD scales: μ=μF=μR=MW, uncertainty estimated in the range 1/2 < μ/MW < 2 (scales have been varied independently by factor 2).
- No additional THU nor PU uncertainties assigned.
- PDF set: PDF4LHC15_nnlo_30_pdfas
| mH (GeV) | Cross Section (pb) | +QCD Scale % | -QCD Scale % | ±(PDF+αs) % | ±PDF % | ±αs % | 1+δEW |
| 10.00 | 5.474E+00 | +0.9 | -0.5 | ±2.0 | ±1.8 | ±0.8 | |
| 15.00 | 5.208E+00 | +0.8 | -0.5 | ±2.0 | ±1.8 | ±0.7 | |
| 20.00 | 4.934E+00 | +0.8 | -0.5 | ±2.0 | ±1.8 | ±0.7 | |
| 25.00 | 4.667E+00 | +0.8 | -0.4 | ±2.0 | ±1.8 | ±0.7 | |
| 30.00 | 4.413E+00 | +0.7 | -0.4 | ±1.9 | ±1.8 | ±0.7 | |
| 35.00 | 4.169E+00 | +0.7 | -0.4 | ±1.9 | ±1.8 | ±0.7 | |
| 40.00 | 3.938E+00 | +0.6 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 45.00 | 3.722E+00 | +0.6 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 50.00 | 3.519E+00 | +0.6 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 55.00 | 3.329E+00 | +0.5 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 60.00 | 3.152E+00 | +0.5 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 65.00 | 2.986E+00 | +0.5 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 70.00 | 2.831E+00 | +0.5 | -0.3 | ±1.9 | ±1.8 | ±0.6 | |
| 75.00 | 2.686E+00 | +0.4 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 80.00 | 2.550E+00 | +0.4 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 85.00 | 2.423E+00 | +0.4 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 90.00 | 2.304E+00 | +0.4 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 95.00 | 2.192E+00 | +0.4 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 100.00 | 2.087E+00 | +0.3 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 105.00 | 1.988E+00 | +0.3 | -0.2 | ±1.9 | ±1.8 | ±0.5 | |
| 110.00 | 1.896E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.5 | |
| 115.00 | 1.809E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.5 | |
| 120.00 | 1.727E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.5 | |
| 125.00 | 1.650E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.5 | |
| 130.00 | 1.577E+00 | +0.2 | -0.2 | ±1.9 | ±1.9 | ±0.4 | |
| 135.00 | 1.508E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.4 | |
| 140.00 | 1.443E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.4 | |
| 145.00 | 1.382E+00 | +0.3 | -0.2 | ±1.9 | ±1.9 | ±0.4 | |
| 150.00 | 1.323E+00 | +0.2 | -0.1 | ±1.9 | ±1.9 | ±0.4 | |
| 160.00 | 1.216E+00 | +0.3 | -0.1 | ±1.9 | ±1.9 | ±0.4 | |
| 170.00 | 1.120E+00 | +0.3 | -0.1 | ±1.9 | ±1.9 | ±0.4 | |
| 180.00 | 1.033E+00 | +0.3 | -0.1 | ±1.9 | ±1.9 | ±0.4 | |
| 190.00 | 9.549E-01 | +0.2 | -0.1 | ±2.0 | ±1.9 | ±0.4 | |
| 200.00 | 8.839E-01 | +0.2 | -0.1 | ±2.0 | ±1.9 | ±0.3 | |
| 210.00 | 8.195E-01 | +0.2 | -0.1 | ±2.0 | ±1.9 | ±0.3 | |
| 220.00 | 7.609E-01 | +0.3 | -0.1 | ±2.0 | ±1.9 | ±0.3 | |
| 230.00 | 7.074E-01 | +0.3 | -0.1 | ±2.0 | ±2.0 | ±0.3 | |
| 240.00 | 6.587E-01 | +0.3 | -0.1 | ±2.0 | ±2.0 | ±0.3 | |
| 250.00 | 6.140E-01 | +0.3 | -0.1 | ±2.0 | ±2.0 | ±0.3 | |
| 260.00 | 5.731E-01 | +0.3 | -0.1 | ±2.0 | ±2.0 | ±0.3 | |
| 270.00 | 5.356E-01 | +0.3 | -0.1 | ±2.0 | ±2.0 | ±0.3 | |
| 280.00 | 5.011E-01 | +0.3 | -0.1 | ±2.0 | ±2.0 | ±0.3 | |
| 290.00 | 4.692E-01 | +0.3 | -0.2 | ±2.0 | ±2.0 | ±0.2 | |
| 300.00 | 4.399E-01 | +0.3 | -0.2 | ±2.1 | ±2.0 | ±0.2 | |
| 310.00 | 4.128E-01 | +0.3 | -0.2 | ±2.1 | ±2.1 | ±0.2 | |
| 320.00 | 3.877E-01 | +0.3 | -0.2 | ±2.1 | ±2.1 | ±0.2 | |
| 330.00 | 3.644E-01 | +0.3 | -0.2 | ±2.1 | ±2.1 | ±0.2 | |
| 340.00 | 3.428E-01 | +0.3 | -0.2 | ±2.1 | ±2.1 | ±0.2 | |
| 350.00 | 3.228E-01 | +0.3 | -0.3 | ±2.1 | ±2.1 | ±0.2 | |
| 360.00 | 3.042E-01 | +0.3 | -0.3 | ±2.1 | ±2.1 | ±0.2 | |
| 370.00 | 2.868E-01 | +0.3 | -0.3 | ±2.1 | ±2.1 | ±0.2 | |
| 380.00 | 2.707E-01 | +0.3 | -0.3 | ±2.1 | ±2.1 | ±0.2 | |
| 390.00 | 2.556E-01 | +0.3 | -0.3 | ±2.2 | ±2.2 | ±0.2 | |
| 400.00 | 2.415E-01 | +0.3 | -0.4 | ±2.2 | ±2.2 | ±0.2 | |
| 410.00 | 2.284E-01 | +0.3 | -0.4 | ±2.2 | ±2.2 | ±0.1 | |
| 420.00 | 2.161E-01 | +0.3 | -0.4 | ±2.2 | ±2.2 | ±0.1 | |
| 430.00 | 2.046E-01 | +0.3 | -0.4 | ±2.2 | ±2.2 | ±0.1 | |
| 440.00 | 1.938E-01 | +0.3 | -0.4 | ±2.2 | ±2.2 | ±0.1 | |
| 450.00 | 1.837E-01 | +0.3 | -0.4 | ±2.2 | ±2.2 | ±0.1 | |
| 460.00 | 1.742E-01 | +0.3 | -0.5 | ±2.2 | ±2.2 | ±0.1 | |
| 470.00 | 1.652E-01 | +0.3 | -0.5 | ±2.3 | ±2.3 | ±0.1 | |
| 480.00 | 1.569E-01 | +0.3 | -0.5 | ±2.3 | ±2.3 | ±0.1 | |
| 490.00 | 1.490E-01 | +0.3 | -0.5 | ±2.3 | ±2.3 | ±0.1 | |
| 500.00 | 1.415E-01 | +0.3 | -0.5 | ±2.3 | ±2.3 | ±0.1 | |
| 550.00 | 1.103E-01 | +0.3 | -0.6 | ±2.4 | ±2.4 | ±0.0 | |
| 600.00 | 8.684E-02 | +0.3 | -0.7 | ±2.5 | ±2.5 | ±0.0 | |
| 650.00 | 6.892E-02 | +0.3 | -0.8 | ±2.5 | ±2.5 | ±0.0 | |
| 700.00 | 5.510E-02 | +0.3 | -0.8 | ±2.6 | ±2.6 | ±0.0 | |
| 750.00 | 4.433E-02 | +0.3 | -0.9 | ±2.7 | ±2.7 | ±0.1 | |
| 800.00 | 3.588E-02 | +0.3 | -1.0 | ±2.8 | ±2.8 | ±0.1 | |
| 850.00 | 2.918E-02 | +0.4 | -1.1 | ±2.9 | ±2.9 | ±0.1 | |
| 900.00 | 2.383E-02 | +0.4 | -1.1 | ±3.0 | ±3.0 | ±0.1 | |
| 950.00 | 1.954E-02 | +0.4 | -1.2 | ±3.1 | ±3.1 | ±0.1 | |
| 1000.00 | 1.608E-02 | +0.5 | -1.3 | ±3.2 | ±3.1 | ±0.1 | |
| 1050.00 | 1.328E-02 | +0.5 | -1.4 | ±3.3 | ±3.2 | ±0.2 | |
| 1100.00 | 1.099E-02 | +0.6 | -1.4 | ±3.4 | ±3.4 | ±0.2 | |
| 1150.00 | 9.126E-03 | +0.6 | -1.5 | ±3.5 | ±3.5 | ±0.2 | |
| 1200.00 | 7.593E-03 | +0.6 | -1.6 | ±3.6 | ±3.6 | ±0.2 | |
| 1250.00 | 6.331E-03 | +0.7 | -1.7 | ±3.7 | ±3.7 | ±0.2 | |
| 1300.00 | 5.289E-03 | +0.7 | -1.8 | ±3.8 | ±3.8 | ±0.2 | |
| 1350.00 | 4.425E-03 | +0.8 | -1.8 | ±4.0 | ±4.0 | ±0.2 | |
| 1400.00 | 3.709E-03 | +0.8 | -1.9 | ±4.1 | ±4.1 | ±0.2 | |
| 1450.00 | 3.113E-03 | +0.8 | -2.0 | ±4.2 | ±4.2 | ±0.2 | |
| 1500.00 | 2.616E-03 | +0.9 | -2.1 | ±4.4 | ±4.4 | ±0.2 | |
| 1550.00 | 2.200E-03 | +0.9 | -2.2 | ±4.6 | ±4.5 | ±0.2 | |
| 1600.00 | 1.853E-03 | +1.0 | -2.3 | ±4.7 | ±4.7 | ±0.2 | |
| 1650.00 | 1.562E-03 | +1.0 | -2.3 | ±4.9 | ±4.9 | ±0.2 | |
| 1700.00 | 1.318E-03 | +1.1 | -2.4 | ±5.1 | ±5.1 | ±0.2 | |
| 1750.00 | 1.112E-03 | +1.1 | -2.5 | ±5.3 | ±5.3 | ±0.2 | |
| 1800.00 | 9.395E-04 | +1.2 | -2.6 | ±5.5 | ±5.5 | ±0.2 | |
| 1850.00 | 7.941E-04 | +1.2 | -2.7 | ±5.7 | ±5.7 | ±0.2 | |
| 1900.00 | 6.714E-04 | +1.3 | -2.8 | ±5.9 | ±5.9 | ±0.1 | |
| 1950.00 | 5.680E-04 | +1.3 | -2.9 | ±6.2 | ±6.2 | ±0.1 | |
| 2000.00 | 4.807E-04 | +1.4 | -3.0 | ±6.4 | ±6.4 | ±0.1 | |
| 2050.00 | 4.068E-04 | +1.4 | -3.0 | ±6.7 | ±6.7 | ±0.1 | |
| 2100.00 | 3.444E-04 | +1.5 | -3.1 | ±7.0 | ±7.0 | ±0.1 | |
| 2150.00 | 2.917E-04 | +1.5 | -3.2 | ±7.2 | ±7.2 | ±0.1 | |
| 2200.00 | 2.470E-04 | +1.6 | -3.3 | ±7.5 | ±7.5 | ±0.0 | |
| 2250.00 | 2.092E-04 | +1.6 | -3.4 | ±7.8 | ±7.8 | ±0.0 | |
| 2300.00 | 1.772E-04 | +1.7 | -3.5 | ±8.2 | ±8.2 | ±0.0 | |
| 2350.00 | 1.501E-04 | +1.8 | -3.6 | ±8.5 | ±8.5 | ±0.0 | |
| 2400.00 | 1.271E-04 | +1.8 | -3.7 | ±8.9 | ±8.9 | ±0.1 | |
| 2450.00 | 1.076E-04 | +1.9 | -3.8 | ±9.2 | ±9.2 | ±0.1 | |
| 2500.00 | 9.112E-05 | +1.9 | -3.9 | ±9.6 | ±9.6 | ±0.1 | |
| 2550.00 | 7.713E-05 | +2.0 | -4.0 | ±10.0 | ±10.0 | ±0.2 | |
| 2600.00 | 6.527E-05 | +2.1 | -4.1 | ±10.4 | ±10.4 | ±0.2 | |
| 2650.00 | 5.522E-05 | +2.1 | -4.2 | ±10.8 | ±10.8 | ±0.2 | |
| 2700.00 | 4.670E-05 | +2.2 | -4.3 | ±11.3 | ±11.3 | ±0.3 | |
| 2750.00 | 3.948E-05 | +2.3 | -4.4 | ±11.8 | ±11.7 | ±0.3 | |
| 2800.00 | 3.337E-05 | +2.4 | -4.5 | ±12.2 | ±12.2 | ±0.3 | |
| 2850.00 | 2.819E-05 | +2.4 | -4.6 | ±12.7 | ±12.7 | ±0.4 | |
| 2900.00 | 2.380E-05 | +2.5 | -4.7 | ±13.2 | ±13.2 | ±0.4 | |
| 2950.00 | 2.009E-05 | +2.6 | -4.8 | ±13.8 | ±13.8 | ±0.5 | |
| 3000.00 | 1.695E-05 | +2.6 | -4.9 | ±14.3 | ±14.3 | ±0.5 |
WH Process
- Cross sections are calculated at NNLO QCD accuracy.
- Calculations are the same as CERN Report 3.
- Program: NNLO QCD (VH@NNLO)
- QCD scales: μ=μF=μR=MVH=(pV+pH)2 for QCD 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)
- Photon-induced contribution of O(5%)
- NOT included for total cross section (agrees with CERN Report 3 numbers within 1%).
| mH (GeV) | Cross Section (pb) | +QCD Scale % | -QCD Scale % | ±(PDF+αs) % | ±PDF % | ±αs % | 1+δEW | W+H (pb) | W-H (pb) |
| 10.00 | 1.392E+02 | +0.9 | -1.4 | ±2.0 | 8.281E+01 | 5.643E+01 | |||
| 15.00 | 8.577E+01 | +0.9 | -1.3 | ±2.0 | 5.128E+01 | 3.449E+01 | |||
| 20.00 | 5.708E+01 | +0.6 | -1.2 | ±2.0 | 3.419E+01 | 2.289E+01 | |||
| 25.00 | 3.985E+01 | +0.7 | -1.0 | ±2.0 | 2.396E+01 | 1.589E+01 | |||
| 30.00 | 2.888E+01 | +0.4 | -0.9 | ±2.0 | 1.742E+01 | 1.146E+01 | |||
| 35.00 | 2.151E+01 | +0.3 | -1.1 | ±2.0 | 1.303E+01 | 8.482E+00 | |||
| 40.00 | 1.635E+01 | +0.4 | -0.9 | ±2.0 | 9.925E+00 | 6.423E+00 | |||
| 45.00 | 1.266E+01 | +0.5 | -0.8 | ±2.0 | 7.710E+00 | 4.953E+00 | |||
| 50.00 | 9.959E+00 | +0.4 | -0.9 | ±1.9 | 6.084E+00 | 3.875E+00 | |||
| 55.00 | 7.925E+00 | +0.4 | -0.6 | ±2.0 | 4.853E+00 | 3.072E+00 | |||
| 60.00 | 6.388E+00 | +0.4 | -0.6 | ±2.0 | 3.922E+00 | 2.466E+00 | |||
| 65.00 | 5.204E+00 | +0.4 | -0.6 | ±2.0 | 3.206E+00 | 1.998E+00 | |||
| 70.00 | 4.277E+00 | +0.4 | -0.7 | ±2.0 | 2.641E+00 | 1.636E+00 | |||
| 75.00 | 3.545E+00 | +0.3 | -0.7 | ±2.0 | 2.196E+00 | 1.349E+00 | |||
| 80.00 | 2.961E+00 | +0.3 | -0.7 | ±2.0 | 1.839E+00 | 1.122E+00 | |||
| 85.00 | 2.490E+00 | +0.4 | -0.8 | ±2.0 | 1.549E+00 | 9.407E-01 | |||
| 90.00 | 2.106E+00 | +0.5 | -0.7 | ±2.0 | 1.314E+00 | 7.920E-01 | |||
| 95.00 | 1.793E+00 | +0.4 | -0.8 | ±2.1 | 1.121E+00 | 6.720E-01 | |||
| 100.00 | 1.534E+00 | +0.5 | -0.8 | ±2.1 | 9.613E-01 | 5.724E-01 | |||
| 105.00 | 1.319E+00 | +0.6 | -0.8 | ±2.1 | 8.289E-01 | 4.903E-01 | |||
| 110.00 | 1.139E+00 | +0.5 | -0.8 | ±2.0 | 7.176E-01 | 4.216E-01 | |||
| 115.00 | 9.892E-01 | +0.5 | -0.9 | ±2.1 | 6.243E-01 | 3.649E-01 | |||
| 120.00 | 8.623E-01 | +0.6 | -0.8 | ±2.1 | 5.454E-01 | 3.169E-01 | |||
| 125.00 | 7.541E-01 | +0.6 | -0.9 | ±2.0 | 4.784E-01 | 2.757E-01 | |||
| 130.00 | 6.623E-01 | +0.6 | -0.9 | ±2.1 | 4.209E-01 | 2.414E-01 | |||
| 135.00 | 5.832E-01 | +0.7 | -0.9 | ±2.1 | 3.713E-01 | 2.119E-01 | |||
| 140.00 | 5.152E-01 | +0.7 | -0.9 | ±2.1 | 3.288E-01 | 1.864E-01 | |||
| 145.00 | 4.572E-01 | +0.7 | -0.9 | ±2.2 | 2.923E-01 | 1.649E-01 | |||
| 150.00 | 4.066E-01 | +0.7 | -1.0 | ±2.2 | 2.605E-01 | 1.461E-01 | |||
| 160.00 | 3.239E-01 | +0.8 | -0.9 | ±2.2 | 2.084E-01 | 1.155E-01 | |||
| 170.00 | 2.608E-01 | +0.8 | -0.9 | ±2.3 | 1.685E-01 | 9.231E-02 | |||
| 180.00 | 2.120E-01 | +0.8 | -0.9 | ±2.3 | 1.375E-01 | 7.449E-02 | |||
| 190.00 | 1.736E-01 | +0.9 | -1.0 | ±2.4 | 1.130E-01 | 6.062E-02 | |||
| 200.00 | 1.434E-01 | +0.8 | -1.0 | ±2.4 | 9.370E-02 | 4.970E-02 | |||
| 210.00 | 1.193E-01 | +0.9 | -1.0 | ±2.4 | 7.823E-02 | 4.104E-02 | |||
| 220.00 | 9.978E-02 | +1.0 | -1.0 | ±2.5 | 6.567E-02 | 3.411E-02 | |||
| 230.00 | 8.402E-02 | +0.9 | -1.0 | ±2.5 | 5.549E-02 | 2.853E-02 | |||
| 240.00 | 7.114E-02 | +1.0 | -1.0 | ±2.5 | 4.714E-02 | 2.400E-02 | |||
| 250.00 | 6.053E-02 | +1.0 | -1.1 | ±2.6 | 4.024E-02 | 2.029E-02 | |||
| 260.00 | 5.178E-02 | +1.0 | -1.2 | ±2.6 | 3.453E-02 | 1.725E-02 | |||
| 270.00 | 4.448E-02 | +1.0 | -1.2 | ±2.6 | 2.976E-02 | 1.472E-02 | |||
| 280.00 | 3.837E-02 | +1.1 | -1.2 | ±2.7 | 2.576E-02 | 1.261E-02 | |||
| 290.00 | 3.324E-02 | +1.1 | -1.3 | ±2.7 | 2.238E-02 | 1.086E-02 | |||
| 300.00 | 2.888E-02 | +1.2 | -1.3 | ±2.7 | 1.950E-02 | 9.382E-03 | |||
| 310.00 | 2.520E-02 | +1.2 | -1.3 | ±2.8 | 1.706E-02 | 8.137E-03 | |||
| 320.00 | 2.205E-02 | +1.2 | -1.4 | ±2.8 | 1.497E-02 | 7.079E-03 | |||
| 330.00 | 1.936E-02 | +1.2 | -1.4 | ±2.8 | 1.318E-02 | 6.179E-03 | |||
| 340.00 | 1.705E-02 | +1.2 | -1.5 | ±2.9 | 1.164E-02 | 5.408E-03 | |||
| 350.00 | 1.506E-02 | +1.2 | -1.5 | ±3.0 | 1.031E-02 | 4.748E-03 | |||
| 360.00 | 1.333E-02 | +1.3 | -1.5 | ±3.0 | 9.148E-03 | 4.181E-03 | |||
| 370.00 | 1.183E-02 | +1.3 | -1.5 | ±3.1 | 8.139E-03 | 3.690E-03 | |||
| 380.00 | 1.052E-02 | +1.3 | -1.6 | ±3.2 | 7.258E-03 | 3.264E-03 | |||
| 390.00 | 9.382E-03 | +1.3 | -1.6 | ±3.2 | 6.487E-03 | 2.895E-03 | |||
| 400.00 | 8.384E-03 | +1.4 | -1.6 | ±3.3 | 5.810E-03 | 2.574E-03 | |||
| 410.00 | 7.505E-03 | +1.4 | -1.6 | ±3.3 | 5.213E-03 | 2.292E-03 | |||
| 420.00 | 6.734E-03 | +1.4 | -1.7 | ±3.4 | 4.688E-03 | 2.046E-03 | |||
| 430.00 | 6.053E-03 | +1.4 | -1.7 | ±3.5 | 4.224E-03 | 1.829E-03 | |||
| 440.00 | 5.451E-03 | +1.4 | -1.8 | ±3.6 | 3.812E-03 | 1.639E-03 | |||
| 450.00 | 4.917E-03 | +1.4 | -1.8 | ±3.6 | 3.446E-03 | 1.471E-03 | |||
| 460.00 | 4.442E-03 | +1.4 | -1.8 | ±3.7 | 3.119E-03 | 1.323E-03 | |||
| 470.00 | 4.019E-03 | +1.4 | -1.8 | ±3.8 | 2.828E-03 | 1.191E-03 | |||
| 480.00 | 3.642E-03 | +1.5 | -1.9 | ±3.9 | 2.568E-03 | 1.074E-03 | |||
| 490.00 | 3.305E-03 | +1.5 | -1.9 | ±4.0 | 2.335E-03 | 9.703E-04 | |||
| 500.00 | 3.003E-03 | +1.5 | -1.9 | ±4.1 | 2.125E-03 | 8.780E-04 | |||
| 550.00 | 1.896E-03 | +1.6 | -2.0 | ±4.5 | 1.354E-03 | 5.423E-04 | |||
| 600.00 | 1.230E-03 | +1.7 | -2.1 | ±4.9 | 8.850E-04 | 3.449E-04 | |||
| 650.00 | 8.162E-04 | +1.8 | -2.3 | ±5.3 | 5.914E-04 | 2.248E-04 | |||
| 700.00 | 5.522E-04 | +1.8 | -2.4 | ±5.7 | 4.026E-04 | 1.496E-04 | |||
| 750.00 | 3.797E-04 | +1.9 | -2.5 | ±6.1 | 2.783E-04 | 1.014E-04 | |||
| 800.00 | 2.647E-04 | +2.0 | -2.6 | ±6.6 | 1.949E-04 | 6.978E-05 | |||
| 850.00 | 1.868E-04 | +2.0 | -2.7 | ±7.0 | 1.381E-04 | 4.869E-05 | |||
| 900.00 | 1.332E-04 | +2.1 | -2.8 | ±7.4 | 9.883E-05 | 3.439E-05 | |||
| 950.00 | 9.590E-05 | +2.2 | -2.9 | ±7.8 | 7.134E-05 | 2.456E-05 | |||
| 1000.00 | 6.961E-05 | +2.2 | -3.1 | ±8.2 | 5.190E-05 | 1.771E-05 | |||
| 1050.00 | 5.087E-05 | +2.3 | -3.2 | ±11.0 | 3.799E-05 | 1.288E-05 | |||
| 1100.00 | 3.742E-05 | +2.3 | -3.3 | ±13.9 | 2.798E-05 | 9.439E-06 | |||
| 1150.00 | 2.768E-05 | +2.4 | -3.4 | ±16.8 | 2.071E-05 | 6.967E-06 | |||
| 1200.00 | 2.058E-05 | +2.5 | -3.5 | ±19.7 | 1.540E-05 | 5.176E-06 | |||
| 1250.00 | 1.536E-05 | +2.5 | -3.5 | ±22.6 | 1.149E-05 | 3.868E-06 | |||
| 1300.00 | 1.151E-05 | +2.6 | -3.6 | ±25.5 | 8.607E-06 | 2.907E-06 | |||
| 1350.00 | 8.661E-06 | +2.7 | -3.7 | ±28.3 | 6.466E-06 | 2.195E-06 | |||
| 1400.00 | 6.537E-06 | +2.8 | -3.8 | ±31.1 | 4.872E-06 | 1.665E-06 | |||
| 1450.00 | 4.946E-06 | +2.8 | -3.9 | ±34.0 | 3.678E-06 | 1.268E-06 | |||
| 1500.00 | 3.751E-06 | +2.9 | -4.0 | ±36.8 | 2.781E-06 | 9.697E-07 | |||
| 1550.00 | 2.851E-06 | +3.0 | -4.1 | ±39.6 | 2.107E-06 | 7.441E-07 | |||
| 1600.00 | 2.171E-06 | +3.0 | -4.3 | ±42.4 | 1.598E-06 | 5.729E-07 | |||
| 1650.00 | 1.656E-06 | +3.1 | -4.4 | ±45.1 | 1.213E-06 | 4.425E-07 | |||
| 1700.00 | 1.264E-06 | +3.2 | -4.5 | ±47.7 | 9.215E-07 | 3.426E-07 | |||
| 1750.00 | 9.664E-07 | +3.3 | -4.6 | ±50.4 | 7.004E-07 | 2.660E-07 | |||
| 1800.00 | 7.394E-07 | +3.4 | -4.7 | ±53.0 | 5.323E-07 | 2.071E-07 | |||
| 1850.00 | 5.660E-07 | +3.5 | -4.8 | ±55.6 | 4.044E-07 | 1.616E-07 | |||
| 1900.00 | 4.336E-07 | +3.6 | -4.9 | ±58.1 | 3.072E-07 | 1.264E-07 | |||
| 1950.00 | 3.320E-07 | +3.7 | -5.1 | ±60.5 | 2.330E-07 | 9.900E-08 | |||
| 2000.00 | 2.543E-07 | +3.8 | -5.2 | ±62.9 | 1.766E-07 | 7.770E-08 |
ZH Process
- Cross sections are calculated at NNLO QCD accuracy.
- Calculations are the same as CERN Report 3.
- gg→ZH (box-diagram) occurs as a part of NNLO QCD correction and included in the total cross section.
- Program: NNLO QCD (VH@NNLO)
- QCD scales: μ=μF=μR=MVH=(pV+pH)2 for QCD 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)
- Photon-induced contribution of O(1%) or below
- NOT included for total cross section (agrees with CERN Report 3 numbers).
| mH (GeV) | Cross Section (pb) | +QCD Scale % | -QCD Scale % | ±(PDF+αs) % | ±PDF % | ±αs % | 1+δEW | σ(gg→ZH) (pb) |
| 10.00 | 6.051E+01 | +0.8 | -1.3 | ±2.1 | ||||
| 15.00 | 3.824E+01 | +0.6 | -1.2 | ±2.1 | ||||
| 20.00 | 2.602E+01 | +0.4 | -1.2 | ±2.1 | ||||
| 25.00 | 1.847E+01 | +0.7 | -0.8 | ±2.1 | ||||
| 30.00 | 1.364E+01 | +0.3 | -0.9 | ±2.1 | ||||
| 35.00 | 1.030E+01 | +0.5 | -0.8 | ±2.1 | ||||
| 40.00 | 7.936E+00 | +0.6 | -0.6 | ±2.1 | ||||
| 45.00 | 6.237E+00 | +0.6 | -0.9 | ±2.1 | ||||
| 50.00 | 4.963E+00 | +0.7 | -0.8 | ±2.1 | ||||
| 55.00 | 4.002E+00 | +0.8 | -0.9 | ±2.0 | ||||
| 60.00 | 3.259E+00 | +1.0 | -0.9 | ±2.0 | ||||
| 65.00 | 2.685E+00 | +1.1 | -1.0 | ±2.0 | ||||
| 70.00 | 2.232E+00 | +1.2 | -1.2 | ±1.9 | ||||
| 75.00 | 1.869E+00 | +1.2 | -1.2 | ±1.9 | ||||
| 80.00 | 1.577E+00 | +1.3 | -1.4 | ±1.8 | ||||
| 85.00 | 1.338E+00 | +1.5 | -1.4 | ±1.8 | ||||
| 90.00 | 1.142E+00 | +1.8 | -1.4 | ±1.8 | ||||
| 95.00 | 9.816E-01 | +1.8 | -1.6 | ±1.8 | ||||
| 100.00 | 8.479E-01 | +2.0 | -1.7 | ±1.8 | ||||
| 105.00 | 7.359E-01 | +2.2 | -1.8 | ±1.8 | ||||
| 110.00 | 6.416E-01 | +2.3 | -1.9 | ±1.7 | ||||
| 115.00 | 5.611E-01 | +2.5 | -2.0 | ±1.7 | ||||
| 120.00 | 4.935E-01 | +2.7 | -2.2 | ±1.7 | ||||
| 125.00 | 4.353E-01 | +2.9 | -2.2 | ±1.7 | ||||
| 130.00 | 3.854E-01 | +3.0 | -2.3 | ±1.7 | ||||
| 135.00 | 3.422E-01 | +3.1 | -2.4 | ±1.7 | ||||
| 140.00 | 3.046E-01 | +3.3 | -2.5 | ±1.7 | ||||
| 145.00 | 2.719E-01 | +3.5 | -2.7 | ±1.7 | ||||
| 150.00 | 2.435E-01 | +3.6 | -2.8 | ±1.7 | ||||
| 160.00 | 1.965E-01 | +3.8 | -3.1 | ±1.7 | ||||
| 170.00 | 1.599E-01 | +4.0 | -3.3 | ±1.8 | ||||
| 180.00 | 1.309E-01 | +4.1 | -3.4 | ±1.8 | ||||
| 190.00 | 1.078E-01 | +4.3 | -3.5 | ±1.8 | ||||
| 200.00 | 8.927E-02 | +4.3 | -3.6 | ±1.8 | ||||
| 210.00 | 7.419E-02 | +4.3 | -3.6 | ±1.8 | ||||
| 220.00 | 6.194E-02 | +4.1 | -3.7 | ±1.9 | ||||
| 230.00 | 5.184E-02 | +4.1 | -3.5 | ±1.9 | ||||
| 240.00 | 4.355E-02 | +4.0 | -3.4 | ±2.0 | ||||
| 250.00 | 3.674E-02 | +3.8 | -3.3 | ±2.0 | ||||
| 260.00 | 3.114E-02 | +3.6 | -3.2 | ±2.1 | ||||
| 270.00 | 2.651E-02 | +3.3 | -3.1 | ±2.1 | ||||
| 280.00 | 2.266E-02 | +3.2 | -2.9 | ±2.2 | ||||
| 290.00 | 1.945E-02 | +3.0 | -2.8 | ±2.2 | ||||
| 300.00 | 1.677E-02 | +2.8 | -2.7 | ±2.2 | ||||
| 310.00 | 1.452E-02 | +2.7 | -2.6 | ±2.3 | ||||
| 320.00 | 1.262E-02 | +2.6 | -2.5 | ±2.3 | ||||
| 330.00 | 1.101E-02 | +2.5 | -2.4 | ±2.4 | ||||
| 340.00 | 9.647E-03 | +2.4 | -2.3 | ±2.4 | ||||
| 350.00 | 8.490E-03 | +2.4 | -2.3 | ±2.5 | ||||
| 360.00 | 7.503E-03 | +2.4 | -2.3 | ±2.5 | ||||
| 370.00 | 6.653E-03 | +2.4 | -2.4 | ±2.6 | ||||
| 380.00 | 5.917E-03 | +2.4 | -2.4 | ±2.6 | ||||
| 390.00 | 5.274E-03 | +2.5 | -2.5 | ±2.7 | ||||
| 400.00 | 4.715E-03 | +2.6 | -2.6 | ±2.7 | ||||
| 410.00 | 4.225E-03 | +2.7 | -2.6 | ±2.8 | ||||
| 420.00 | 3.794E-03 | +2.8 | -2.7 | ±2.8 | ||||
| 430.00 | 3.415E-03 | +2.8 | -2.8 | ±2.8 | ||||
| 440.00 | 3.079E-03 | +3.0 | -2.9 | ±2.8 | ||||
| 450.00 | 2.782E-03 | +3.1 | -3.0 | ±2.8 | ||||
| 460.00 | 2.519E-03 | +3.1 | -3.1 | ±2.8 | ||||
| 470.00 | 2.284E-03 | +3.3 | -3.2 | ±2.9 | ||||
| 480.00 | 2.074E-03 | +3.4 | -3.3 | ±2.9 | ||||
| 490.00 | 1.887E-03 | +3.5 | -3.4 | ±2.9 | ||||
| 500.00 | 1.719E-03 | +3.7 | -3.5 | ±2.9 | ||||
| 550.00 | 1.102E-03 | +4.4 | -4.1 | ±3.1 | ||||
| 600.00 | 7.277E-04 | +5.2 | -4.7 | ±3.4 | ||||
| 650.00 | 4.925E-04 | +6.0 | -5.4 | ±3.6 | ||||
| 700.00 | 3.404E-04 | +6.7 | -6.1 | ±3.8 | ||||
| 750.00 | 2.395E-04 | +7.5 | -6.8 | ±4.0 | ||||
| 800.00 | 1.710E-04 | +8.3 | -7.4 | ±4.2 | ||||
| 850.00 | 1.236E-04 | +9.0 | -8.1 | ±4.4 | ||||
| 900.00 | 9.037E-05 | +9.9 | -8.7 | ±4.7 | ||||
| 950.00 | 6.673E-05 | +10.7 | -9.2 | ±4.9 | ||||
| 1000.00 | 4.968E-05 | +11.5 | -9.8 | ±5.1 | ||||
| 1050.00 | 3.734E-05 | +12.2 | -10.4 | ±5.5 | ||||
| 1100.00 | 2.821E-05 | +13.0 | -11.0 | ±5.9 | ||||
| 1150.00 | 2.147E-05 | +13.6 | -11.6 | ±6.3 | ||||
| 1200.00 | 1.642E-05 | +14.2 | -12.2 | ±6.7 | ||||
| 1250.00 | 1.261E-05 | +15.1 | -12.6 | ±7.1 | ||||
| 1300.00 | 9.739E-06 | +15.8 | -13.1 | ±7.5 | ||||
| 1350.00 | 7.553E-06 | +16.4 | -13.6 | ±7.9 | ||||
| 1400.00 | 5.881E-06 | +17.0 | -14.2 | ±8.3 | ||||
| 1450.00 | 4.591E-06 | +17.9 | -14.5 | ±8.7 | ||||
| 1500.00 | 3.600E-06 | +18.5 | -15.1 | ±9.1 | ||||
| 1550.00 | 2.829E-06 | +19.1 | -15.6 | ±9.5 | ||||
| 1600.00 | 2.230E-06 | +19.7 | -16.1 | ±9.9 | ||||
| 1650.00 | 1.761E-06 | +20.4 | -16.5 | ±10.2 | ||||
| 1700.00 | 1.395E-06 | +21.0 | -16.9 | ±10.6 | ||||
| 1750.00 | 1.107E-06 | +21.6 | -17.4 | ±11.0 | ||||
| 1800.00 | 8.799E-07 | +22.3 | -17.8 | ±11.4 | ||||
| 1850.00 | 7.005E-07 | +22.9 | -18.2 | ±11.8 | ||||
| 1900.00 | 5.586E-07 | +23.6 | -18.5 | ±12.2 | ||||
| 1950.00 | 4.460E-07 | +24.1 | -18.9 | ±12.6 | ||||
| 2000.00 | 3.571E-07 | +24.6 | -19.3 | ±13.6 |
ttH Process
- Cross sections are calculated at NLO QCD accuracy.
- Calculations are the same as CERN Report 3.
- 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 % | 1+δEW |
| 10.00 | 7.926E+00 | +7.1 | -10.6 | ±3.9 | ±3.4 | ±2.0 | 0.984 |
| 30.00 | 2.562E+00 | +6.4 | -10.3 | ±4.0 | ±3.5 | ±2.0 | 1.011 |
| 70.00 | 5.830E-01 | +5.2 | -9.8 | ±4.2 | ±3.6 | ±2.1 | 1.025 |
| 100.00 | 2.441E-01 | +4.5 | -9.4 | ±4.2 | ±3.7 | ±2.1 | 1.029 |
| 120.00 | 1.461E-01 | +4.1 | -9.2 | ±4.3 | ±3.7 | ±2.1 | 1.027 |
| 125.00 | 1.296E-01 | +4.1 | -9.2 | ±4.3 | ±3.7 | ±2.1 | 1.026 |
| 130.00 | 1.152E-01 | +4.0 | -9.2 | ±4.3 | ±3.7 | ±2.2 | 1.025 |
| 150.00 | 7.364E-02 | +3.7 | -9.1 | ±4.4 | ±3.8 | ±2.2 | 1.016 |
| 200.00 | 2.850E-02 | +3.5 | -9.1 | ±4.7 | ±4.1 | ±2.2 | 1.006 |
| 250.00 | 1.361E-02 | +4.1 | -9.5 | ±5.2 | ±4.6 | ±2.3 | 1.003 |
| 300.00 | 7.637E-03 | +5.0 | -10.3 | ±5.8 | ±5.3 | ±2.4 | 1.018 |
| 400.00 | 3.244E-03 | +6.9 | -11.7 | ±7.4 | ±6.9 | ±2.7 | 1.016 |
| 500.00 | 1.645E-03 | +8.7 | -13.0 | ±8.8 | ±8.3 | ±2.9 | 1.034 |
| 750.00 | 3.840E-04 | +11.4 | -14.8 | ±11.9 | ±11.3 | ±3.6 | 1.153 |
| 1000.00 | 1.000E-04 | +12.9 | -15.9 | ±15.0 | ±14.3 | ±4.4 | 1.197 |
| 1500.00 | 8.181E-06 | +15.0 | -17.4 | ±21.8 | ±20.8 | ±6.5 | 1.522 |
| 2000.00 | 7.601E-07 | +17.1 | -18.8 | ±29.3 | ±27.8 | ±9.1 | 1.547 |
| 2500.00 | 7.201E-08 | +18.8 | -19.9 | ±37.6 | ±35.4 | ±12.8 | 3.082 |
| 3000.00 | 6.456E-09 | +20.5 | -20.8 | ±47.6 | ±43.9 | ±18.2 | 2.095 |
bbH Process
- The cross sections are the Santander matched numbers with 5FS (NNLO) and 4FS (NLO).
- 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) % | 1+δEW |
| 10.00 | 6.366E+01 | +84.0 | -56.2 | |
| 15.00 | 3.458E+01 | +60.6 | -48.7 | |
| 20.00 | 2.171E+01 | +48.8 | -43.6 | |
| 25.00 | 1.450E+01 | +45.0 | -39.8 | |
| 30.00 | 9.894E+00 | +38.2 | -36.8 | |
| 35.00 | 7.077E+00 | +35.2 | -34.4 | |
| 40.00 | 5.161E+00 | +33.8 | -36.9 | |
| 45.00 | 3.900E+00 | +32.5 | -38.0 | |
| 50.00 | 2.991E+00 | +31.0 | -37.5 | |
| 55.00 | 2.351E+00 | +29.5 | -36.3 | |
| 60.00 | 1.871E+00 | +28.1 | -35.0 | |
| 65.00 | 1.510E+00 | +27.2 | -33.6 | |
| 70.00 | 1.228E+00 | +26.2 | -32.1 | |
| 75.00 | 1.012E+00 | +25.7 | -30.9 | |
| 80.00 | 8.349E-01 | +24.8 | -29.7 | |
| 85.00 | 6.966E-01 | +24.2 | -28.6 | |
| 90.00 | 5.842E-01 | +23.6 | -27.6 | |
| 95.00 | 4.955E-01 | +23.1 | -26.6 | |
| 100.00 | 4.215E-01 | +22.5 | -25.7 | |
| 105.00 | 3.595E-01 | +22.2 | -24.9 | |
| 110.00 | 3.094E-01 | +21.8 | -24.2 | |
| 115.00 | 2.665E-01 | +21.0 | -23.5 | |
| 120.00 | 2.315E-01 | +20.8 | -22.8 | |
| 125.00 | 2.021E-01 | +20.7 | -22.3 | |
| 130.00 | 1.763E-01 | +20.3 | -21.9 | |
| 135.00 | 1.550E-01 | +20.1 | -21.6 | |
| 140.00 | 1.364E-01 | +19.7 | -21.3 | |
| 145.00 | 1.203E-01 | +19.3 | -20.9 | |
| 150.00 | 1.066E-01 | +19.1 | -20.7 | |
| 160.00 | 8.430E-02 | +18.7 | -20.1 | |
| 170.00 | 6.734E-02 | +18.2 | -19.7 | |
| 180.00 | 5.441E-02 | +18.0 | -19.3 | |
| 190.00 | 4.434E-02 | +17.8 | -19.0 | |
| 200.00 | 3.636E-02 | +17.5 | -18.7 | |
| 210.00 | 3.004E-02 | +17.3 | -18.5 | |
| 220.00 | 2.494E-02 | +16.9 | -18.2 | |
| 230.00 | 2.088E-02 | +16.9 | -18.0 | |
| 240.00 | 1.755E-02 | +16.8 | -17.8 | |
| 250.00 | 1.484E-02 | +16.9 | -17.6 | |
| 260.00 | 1.262E-02 | +16.9 | -17.4 | |
| 270.00 | 1.076E-02 | +16.7 | -17.3 | |
| 280.00 | 9.229E-03 | +16.6 | -17.2 | |
| 290.00 | 7.945E-03 | +16.8 | -17.1 | |
| 300.00 | 6.846E-03 | +16.7 | -17.0 | |
| 310.00 | 5.935E-03 | +16.6 | -17.0 | |
| 320.00 | 5.156E-03 | +16.4 | -16.9 | |
| 330.00 | 4.494E-03 | +16.4 | -16.8 | |
| 340.00 | 3.937E-03 | +16.6 | -16.8 | |
| 350.00 | 3.451E-03 | +16.7 | -16.7 | |
| 360.00 | 3.033E-03 | +16.7 | -16.7 | |
| 370.00 | 2.674E-03 | +16.9 | -16.8 | |
| 380.00 | 2.361E-03 | +16.9 | -16.7 | |
| 390.00 | 2.095E-03 | +17.1 | -16.8 | |
| 400.00 | 1.860E-03 | +17.2 | -16.8 | |
| 410.00 | 1.653E-03 | +17.3 | -16.8 | |
| 420.00 | 1.474E-03 | +17.5 | -16.8 | |
| 430.00 | 1.317E-03 | +17.5 | -16.8 | |
| 440.00 | 1.177E-03 | +17.6 | -16.8 | |
| 450.00 | 1.055E-03 | +17.8 | -16.8 | |
| 460.00 | 9.463E-04 | +17.9 | -16.8 | |
| 470.00 | 8.517E-04 | +18.0 | -16.7 | |
| 480.00 | 7.668E-04 | +18.2 | -16.8 | |
| 490.00 | 6.913E-04 | +18.2 | -16.8 | |
| 500.00 | 6.256E-04 | +18.4 | -16.9 | |
| 550.00 | 3.832E-04 | +19.1 | -17.3 | |
| 600.00 | 2.418E-04 | +19.9 | -17.7 | |
| 650.00 | 1.567E-04 | +20.2 | -18.4 | |
| 700.00 | 1.037E-04 | +20.5 | -19.1 | |
| 750.00 | 6.987E-05 | +20.8 | -20.0 | |
| 800.00 | 4.789E-05 | +21.2 | -21.0 | |
| 850.00 | 3.326E-05 | +21.8 | -22.4 | |
| 900.00 | 2.346E-05 | +22.5 | -23.7 | |
| 950.00 | 1.672E-05 | +23.4 | -25.1 | |
| 1000.00 | 1.205E-05 | +24.8 | -26.0 | |
| 1050.00 | 8.756E-06 | +26.2 | -27.0 | |
| 1100.00 | 6.423E-06 | +27.7 | -28.0 | |
| 1150.00 | 4.747E-06 | +28.9 | -29.0 | |
| 1200.00 | 3.537E-06 | +30.1 | -30.1 | |
| 1250.00 | 2.653E-06 | +31.3 | -31.3 | |
| 1300.00 | 2.000E-06 | +32.4 | -32.4 | |
| 1350.00 | 1.517E-06 | +33.5 | -34.0 | |
| 1400.00 | 1.158E-06 | +34.8 | -35.8 | |
| 1450.00 | 8.871E-07 | +36.5 | -37.7 | |
| 1500.00 | 6.828E-07 | +38.3 | -39.5 | |
| 1550.00 | 5.273E-07 | +39.9 | -41.4 | |
| 1600.00 | 4.096E-07 | +41.6 | -43.3 | |
| 1650.00 | 3.188E-07 | +43.4 | -45.2 | |
| 1700.00 | 2.489E-07 | +45.5 | -46.8 | |
| 1750.00 | 1.949E-07 | +47.7 | -48.4 | |
| 1800.00 | 1.533E-07 | +50.1 | -49.9 | |
| 1850.00 | 1.200E-07 | +52.5 | -51.7 | |
| 1900.00 | 9.539E-08 | +55.0 | -53.2 | |
| 1950.00 | 7.518E-08 | +57.7 | -55.0 | |
| 2000.00 | 5.992E-08 | +59.5 | -56.3 | |
| 2050.00 | 4.764E-08 | +60.1 | -57.8 | |
| 2100.00 | 3.804E-08 | +60.5 | -59.1 | |
| 2150.00 | 3.028E-08 | +60.9 | -61.6 | |
| 2200.00 | 2.407E-08 | +61.8 | -64.0 | |
| 2250.00 | 1.937E-08 | +64.6 | -65.8 | |
| 2300.00 | 1.551E-08 | +67.6 | -68.0 | |
| 2350.00 | 1.245E-08 | +70.7 | -70.3 | |
| 2400.00 | 1.001E-08 | +74.0 | -72.6 | |
| 2450.00 | 8.063E-09 | +77.3 | -74.9 | |
| 2500.00 | 6.396E-09 | +81.5 | -78.0 | |
| 2550.00 | 5.217E-09 | +84.6 | -80.0 | |
| 2600.00 | 4.206E-09 | +88.5 | -82.7 | |
| 2650.00 | 3.421E-09 | +92.0 | -85.0 | |
| 2700.00 | 2.742E-09 | +95.6 | -88.2 | |
| 2750.00 | 2.215E-09 | +97.5 | -91.0 | |
| 2800.00 | 1.798E-09 | +99.2 | -93.7 | |
| 2850.00 | 1.448E-09 | +103.0 | -96.8 | |
| 2900.00 | 1.171E-09 | +107.5 | -99.9 | |
| 2950.00 | 9.427E-10 | +112.1 | -103.3 | |
| 3000.00 | 7.647E-10 | +112.7 | -105.4 |
tH Process (t-ch)
- Cross sections are calculated at NLO QCD accuracy 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 % | 1+δEW | tH (pb) | tbarH (pb) |
tH Process (s-ch)
- Cross sections are calculated at NLO QCD accuracy 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 % | 1+δEW | tH (pb) | tbarH (pb) |
Topic revision: r18 - 2023-11-13 - TatsuyaMasubuchi
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