BSM 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.
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:
- 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
N3LO
- Cross section in the effective field theory (EFT) by Zürich group at N3LO QCD [Anastasiou:2016hlm].
- Lagrangian includes a direct Yukawa interaction between the scalar S and the top quark
where λt is the ratio of the Yukawa coupling of the scalar S and the Yukawa coupling of the Higgs boson to the top quark and λwc=CS/C denotes the ratio of the effective coefficient of a higher dimensional operator of the scalar S and that of the Standard Model Higgs after integrating out the top-quark.
- Numbers in the table are with λwc=1 and λt=0 in NWA (ΓS=0). In particular, this configuration corresponds to the prediction of the Higgs boson gluon fusion cross section in the infinite top quark mass limit. No additional mass or electro-weak effects are considered.
- QCD scales: μ=μF=μR=MS/2 varied in the range of [MS/4,MS].
- 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.
- PDF set: PDF4LHC15_nnlo_100
NNLO+NNLL
- Cross section for SM-like coupling heavy Higgs boson.
- 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.
- 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).
- Includes top- and bottom-quark mass effects up to NLO.
- 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 |
mS or mH (GeV) |
Cross Section (pb) |
+Theory % |
-Theory % |
TH Gaussian % |
±(PDF+αs) % |
|
Cross Section (pb) |
+QCD Scale % |
-QCD Scale % |
±(PDF+αs) % |
±PDF % |
±αs % |
1+δEW |
10.00 |
1.900E+03 |
+17.8 |
-21.3 |
±12.3 |
±12.2 |
|
6.996E+03 |
+49.9 |
-38.9 |
±8.0 |
±7.5 |
±2.7 |
0 |
15.00 |
1.203E+03 |
+11.6 |
-15.0 |
±8.7 |
±6.7 |
|
4.275E+03 |
+34.8 |
-29.2 |
±5.9 |
±5.1 |
±2.9 |
0 |
20.00 |
8.458E+02 |
+8.8 |
-11.8 |
±6.8 |
±5.4 |
|
2.085E+03 |
+25.7 |
-22.5 |
±4.8 |
±3.7 |
±3.0 |
0 |
25.00 |
6.322E+02 |
+7.1 |
-10.0 |
±5.8 |
±4.9 |
|
1.146E+03 |
+20.8 |
-18.2 |
±4.3 |
±3.1 |
±3.0 |
0 |
30.00 |
4.923E+02 |
+6.1 |
-8.8 |
±5.1 |
±4.6 |
|
7.103E+02 |
+18.5 |
-15.6 |
±4.2 |
±2.8 |
±3.1 |
0 |
35.00 |
3.949E+02 |
+5.5 |
-7.8 |
±4.5 |
±4.3 |
|
4.846E+02 |
+16.3 |
-13.9 |
±4.0 |
±2.6 |
±3.1 |
0 |
40.00 |
3.240E+02 |
+4.8 |
-7.3 |
±4.2 |
±4.2 |
|
3.555E+02 |
+14.8 |
-12.9 |
±3.9 |
±2.4 |
±3.1 |
0 |
45.00 |
2.706E+02 |
+4.3 |
-6.7 |
±3.9 |
±4.0 |
|
2.751E+02 |
+13.5 |
-12.1 |
±3.8 |
±2.3 |
±3.0 |
0 |
50.00 |
2.294E+02 |
+3.7 |
-6.0 |
±3.5 |
±4.0 |
|
2.214E+02 |
+12.5 |
-11.6 |
±3.7 |
±2.2 |
±3.0 |
0 |
55.00 |
1.968E+02 |
+3.5 |
-5.7 |
±3.3 |
±3.8 |
|
1.835E+02 |
+11.7 |
-11.1 |
±3.7 |
±2.2 |
±2.9 |
0 |
60.00 |
1.706E+02 |
+3.2 |
-5.4 |
±3.1 |
±3.7 |
|
1.555E+02 |
+11.1 |
-10.7 |
±3.6 |
±2.1 |
±2.9 |
0 |
65.00 |
1.492E+02 |
+3.1 |
-5.2 |
±3.0 |
±3.7 |
|
1.341E+02 |
+10.5 |
-10.3 |
±3.5 |
±2.1 |
±2.9 |
0 |
70.00 |
1.315E+02 |
+2.8 |
-4.9 |
±2.8 |
±3.6 |
|
1.172E+02 |
+10.1 |
-10.0 |
±3.5 |
±2.0 |
±2.8 |
0 |
75.00 |
1.166E+02 |
+2.6 |
-4.7 |
±2.7 |
±3.6 |
|
1.036E+02 |
+9.7 |
-9.7 |
±3.4 |
±2.0 |
±2.8 |
0 |
80.00 |
1.041E+02 |
+2.5 |
-4.7 |
±2.7 |
±3.5 |
|
9.240E+01 |
+9.4 |
-9.5 |
±3.4 |
±2.0 |
±2.7 |
0 |
85.00 |
9.340E+01 |
+2.4 |
-4.5 |
±2.6 |
±3.5 |
|
8.302E+01 |
+9.1 |
-9.3 |
±3.3 |
±1.9 |
±2.7 |
0 |
90.00 |
8.420E+01 |
+2.3 |
-4.3 |
±2.5 |
±3.4 |
|
7.507E+01 |
+8.8 |
-9.1 |
±3.3 |
±1.9 |
±2.7 |
0 |
95.00 |
7.630E+01 |
+2.2 |
-4.1 |
±2.4 |
±3.4 |
|
6.825E+01 |
+8.6 |
-8.9 |
±3.3 |
±1.9 |
±2.6 |
0 |
100.00 |
6.930E+01 |
+2.0 |
-4.0 |
±2.3 |
±3.4 |
|
6.235E+01 |
+8.4 |
-8.8 |
±3.2 |
±1.9 |
±2.6 |
1.0418 |
105.00 |
6.320E+01 |
+2.0 |
-3.9 |
±2.3 |
±3.3 |
|
5.720E+01 |
+8.2 |
-8.6 |
±3.2 |
±1.9 |
±2.6 |
1.0436 |
110.00 |
5.790E+01 |
+1.9 |
-3.9 |
±2.3 |
±3.3 |
|
5.268E+01 |
+8.0 |
-8.5 |
±3.2 |
±1.9 |
±2.6 |
1.0455 |
115.00 |
5.310E+01 |
+1.8 |
-3.8 |
±2.2 |
±3.3 |
|
4.869E+01 |
+7.9 |
-8.3 |
±3.1 |
±1.8 |
±2.5 |
1.0474 |
120.00 |
4.890E+01 |
+1.8 |
-3.7 |
±2.1 |
±3.2 |
|
4.514E+01 |
+7.7 |
-8.2 |
±3.1 |
±1.8 |
±2.5 |
1.0494 |
125.00 |
4.520E+01 |
+1.7 |
-3.7 |
±2.1 |
±3.2 |
|
4.198E+01 |
+7.6 |
-8.1 |
±3.1 |
±1.8 |
±2.5 |
1.0514 |
130.00 |
4.180E+01 |
+1.7 |
-3.6 |
±2.1 |
±3.2 |
|
3.914E+01 |
+7.5 |
-8.0 |
±3.1 |
±1.8 |
±2.5 |
1.0534 |
135.00 |
3.880E+01 |
+1.6 |
-3.5 |
±2.0 |
±3.2 |
|
3.659E+01 |
+7.4 |
-7.9 |
±3.1 |
±1.8 |
±2.5 |
1.0553 |
140.00 |
3.600E+01 |
+1.6 |
-3.5 |
±2.0 |
±3.2 |
|
3.428E+01 |
+7.2 |
-7.8 |
±3.0 |
±1.8 |
±2.5 |
1.0571 |
145.00 |
3.350E+01 |
+1.5 |
-3.5 |
±2.0 |
±3.2 |
|
3.219E+01 |
+7.1 |
-7.7 |
±3.0 |
±1.8 |
±2.4 |
1.0587 |
150.00 |
3.129E+01 |
+1.5 |
-3.4 |
±2.0 |
±3.1 |
|
3.029E+01 |
+7.0 |
-7.6 |
±3.0 |
±1.8 |
±2.4 |
1.0598 |
160.00 |
2.737E+01 |
+1.5 |
-3.3 |
±1.9 |
±3.1 |
|
2.697E+01 |
+6.9 |
-7.5 |
±3.0 |
±1.8 |
±2.4 |
1.0486 |
170.00 |
2.409E+01 |
+1.4 |
-3.2 |
±1.8 |
±3.1 |
|
2.419E+01 |
+6.7 |
-7.4 |
±3.0 |
±1.8 |
±2.4 |
1.0206 |
180.00 |
2.132E+01 |
+1.3 |
-3.2 |
±1.8 |
±3.1 |
|
2.184E+01 |
+6.5 |
-7.2 |
±2.9 |
±1.8 |
±2.4 |
1.0053 |
190.00 |
1.896E+01 |
+1.3 |
-3.1 |
±1.8 |
±3.0 |
|
1.984E+01 |
+6.4 |
-7.1 |
±2.9 |
±1.7 |
±2.3 |
0.9872 |
200.00 |
1.694E+01 |
+1.3 |
-3.2 |
±1.8 |
±3.0 |
|
1.812E+01 |
+6.3 |
-7.0 |
±2.9 |
±1.7 |
±2.3 |
0.9793 |
210.00 |
1.520E+01 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.665E+01 |
+6.2 |
-6.9 |
±2.9 |
±1.7 |
±2.3 |
0.9761 |
220.00 |
1.369E+01 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.537E+01 |
+6.1 |
-6.8 |
±2.9 |
±1.7 |
±2.3 |
0.9749 |
230.00 |
1.237E+01 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.426E+01 |
+6.0 |
-6.7 |
±2.9 |
±1.7 |
±2.3 |
0.9749 |
240.00 |
1.122E+01 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.331E+01 |
+5.9 |
-6.6 |
±2.9 |
±1.7 |
±2.3 |
0.9755 |
250.00 |
1.020E+01 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.248E+01 |
+5.9 |
-6.5 |
±2.9 |
±1.8 |
±2.3 |
0.9762 |
260.00 |
9.300E+00 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.176E+01 |
+5.8 |
-6.5 |
±2.9 |
±1.8 |
±2.3 |
0.9772 |
270.00 |
8.510E+00 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.114E+01 |
+5.8 |
-6.4 |
±2.9 |
±1.8 |
±2.3 |
0.9783 |
280.00 |
7.800E+00 |
+1.4 |
-3.2 |
±1.8 |
±3.0 |
|
1.062E+01 |
+5.8 |
-6.3 |
±2.9 |
±1.8 |
±2.2 |
0.9795 |
290.00 |
7.160E+00 |
+1.5 |
-3.2 |
±1.8 |
±3.0 |
|
1.018E+01 |
+5.8 |
-6.3 |
±2.9 |
±1.8 |
±2.2 |
0.9805 |
300.00 |
6.590E+00 |
+1.5 |
-3.2 |
±1.8 |
±3.0 |
|
9.823E+00 |
+5.8 |
-6.2 |
±2.9 |
±1.8 |
±2.2 |
0.9813 |
310.00 |
6.080E+00 |
+1.5 |
-3.3 |
±1.9 |
±3.0 |
|
9.559E+00 |
+5.7 |
-6.1 |
±2.9 |
±1.8 |
±2.2 |
0.9819 |
320.00 |
5.620E+00 |
+1.5 |
-3.2 |
±1.8 |
±3.0 |
|
9.392E+00 |
+5.7 |
-6.1 |
±2.9 |
±1.8 |
±2.2 |
0.982 |
330.00 |
5.200E+00 |
+1.5 |
-3.3 |
±1.9 |
±3.0 |
|
9.349E+00 |
+5.7 |
-6.0 |
±2.9 |
±1.8 |
±2.2 |
0.9813 |
340.00 |
4.820E+00 |
+1.5 |
-3.3 |
±1.9 |
±3.0 |
|
9.521E+00 |
+5.7 |
-5.9 |
±2.9 |
±1.8 |
±2.2 |
0.9779 |
350.00 |
4.480E+00 |
+1.5 |
-3.3 |
±1.9 |
±3.0 |
|
1.025E+01 |
+5.7 |
-5.8 |
±2.9 |
±1.8 |
±2.2 |
0.9595 |
360.00 |
4.160E+00 |
+1.5 |
-3.3 |
±1.9 |
±3.0 |
|
1.063E+01 |
+5.7 |
-5.8 |
±2.9 |
±1.9 |
±2.2 |
0.9608 |
370.00 |
3.880E+00 |
+1.6 |
-3.3 |
±1.9 |
±3.0 |
|
1.064E+01 |
+5.7 |
-5.7 |
±2.9 |
±1.9 |
±2.2 |
0.9642 |
380.00 |
3.620E+00 |
+1.6 |
-3.3 |
±1.9 |
±3.0 |
|
1.040E+01 |
+5.7 |
-5.7 |
±2.9 |
±1.9 |
±2.2 |
0.9677 |
390.00 |
3.380E+00 |
+1.6 |
-3.3 |
±1.9 |
±3.1 |
|
1.000E+01 |
+5.7 |
-5.6 |
±2.9 |
±1.9 |
±2.2 |
0.9713 |
400.00 |
3.160E+00 |
+1.6 |
-3.3 |
±1.9 |
±3.1 |
|
9.516E+00 |
+5.7 |
-5.5 |
±2.9 |
±1.9 |
±2.2 |
0.9741 |
410.00 |
2.960E+00 |
+1.6 |
-3.4 |
±2.0 |
±3.1 |
|
8.976E+00 |
+5.7 |
-5.5 |
±3.0 |
±2.0 |
±2.2 |
0.9771 |
420.00 |
2.770E+00 |
+1.6 |
-3.4 |
±2.0 |
±3.1 |
|
8.415E+00 |
+5.7 |
-5.4 |
±3.0 |
±2.0 |
±2.2 |
0.9802 |
430.00 |
2.600E+00 |
+1.6 |
-3.4 |
±2.0 |
±3.1 |
|
7.853E+00 |
+5.7 |
-5.4 |
±3.0 |
±2.0 |
±2.2 |
0.983 |
440.00 |
2.440E+00 |
+1.7 |
-3.4 |
±2.0 |
±3.1 |
|
7.301E+00 |
+5.7 |
-5.3 |
±3.0 |
±2.0 |
±2.2 |
0.9853 |
450.00 |
2.300E+00 |
+1.6 |
-3.4 |
±2.0 |
±3.1 |
|
6.771E+00 |
+5.7 |
-5.3 |
±3.0 |
±2.0 |
±2.2 |
0.9878 |
460.00 |
2.160E+00 |
+1.7 |
-3.4 |
±2.0 |
±3.2 |
|
6.266E+00 |
+5.6 |
-5.2 |
±3.0 |
±2.1 |
±2.2 |
0.99 |
470.00 |
2.030E+00 |
+1.7 |
-3.4 |
±2.0 |
±3.2 |
|
5.788E+00 |
+5.6 |
-5.2 |
±3.1 |
±2.1 |
±2.2 |
0.9921 |
480.00 |
1.920E+00 |
+1.7 |
-3.4 |
±2.0 |
±3.2 |
|
5.341E+00 |
+5.6 |
-5.2 |
±3.1 |
±2.1 |
±2.2 |
0.994 |
490.00 |
1.810E+00 |
+1.7 |
-3.4 |
±2.0 |
±3.2 |
|
4.924E+00 |
+5.6 |
-5.1 |
±3.1 |
±2.1 |
±2.3 |
0.9961 |
500.00 |
1.709E+00 |
+1.7 |
-3.5 |
±2.0 |
±3.3 |
|
4.538E+00 |
+5.6 |
-5.1 |
±3.1 |
±2.2 |
±2.3 |
0.9981 |
550.00 |
1.297E+00 |
+1.8 |
-3.5 |
±2.0 |
±3.4 |
|
3.008E+00 |
+5.5 |
-5.0 |
±3.2 |
±2.3 |
±2.3 |
1.0069 |
600.00 |
1.001E+00 |
+1.8 |
-3.6 |
±2.1 |
±3.5 |
|
2.006E+00 |
+5.5 |
-4.9 |
±3.4 |
±2.5 |
±2.3 |
1.0152 |
650.00 |
7.834E-01 |
+1.9 |
-3.6 |
±2.1 |
±3.7 |
|
1.352E+00 |
+5.5 |
-4.9 |
±3.5 |
±2.6 |
±2.3 |
1.0226 |
700.00 |
6.206E-01 |
+1.9 |
-3.7 |
±2.1 |
±3.8 |
|
9.235E-01 |
+5.4 |
-4.8 |
±3.7 |
±2.8 |
±2.4 |
1.0301 |
750.00 |
4.969E-01 |
+2.0 |
-3.7 |
±2.1 |
±4.0 |
|
6.398E-01 |
+5.4 |
-4.8 |
±3.9 |
±3.0 |
±2.4 |
1.0377 |
800.00 |
4.015E-01 |
+2.0 |
-3.8 |
±2.2 |
±4.2 |
|
4.491E-01 |
+5.5 |
-4.7 |
±4.0 |
±3.2 |
±2.4 |
1.0454 |
850.00 |
3.271E-01 |
+2.1 |
-3.8 |
±2.2 |
±4.4 |
|
3.195E-01 |
+5.5 |
-4.7 |
±4.2 |
±3.4 |
±2.5 |
1.0532 |
900.00 |
2.685E-01 |
+2.1 |
-3.8 |
±2.2 |
±4.6 |
|
2.301E-01 |
+5.5 |
-4.8 |
±4.4 |
±3.6 |
±2.5 |
1.061 |
950.00 |
2.219E-01 |
+2.2 |
-3.9 |
±2.3 |
±4.8 |
|
1.675E-01 |
+5.5 |
-4.8 |
±4.6 |
±3.8 |
±2.6 |
1.0695 |
1000.00 |
1.845E-01 |
+2.2 |
-4.0 |
±2.3 |
±5.0 |
|
1.233E-01 |
+5.5 |
-4.8 |
±4.8 |
±4.0 |
±2.6 |
1.0783 |
1050.00 |
1.542E-01 |
+2.2 |
-4.0 |
±2.3 |
±5.2 |
|
9.159E-02 |
+5.5 |
-4.8 |
±5.0 |
±4.2 |
±2.7 |
1.089 |
1100.00 |
1.295E-01 |
+2.3 |
-4.0 |
±2.3 |
±5.4 |
|
6.868E-02 |
+5.5 |
-4.8 |
±5.2 |
±4.4 |
±2.7 |
1.1004 |
1150.00 |
1.093E-01 |
+2.3 |
-4.1 |
±2.4 |
±5.6 |
|
5.193E-02 |
+5.6 |
-4.9 |
±5.4 |
±4.7 |
±2.8 |
1.1122 |
1200.00 |
9.260E-02 |
+2.3 |
-4.1 |
±2.4 |
±5.9 |
|
3.958E-02 |
+5.6 |
-4.9 |
±5.6 |
±4.9 |
±2.8 |
1.1242 |
1250.00 |
7.880E-02 |
+2.3 |
-4.1 |
±2.4 |
±6.1 |
|
3.040E-02 |
+5.6 |
-4.9 |
±5.9 |
±5.1 |
±2.9 |
1.1364 |
1300.00 |
6.730E-02 |
+2.4 |
-4.2 |
±2.4 |
±6.3 |
|
2.349E-02 |
+5.6 |
-4.9 |
±6.1 |
±5.3 |
±2.9 |
1.1475 |
1350.00 |
5.760E-02 |
+2.3 |
-4.2 |
±2.4 |
±6.6 |
|
1.828E-02 |
+5.6 |
-5.0 |
±6.3 |
±5.6 |
±3.0 |
1.1586 |
1400.00 |
4.950E-02 |
+2.4 |
-4.2 |
±2.4 |
±6.8 |
|
1.431E-02 |
+5.7 |
-5.0 |
±6.5 |
±5.8 |
±3.0 |
1.17 |
1450.00 |
4.270E-02 |
+2.4 |
-4.2 |
±2.4 |
±7.0 |
|
1.126E-02 |
+5.8 |
-5.0 |
±6.8 |
±6.0 |
±3.1 |
1.1816 |
1500.00 |
3.690E-02 |
+2.4 |
-4.3 |
±2.5 |
±7.3 |
|
8.913E-03 |
+5.9 |
-5.1 |
±7.0 |
±6.3 |
±3.2 |
1.1937 |
1550.00 |
3.190E-02 |
+2.5 |
-4.3 |
±2.5 |
±7.6 |
|
7.089E-03 |
+6.1 |
-5.1 |
±7.3 |
±6.5 |
±3.2 |
1.2069 |
1600.00 |
2.770E-02 |
+2.5 |
-4.3 |
±2.5 |
±7.8 |
|
5.666E-03 |
+6.3 |
-5.1 |
±7.5 |
±6.7 |
±3.3 |
1.2206 |
1650.00 |
2.410E-02 |
+2.5 |
-4.4 |
±2.5 |
±8.1 |
|
4.546E-03 |
+6.5 |
-5.2 |
±7.7 |
±7.0 |
±3.3 |
1.2347 |
1700.00 |
2.100E-02 |
+2.5 |
-4.5 |
±2.6 |
±8.5 |
|
3.662E-03 |
+6.8 |
-5.2 |
±8.0 |
±7.2 |
±3.4 |
1.2493 |
1750.00 |
1.838E-02 |
+3.2 |
-4.4 |
±2.5 |
±8.7 |
|
2.965E-03 |
+9.4 |
-3.5 |
±7.5 |
±7.2 |
±1.8 |
1.2644 |
1800.00 |
1.609E-02 |
+2.5 |
-4.4 |
±2.5 |
±8.9 |
|
2.408E-03 |
+9.1 |
-3.9 |
±7.9 |
±7.6 |
±2.1 |
1.2798 |
1850.00 |
1.411E-02 |
+2.6 |
-4.4 |
±2.5 |
±9.1 |
|
1.963E-03 |
+8.8 |
-4.2 |
±8.2 |
±7.9 |
±2.5 |
1.2955 |
1900.00 |
1.239E-02 |
+2.5 |
-4.4 |
±2.5 |
±9.4 |
|
1.606E-03 |
+8.6 |
-4.5 |
±8.6 |
±8.2 |
±2.8 |
1.3117 |
1950.00 |
1.090E-02 |
+2.6 |
-4.5 |
±2.6 |
±9.7 |
|
1.317E-03 |
+8.4 |
-4.7 |
±9.0 |
±8.4 |
±3.1 |
1.3283 |
2000.00 |
9.600E-03 |
+2.6 |
-4.5 |
±2.6 |
±9.7 |
|
1.084E-03 |
+8.3 |
-4.9 |
±9.4 |
±8.7 |
±3.3 |
1.3453 |
2050.00 |
8.470E-03 |
+2.5 |
-4.5 |
±2.6 |
±10.0 |
|
8.953E-04 |
+8.2 |
-5.1 |
±9.7 |
±9.0 |
±3.6 |
1.3627 |
2100.00 |
7.480E-03 |
+2.6 |
-4.5 |
±2.6 |
±10.5 |
|
7.415E-04 |
+8.1 |
-5.3 |
±10.0 |
±9.3 |
±3.8 |
1.3806 |
2150.00 |
6.620E-03 |
+2.6 |
-4.5 |
±2.6 |
±10.8 |
|
6.144E-04 |
+8.1 |
-5.5 |
±10.4 |
±9.6 |
±3.9 |
1.3989 |
2200.00 |
5.860E-03 |
+2.7 |
-4.6 |
±2.7 |
±11.2 |
|
5.108E-04 |
+8.1 |
-5.6 |
±10.7 |
±9.9 |
±4.1 |
1.4176 |
2250.00 |
5.190E-03 |
+2.6 |
-4.6 |
±2.7 |
±11.8 |
|
4.267E-04 |
+8.1 |
-5.7 |
±11.0 |
±10.1 |
±4.2 |
1.4367 |
2300.00 |
4.610E-03 |
+2.6 |
-4.5 |
±2.6 |
±12.0 |
|
3.569E-04 |
+8.1 |
-5.8 |
±11.3 |
±10.4 |
±4.3 |
1.4563 |
2350.00 |
4.090E-03 |
+2.6 |
-4.5 |
±2.6 |
±12.1 |
|
2.988E-04 |
+8.2 |
-5.9 |
±11.6 |
±10.7 |
±4.4 |
1.4763 |
2400.00 |
3.640E-03 |
+2.6 |
-4.5 |
±2.6 |
±12.4 |
|
2.509E-04 |
+8.3 |
-6.0 |
±11.9 |
±11.0 |
±4.5 |
1.4968 |
2450.00 |
3.240E-03 |
+2.5 |
-4.5 |
±2.6 |
±12.7 |
|
2.110E-04 |
+8.3 |
-6.0 |
±12.2 |
±11.3 |
±4.6 |
1.5177 |
2500.00 |
2.890E-03 |
+2.6 |
-4.5 |
±2.6 |
±13.1 |
|
1.778E-04 |
+8.4 |
-6.1 |
±12.5 |
±11.6 |
±4.6 |
1.539 |
2550.00 |
2.570E-03 |
+2.5 |
-4.5 |
±2.6 |
±13.4 |
|
1.499E-04 |
+8.5 |
-6.2 |
±12.8 |
±11.9 |
±4.7 |
0 |
2600.00 |
2.300E-03 |
+2.5 |
-4.5 |
±2.6 |
±13.7 |
|
1.272E-04 |
+8.6 |
-6.2 |
±13.1 |
±12.2 |
±4.8 |
0 |
2650.00 |
2.050E-03 |
+2.6 |
-4.6 |
±2.7 |
±14.1 |
|
1.077E-04 |
+8.7 |
-6.3 |
±13.4 |
±12.5 |
±4.8 |
0 |
2700.00 |
1.830E-03 |
+2.7 |
-4.7 |
±2.7 |
±14.5 |
|
9.121E-05 |
+8.7 |
-6.3 |
±13.7 |
±12.8 |
±4.9 |
0 |
2750.00 |
1.640E-03 |
+2.8 |
-4.8 |
±2.8 |
±14.8 |
|
7.771E-05 |
+8.8 |
-6.4 |
±14.0 |
±13.1 |
±4.9 |
0 |
2800.00 |
1.460E-03 |
+2.9 |
-4.9 |
±2.8 |
±15.2 |
|
6.611E-05 |
+8.9 |
-6.5 |
±14.4 |
±13.5 |
±5.0 |
0 |
2850.00 |
1.310E-03 |
+3.0 |
-5.0 |
±2.9 |
±15.6 |
|
5.636E-05 |
+8.9 |
-6.6 |
±14.7 |
±13.8 |
±5.0 |
0 |
2900.00 |
1.170E-03 |
+3.1 |
-5.2 |
±3.0 |
±15.9 |
|
4.809E-05 |
+8.9 |
-6.7 |
±15.1 |
±14.2 |
±5.1 |
0 |
2950.00 |
1.050E-03 |
+3.2 |
-5.3 |
±3.1 |
±16.3 |
|
4.112E-05 |
+8.9 |
-6.8 |
±15.5 |
±14.6 |
±5.2 |
0 |
3000.00 |
9.400E-04 |
+3.4 |
-5.5 |
±3.2 |
±16.7 |
|
3.502E-05 |
+8.9 |
-6.9 |
±15.9 |
±15.0 |
±5.3 |
0 |
3050.00 |
8.470E-04 |
+3.4 |
-5.5 |
|
±17.3 |
|
|
|
|
|
|
|
|
3100.00 |
7.600E-04 |
+3.5 |
-5.6 |
|
±17.7 |
|
|
|
|
|
|
|
|
3150.00 |
6.820E-04 |
+3.6 |
-5.7 |
|
±18.1 |
|
|
|
|
|
|
|
|
3200.00 |
6.130E-04 |
+3.7 |
-5.9 |
|
±18.5 |
|
|
|
|
|
|
|
|
3250.00 |
5.510E-04 |
+3.9 |
-6.0 |
|
±19.0 |
|
|
|
|
|
|
|
|
3300.00 |
4.950E-04 |
+4.0 |
-6.2 |
|
±19.4 |
|
|
|
|
|
|
|
|
3350.00 |
4.450E-04 |
+4.1 |
-6.3 |
|
±19.9 |
|
|
|
|
|
|
|
|
3400.00 |
4.000E-04 |
+4.3 |
-6.4 |
|
±20.4 |
|
|
|
|
|
|
|
|
3450.00 |
3.600E-04 |
+4.4 |
-6.6 |
|
±20.9 |
|
|
|
|
|
|
|
|
3500.00 |
3.240E-04 |
+4.5 |
-6.8 |
|
±21.4 |
|
|
|
|
|
|
|
|
3550.00 |
2.920E-04 |
+4.7 |
-6.9 |
|
±21.9 |
|
|
|
|
|
|
|
|
3600.00 |
2.630E-04 |
+4.8 |
-7.1 |
|
±22.4 |
|
|
|
|
|
|
|
|
3650.00 |
2.370E-04 |
+5.0 |
-7.2 |
|
±22.9 |
|
|
|
|
|
|
|
|
3700.00 |
2.130E-04 |
+5.1 |
-7.4 |
|
±23.4 |
|
|
|
|
|
|
|
|
3750.00 |
1.920E-04 |
+5.3 |
-7.6 |
|
±24.0 |
|
|
|
|
|
|
|
|
3800.00 |
1.730E-04 |
+5.5 |
-7.8 |
|
±24.5 |
|
|
|
|
|
|
|
|
3850.00 |
1.560E-04 |
+5.6 |
-7.9 |
|
±25.1 |
|
|
|
|
|
|
|
|
3900.00 |
1.410E-04 |
+5.8 |
-8.1 |
|
±25.7 |
|
|
|
|
|
|
|
|
3950.00 |
1.270E-04 |
+6.0 |
-8.3 |
|
±26.3 |
|
|
|
|
|
|
|
|
4000.00 |
1.140E-04 |
+6.1 |
-8.5 |
|
±26.9 |
|
|
|
|
|
|
|
|
4050.00 |
1.030E-04 |
+6.3 |
-8.7 |
|
±27.5 |
|
|
|
|
|
|
|
|
4100.00 |
9.300E-05 |
+6.5 |
-8.9 |
|
±28.1 |
|
|
|
|
|
|
|
|
4150.00 |
8.400E-05 |
+6.7 |
-9.1 |
|
±28.7 |
|
|
|
|
|
|
|
|
4200.00 |
7.600E-05 |
+6.9 |
-9.3 |
|
±29.4 |
|
|
|
|
|
|
|
|
4250.00 |
6.800E-05 |
+7.1 |
-9.5 |
|
±30.0 |
|
|
|
|
|
|
|
|
4300.00 |
6.100E-05 |
+7.3 |
-9.7 |
|
±30.7 |
|
|
|
|
|
|
|
|
4350.00 |
5.500E-05 |
+7.5 |
-10.0 |
|
±31.4 |
|
|
|
|
|
|
|
|
4400.00 |
5.000E-05 |
+7.7 |
-10.2 |
|
±32.1 |
|
|
|
|
|
|
|
|
4450.00 |
4.500E-05 |
+7.9 |
-10.4 |
|
±32.8 |
|
|
|
|
|
|
|
|
4500.00 |
4.100E-05 |
+8.1 |
-10.7 |
|
±33.5 |
|
|
|
|
|
|
|
|
4550.00 |
3.700E-05 |
+8.3 |
-10.9 |
|
±34.2 |
|
|
|
|
|
|
|
|
4600.00 |
3.300E-05 |
+8.5 |
-11.2 |
|
±35.0 |
|
|
|
|
|
|
|
|
4650.00 |
3.000E-05 |
+8.8 |
-11.4 |
|
±35.7 |
|
|
|
|
|
|
|
|
4700.00 |
2.700E-05 |
+9.0 |
-11.7 |
|
±36.5 |
|
|
|
|
|
|
|
|
4750.00 |
2.400E-05 |
+9.2 |
-11.9 |
|
±37.3 |
|
|
|
|
|
|
|
|
4800.00 |
2.200E-05 |
+9.5 |
-12.2 |
|
±38.1 |
|
|
|
|
|
|
|
|
4850.00 |
2.000E-05 |
+9.7 |
-12.5 |
|
±38.9 |
|
|
|
|
|
|
|
|
4900.00 |
1.800E-05 |
+10.0 |
-12.7 |
|
±39.8 |
|
|
|
|
|
|
|
|
4950.00 |
1.600E-05 |
+10.2 |
-13.0 |
|
±40.6 |
|
|
|
|
|
|
|
|
5000.00 |
1.400E-05 |
+10.5 |
-13.3 |
|
±41.5 |
|
|
|
|
|
|
|
|
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 |
1.121E+01 |
+1.0 |
-0.7 |
±2.0 |
±1.8 |
±0.9 |
|
15.00 |
1.074E+01 |
+1.0 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
|
20.00 |
1.025E+01 |
+0.9 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
|
25.00 |
9.769E+00 |
+0.8 |
-0.6 |
±2.0 |
±1.8 |
±0.8 |
|
30.00 |
9.299E+00 |
+0.9 |
-0.5 |
±2.0 |
±1.8 |
±0.8 |
|
35.00 |
8.847E+00 |
+0.8 |
-0.5 |
±1.9 |
±1.8 |
±0.8 |
|
40.00 |
8.419E+00 |
+0.8 |
-0.5 |
±1.9 |
±1.8 |
±0.7 |
|
45.00 |
8.011E+00 |
+0.8 |
-0.4 |
±1.9 |
±1.8 |
±0.7 |
|
50.00 |
7.627E+00 |
+0.8 |
-0.4 |
±1.9 |
±1.8 |
±0.7 |
|
55.00 |
7.264E+00 |
+0.7 |
-0.4 |
±1.9 |
±1.8 |
±0.7 |
|
60.00 |
6.924E+00 |
+0.7 |
-0.4 |
±1.9 |
±1.8 |
±0.7 |
|
65.00 |
6.603E+00 |
+0.7 |
-0.4 |
±1.9 |
±1.8 |
±0.7 |
|
70.00 |
6.301E+00 |
+0.7 |
-0.4 |
±1.9 |
±1.8 |
±0.7 |
|
75.00 |
6.016E+00 |
+0.6 |
-0.3 |
±1.9 |
±1.8 |
±0.7 |
|
80.00 |
5.748E+00 |
+0.6 |
-0.3 |
±1.9 |
±1.8 |
±0.6 |
|
85.00 |
5.496E+00 |
+0.6 |
-0.3 |
±1.9 |
±1.8 |
±0.6 |
|
90.00 |
5.258E+00 |
+0.6 |
-0.3 |
±1.9 |
±1.8 |
±0.6 |
|
95.00 |
5.034E+00 |
+0.6 |
-0.3 |
±1.9 |
±1.8 |
±0.6 |
|
100.00 |
4.822E+00 |
+0.5 |
-0.3 |
±1.9 |
±1.8 |
±0.6 |
|
105.00 |
4.623E+00 |
+0.5 |
-0.3 |
±1.9 |
±1.8 |
±0.6 |
|
110.00 |
4.434E+00 |
+0.5 |
-0.2 |
±1.9 |
±1.8 |
±0.6 |
|
115.00 |
4.255E+00 |
+0.5 |
-0.2 |
±1.9 |
±1.8 |
±0.6 |
|
120.00 |
4.086E+00 |
+0.5 |
-0.2 |
±1.9 |
±1.8 |
±0.6 |
|
125.00 |
3.925E+00 |
+0.5 |
-0.2 |
±1.9 |
±1.8 |
±0.6 |
|
130.00 |
3.773E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.6 |
|
135.00 |
3.629E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.6 |
|
140.00 |
3.492E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
145.00 |
3.362E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
150.00 |
3.239E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
160.00 |
3.010E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
170.00 |
2.802E+00 |
+0.4 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
180.00 |
2.612E+00 |
+0.3 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
190.00 |
2.440E+00 |
+0.3 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
200.00 |
2.282E+00 |
+0.3 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
210.00 |
2.138E+00 |
+0.3 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
220.00 |
2.006E+00 |
+0.3 |
-0.2 |
±1.9 |
±1.8 |
±0.5 |
|
230.00 |
1.884E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.8 |
±0.4 |
|
240.00 |
1.772E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.8 |
±0.4 |
|
250.00 |
1.669E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.8 |
±0.4 |
|
260.00 |
1.573E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
270.00 |
1.485E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
280.00 |
1.403E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
290.00 |
1.326E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
300.00 |
1.256E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
310.00 |
1.190E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
320.00 |
1.128E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
330.00 |
1.071E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
340.00 |
1.017E+00 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.4 |
|
350.00 |
9.666E-01 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.3 |
|
360.00 |
9.194E-01 |
+0.3 |
-0.1 |
±1.9 |
±1.9 |
±0.3 |
|
370.00 |
8.752E-01 |
+0.3 |
-0.1 |
±2.0 |
±1.9 |
±0.3 |
|
380.00 |
8.337E-01 |
+0.3 |
-0.1 |
±2.0 |
±1.9 |
±0.3 |
|
390.00 |
7.947E-01 |
+0.3 |
-0.1 |
±2.0 |
±1.9 |
±0.3 |
|
400.00 |
7.580E-01 |
+0.3 |
-0.1 |
±2.0 |
±1.9 |
±0.3 |
|
410.00 |
7.235E-01 |
+0.3 |
-0.0 |
±2.0 |
±2.0 |
±0.3 |
|
420.00 |
6.909E-01 |
+0.3 |
-0.0 |
±2.0 |
±2.0 |
±0.3 |
|
430.00 |
6.602E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
440.00 |
6.312E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
450.00 |
6.038E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
460.00 |
5.778E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
470.00 |
5.533E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
480.00 |
5.301E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
490.00 |
5.081E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.3 |
|
500.00 |
4.872E-01 |
+0.3 |
-0.1 |
±2.0 |
±2.0 |
±0.2 |
|
550.00 |
3.975E-01 |
+0.3 |
-0.2 |
±2.1 |
±2.1 |
±0.2 |
|
600.00 |
3.274E-01 |
+0.3 |
-0.3 |
±2.1 |
±2.1 |
±0.2 |
|
650.00 |
2.719E-01 |
+0.3 |
-0.3 |
±2.1 |
±2.1 |
±0.2 |
|
700.00 |
2.275E-01 |
+0.3 |
-0.4 |
±2.2 |
±2.2 |
±0.1 |
|
750.00 |
1.915E-01 |
+0.3 |
-0.4 |
±2.2 |
±2.2 |
±0.1 |
|
800.00 |
1.622E-01 |
+0.3 |
-0.5 |
±2.3 |
±2.3 |
±0.1 |
|
850.00 |
1.380E-01 |
+0.3 |
-0.5 |
±2.3 |
±2.3 |
±0.1 |
|
900.00 |
1.180E-01 |
+0.3 |
-0.6 |
±2.4 |
±2.4 |
±0.1 |
|
950.00 |
1.013E-01 |
+0.3 |
-0.6 |
±2.4 |
±2.4 |
±0.0 |
|
1000.00 |
8.732E-02 |
+0.3 |
-0.7 |
±2.5 |
±2.5 |
±0.0 |
|
1050.00 |
7.551E-02 |
+0.3 |
-0.7 |
±2.5 |
±2.5 |
±0.0 |
|
1100.00 |
6.550E-02 |
+0.3 |
-0.8 |
±2.6 |
±2.6 |
±0.0 |
|
1150.00 |
5.698E-02 |
+0.3 |
-0.8 |
±2.6 |
±2.6 |
±0.0 |
|
1200.00 |
4.970E-02 |
+0.3 |
-0.9 |
±2.7 |
±2.7 |
±0.0 |
|
1250.00 |
4.345E-02 |
+0.3 |
-0.9 |
±2.7 |
±2.7 |
±0.1 |
|
1300.00 |
3.807E-02 |
+0.3 |
-0.9 |
±2.8 |
±2.8 |
±0.1 |
|
1350.00 |
3.343E-02 |
+0.4 |
-1.0 |
±2.8 |
±2.8 |
±0.1 |
|
1400.00 |
2.941E-02 |
+0.4 |
-1.0 |
±2.9 |
±2.9 |
±0.1 |
|
1450.00 |
2.592E-02 |
+0.4 |
-1.1 |
±2.9 |
±2.9 |
±0.1 |
|
1500.00 |
2.288E-02 |
+0.4 |
-1.1 |
±3.0 |
±3.0 |
±0.1 |
|
1550.00 |
2.023E-02 |
+0.5 |
-1.2 |
±3.0 |
±3.0 |
±0.1 |
|
1600.00 |
1.791E-02 |
+0.5 |
-1.2 |
±3.1 |
±3.1 |
±0.1 |
|
1650.00 |
1.588E-02 |
+0.5 |
-1.3 |
±3.2 |
±3.2 |
±0.1 |
|
1700.00 |
1.410E-02 |
+0.5 |
-1.3 |
±3.2 |
±3.2 |
±0.2 |
|
1750.00 |
1.253E-02 |
+0.6 |
-1.4 |
±3.3 |
±3.3 |
±0.2 |
|
1800.00 |
1.115E-02 |
+0.6 |
-1.4 |
±3.4 |
±3.3 |
±0.2 |
|
1850.00 |
9.926E-03 |
+0.6 |
-1.5 |
±3.4 |
±3.4 |
±0.2 |
|
1900.00 |
8.849E-03 |
+0.6 |
-1.5 |
±3.5 |
±3.5 |
±0.2 |
|
1950.00 |
7.896E-03 |
+0.7 |
-1.6 |
±3.6 |
±3.6 |
±0.2 |
|
2000.00 |
7.052E-03 |
+0.7 |
-1.6 |
±3.6 |
±3.6 |
±0.2 |
|
2050.00 |
6.303E-03 |
+0.7 |
-1.7 |
±3.7 |
±3.7 |
±0.2 |
|
2100.00 |
5.638E-03 |
+0.7 |
-1.7 |
±3.8 |
±3.8 |
±0.2 |
|
2150.00 |
5.046E-03 |
+0.7 |
-1.8 |
±3.9 |
±3.9 |
±0.2 |
|
2200.00 |
4.520E-03 |
+0.8 |
-1.8 |
±3.9 |
±3.9 |
±0.2 |
|
2250.00 |
4.051E-03 |
+0.8 |
-1.9 |
±4.0 |
±4.0 |
±0.2 |
|
2300.00 |
3.633E-03 |
+0.8 |
-1.9 |
±4.1 |
±4.1 |
±0.2 |
|
2350.00 |
3.259E-03 |
+0.9 |
-2.0 |
±4.2 |
±4.2 |
±0.2 |
|
2400.00 |
2.925E-03 |
+0.9 |
-2.0 |
±4.3 |
±4.3 |
±0.2 |
|
2450.00 |
2.627E-03 |
+0.9 |
-2.1 |
±4.4 |
±4.4 |
±0.2 |
|
2500.00 |
2.360E-03 |
+1.0 |
-2.1 |
±4.5 |
±4.5 |
±0.2 |
|
2550.00 |
2.122E-03 |
+1.0 |
-2.2 |
±4.6 |
±4.6 |
±0.2 |
|
2600.00 |
1.908E-03 |
+1.0 |
-2.2 |
±4.7 |
±4.7 |
±0.2 |
|
2650.00 |
1.717E-03 |
+1.0 |
-2.3 |
±4.8 |
±4.8 |
±0.2 |
|
2700.00 |
1.545E-03 |
+1.1 |
-2.3 |
±4.9 |
±4.9 |
±0.2 |
|
2750.00 |
1.391E-03 |
+1.1 |
-2.4 |
±5.0 |
±5.0 |
±0.2 |
|
2800.00 |
1.252E-03 |
+1.1 |
-2.4 |
±5.1 |
±5.1 |
±0.2 |
|
2850.00 |
1.128E-03 |
+1.1 |
-2.5 |
±5.3 |
±5.3 |
±0.2 |
|
2900.00 |
1.016E-03 |
+1.2 |
-2.5 |
±5.4 |
±5.4 |
±0.2 |
|
2950.00 |
9.156E-04 |
+1.2 |
-2.6 |
±5.5 |
±5.5 |
±0.2 |
|
3000.00 |
8.253E-04 |
+1.2 |
-2.7 |
±5.7 |
±5.7 |
±0.2 |
|
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 |
2.392E+02 |
+1.1 |
-2.0 |
±2.2 |
|
|
|
1.390E+02 |
1.002E+02 |
15.00 |
1.487E+02 |
+0.7 |
-2.0 |
±2.2 |
|
|
|
8.671E+01 |
6.201E+01 |
20.00 |
9.931E+01 |
+1.2 |
-1.5 |
±2.2 |
|
|
|
5.801E+01 |
4.130E+01 |
25.00 |
7.006E+01 |
+1.0 |
-1.7 |
±2.1 |
|
|
|
4.109E+01 |
2.897E+01 |
30.00 |
5.108E+01 |
+0.8 |
-1.6 |
±2.1 |
|
|
|
3.000E+01 |
2.108E+01 |
35.00 |
3.822E+01 |
+0.7 |
-1.4 |
±2.1 |
|
|
|
2.250E+01 |
1.572E+01 |
40.00 |
2.925E+01 |
+0.6 |
-1.3 |
±2.0 |
|
|
|
1.730E+01 |
1.195E+01 |
45.00 |
2.278E+01 |
+0.5 |
-1.3 |
±2.0 |
|
|
|
1.350E+01 |
9.282E+00 |
50.00 |
1.800E+01 |
+0.7 |
-1.2 |
±1.9 |
|
|
|
1.069E+01 |
7.311E+00 |
55.00 |
1.443E+01 |
+0.7 |
-1.2 |
±1.9 |
|
|
|
8.581E+00 |
5.848E+00 |
60.00 |
1.170E+01 |
+0.6 |
-1.2 |
±1.9 |
|
|
|
6.971E+00 |
4.727E+00 |
65.00 |
9.577E+00 |
+0.5 |
-1.0 |
±1.9 |
|
|
|
5.725E+00 |
3.852E+00 |
70.00 |
7.920E+00 |
+0.3 |
-1.0 |
±1.9 |
|
|
|
4.745E+00 |
3.175E+00 |
75.00 |
6.591E+00 |
+0.4 |
-0.9 |
±1.9 |
|
|
|
3.955E+00 |
2.636E+00 |
80.00 |
5.538E+00 |
+0.3 |
-0.9 |
±1.9 |
|
|
|
3.331E+00 |
2.207E+00 |
85.00 |
4.675E+00 |
+0.5 |
-0.8 |
±1.8 |
|
|
|
2.816E+00 |
1.859E+00 |
90.00 |
3.977E+00 |
+0.5 |
-0.7 |
±1.8 |
|
|
|
2.402E+00 |
1.575E+00 |
95.00 |
3.401E+00 |
+0.4 |
-0.7 |
±1.8 |
|
|
|
2.058E+00 |
1.343E+00 |
100.00 |
2.926E+00 |
+0.4 |
-0.8 |
±1.8 |
|
|
|
1.775E+00 |
1.151E+00 |
105.00 |
2.531E+00 |
+0.3 |
-0.8 |
±1.8 |
|
|
|
1.538E+00 |
9.934E-01 |
110.00 |
2.194E+00 |
+0.5 |
-0.5 |
±1.8 |
|
|
|
1.335E+00 |
8.587E-01 |
115.00 |
1.917E+00 |
+0.3 |
-0.7 |
±1.8 |
|
|
|
1.169E+00 |
7.478E-01 |
120.00 |
1.679E+00 |
+0.5 |
-0.6 |
±1.8 |
|
|
|
1.026E+00 |
6.525E-01 |
125.00 |
1.475E+00 |
+0.5 |
-0.7 |
±1.9 |
|
|
|
9.034E-01 |
5.720E-01 |
130.00 |
1.303E+00 |
+0.4 |
-0.7 |
±1.8 |
|
|
|
7.995E-01 |
5.033E-01 |
135.00 |
1.153E+00 |
+0.5 |
-0.8 |
±1.8 |
|
|
|
7.087E-01 |
4.447E-01 |
140.00 |
1.025E+00 |
+0.5 |
-0.8 |
±1.9 |
|
|
|
6.308E-01 |
3.940E-01 |
145.00 |
9.128E-01 |
+0.5 |
-0.8 |
±1.9 |
|
|
|
5.630E-01 |
3.498E-01 |
150.00 |
8.154E-01 |
+0.5 |
-0.8 |
±1.9 |
|
|
|
5.037E-01 |
3.117E-01 |
160.00 |
6.562E-01 |
+0.6 |
-0.8 |
±1.9 |
|
|
|
4.068E-01 |
2.494E-01 |
170.00 |
5.339E-01 |
+0.7 |
-0.9 |
±1.9 |
|
|
|
3.321E-01 |
2.018E-01 |
180.00 |
4.380E-01 |
+0.7 |
-0.8 |
±1.9 |
|
|
|
2.734E-01 |
1.646E-01 |
190.00 |
3.625E-01 |
+0.7 |
-0.9 |
±1.9 |
|
|
|
2.270E-01 |
1.355E-01 |
200.00 |
3.023E-01 |
+0.7 |
-0.8 |
±1.9 |
|
|
|
1.899E-01 |
1.124E-01 |
210.00 |
2.538E-01 |
+0.7 |
-0.9 |
±2.0 |
|
|
|
1.600E-01 |
9.383E-02 |
220.00 |
2.144E-01 |
+0.8 |
-0.9 |
±2.0 |
|
|
|
1.355E-01 |
7.893E-02 |
230.00 |
1.824E-01 |
+0.8 |
-1.0 |
±2.0 |
|
|
|
1.156E-01 |
6.678E-02 |
240.00 |
1.559E-01 |
+0.9 |
-1.0 |
±2.0 |
|
|
|
9.916E-02 |
5.675E-02 |
250.00 |
1.340E-01 |
+0.9 |
-0.9 |
±2.0 |
|
|
|
8.547E-02 |
4.853E-02 |
260.00 |
1.158E-01 |
+0.9 |
-1.0 |
±2.0 |
|
|
|
7.404E-02 |
4.172E-02 |
270.00 |
1.004E-01 |
+0.9 |
-1.0 |
±2.0 |
|
|
|
6.442E-02 |
3.602E-02 |
280.00 |
8.750E-02 |
+1.0 |
-1.0 |
±2.1 |
|
|
|
5.626E-02 |
3.124E-02 |
290.00 |
7.656E-02 |
+1.0 |
-1.0 |
±2.1 |
|
|
|
4.937E-02 |
2.719E-02 |
300.00 |
6.724E-02 |
+1.0 |
-1.0 |
±2.2 |
|
|
|
4.348E-02 |
2.376E-02 |
310.00 |
5.925E-02 |
+1.0 |
-1.1 |
±2.2 |
|
|
|
3.841E-02 |
2.084E-02 |
320.00 |
5.238E-02 |
+1.1 |
-1.0 |
±2.2 |
|
|
|
3.404E-02 |
1.834E-02 |
330.00 |
4.645E-02 |
+1.1 |
-1.0 |
±2.3 |
|
|
|
3.026E-02 |
1.619E-02 |
340.00 |
4.133E-02 |
+1.1 |
-1.0 |
±2.3 |
|
|
|
2.699E-02 |
1.434E-02 |
350.00 |
3.686E-02 |
+1.2 |
-1.0 |
±2.4 |
|
|
|
2.413E-02 |
1.273E-02 |
360.00 |
3.298E-02 |
+1.2 |
-1.0 |
±2.4 |
|
|
|
2.164E-02 |
1.134E-02 |
370.00 |
2.958E-02 |
+1.2 |
-1.1 |
±2.4 |
|
|
|
1.946E-02 |
1.012E-02 |
380.00 |
2.659E-02 |
+1.1 |
-1.1 |
±2.5 |
|
|
|
1.753E-02 |
9.061E-03 |
390.00 |
2.395E-02 |
+1.2 |
-1.1 |
±2.5 |
|
|
|
1.582E-02 |
8.128E-03 |
400.00 |
2.163E-02 |
+1.2 |
-1.1 |
±2.5 |
|
|
|
1.432E-02 |
7.309E-03 |
410.00 |
1.957E-02 |
+1.2 |
-1.2 |
±2.6 |
|
|
|
1.299E-02 |
6.581E-03 |
420.00 |
1.774E-02 |
+1.3 |
-1.3 |
±2.6 |
|
|
|
1.180E-02 |
5.944E-03 |
430.00 |
1.612E-02 |
+1.3 |
-1.2 |
±2.6 |
|
|
|
1.074E-02 |
5.378E-03 |
440.00 |
1.467E-02 |
+1.3 |
-1.3 |
±2.6 |
|
|
|
9.800E-03 |
4.872E-03 |
450.00 |
1.337E-02 |
+1.3 |
-1.2 |
±2.6 |
|
|
|
8.945E-03 |
4.424E-03 |
460.00 |
1.221E-02 |
+1.3 |
-1.3 |
±2.6 |
|
|
|
8.186E-03 |
4.023E-03 |
470.00 |
1.117E-02 |
+1.3 |
-1.3 |
±2.6 |
|
|
|
7.502E-03 |
3.664E-03 |
480.00 |
1.023E-02 |
+1.4 |
-1.4 |
±2.6 |
|
|
|
6.885E-03 |
3.342E-03 |
490.00 |
9.381E-03 |
+1.4 |
-1.4 |
±2.7 |
|
|
|
6.326E-03 |
3.055E-03 |
500.00 |
8.621E-03 |
+1.3 |
-1.4 |
±2.7 |
|
|
|
5.825E-03 |
2.796E-03 |
550.00 |
5.746E-03 |
+1.5 |
-1.5 |
±2.9 |
|
|
|
3.917E-03 |
1.829E-03 |
600.00 |
3.941E-03 |
+1.5 |
-1.6 |
±3.1 |
|
|
|
2.709E-03 |
1.232E-03 |
650.00 |
2.766E-03 |
+1.6 |
-1.7 |
±3.3 |
|
|
|
1.916E-03 |
8.501E-04 |
700.00 |
1.982E-03 |
+1.6 |
-1.8 |
±3.6 |
|
|
|
1.383E-03 |
5.990E-04 |
750.00 |
1.444E-03 |
+1.7 |
-1.8 |
±3.8 |
|
|
|
1.014E-03 |
4.300E-04 |
800.00 |
1.068E-03 |
+1.8 |
-1.9 |
±4.1 |
|
|
|
7.545E-04 |
3.133E-04 |
850.00 |
8.000E-04 |
+1.8 |
-2.0 |
±4.2 |
|
|
|
5.685E-04 |
2.315E-04 |
900.00 |
6.062E-04 |
+1.8 |
-2.1 |
±4.5 |
|
|
|
4.330E-04 |
1.732E-04 |
950.00 |
4.640E-04 |
+1.9 |
-2.1 |
±4.7 |
|
|
|
3.331E-04 |
1.309E-04 |
1000.00 |
3.585E-04 |
+1.9 |
-2.2 |
±5.0 |
|
|
|
2.585E-04 |
9.997E-05 |
1050.00 |
2.792E-04 |
+1.9 |
-2.2 |
±5.4 |
|
|
|
2.022E-04 |
7.699E-05 |
1100.00 |
2.190E-04 |
+2.0 |
-2.3 |
±5.7 |
|
|
|
1.592E-04 |
5.978E-05 |
1150.00 |
1.729E-04 |
+2.0 |
-2.4 |
±6.1 |
|
|
|
1.261E-04 |
4.675E-05 |
1200.00 |
1.373E-04 |
+2.0 |
-2.4 |
±6.5 |
|
|
|
1.005E-04 |
3.680E-05 |
1250.00 |
1.097E-04 |
+2.0 |
-2.5 |
±6.9 |
|
|
|
8.051E-05 |
2.915E-05 |
1300.00 |
8.801E-05 |
+2.1 |
-2.5 |
±7.3 |
|
|
|
6.480E-05 |
2.321E-05 |
1350.00 |
7.094E-05 |
+2.1 |
-2.6 |
±7.7 |
|
|
|
5.236E-05 |
1.858E-05 |
1400.00 |
5.742E-05 |
+2.2 |
-2.7 |
±8.1 |
|
|
|
4.247E-05 |
1.495E-05 |
1450.00 |
4.664E-05 |
+2.2 |
-2.7 |
±8.5 |
|
|
|
3.457E-05 |
1.207E-05 |
1500.00 |
3.804E-05 |
+2.2 |
-2.8 |
±8.9 |
|
|
|
2.824E-05 |
9.796E-06 |
1550.00 |
3.112E-05 |
+2.2 |
-2.8 |
±9.3 |
|
|
|
2.314E-05 |
7.979E-06 |
1600.00 |
2.553E-05 |
+2.2 |
-2.9 |
±9.7 |
|
|
|
1.901E-05 |
6.522E-06 |
1650.00 |
2.101E-05 |
+2.3 |
-3.0 |
±10.0 |
|
|
|
1.566E-05 |
5.347E-06 |
1700.00 |
1.733E-05 |
+2.3 |
-3.0 |
±10.4 |
|
|
|
1.293E-05 |
4.399E-06 |
1750.00 |
1.433E-05 |
+2.4 |
-3.1 |
±10.8 |
|
|
|
1.070E-05 |
3.629E-06 |
1800.00 |
1.187E-05 |
+2.4 |
-3.1 |
±11.2 |
|
|
|
8.871E-06 |
3.002E-06 |
1850.00 |
9.858E-06 |
+2.4 |
-3.2 |
±11.6 |
|
|
|
7.368E-06 |
2.490E-06 |
1900.00 |
8.199E-06 |
+2.5 |
-3.2 |
±12.0 |
|
|
|
6.128E-06 |
2.071E-06 |
1950.00 |
6.833E-06 |
+2.5 |
-3.3 |
±12.4 |
|
|
|
5.108E-06 |
1.725E-06 |
2000.00 |
5.706E-06 |
+2.5 |
-3.3 |
±12.9 |
|
|
|
4.265E-06 |
1.441E-06 |
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 |
1.064E+02 |
+1.3 |
-1.8 |
±2.2 |
|
|
|
|
15.00 |
6.773E+01 |
+0.9 |
-1.6 |
±2.1 |
|
|
|
|
20.00 |
4.639E+01 |
+0.8 |
-1.5 |
±2.1 |
|
|
|
|
25.00 |
3.336E+01 |
+0.8 |
-1.8 |
±2.1 |
|
|
|
|
30.00 |
2.467E+01 |
+0.5 |
-1.2 |
±2.1 |
|
|
|
|
35.00 |
1.879E+01 |
+0.5 |
-1.2 |
±2.1 |
|
|
|
|
40.00 |
1.460E+01 |
+0.6 |
-1.1 |
±2.1 |
|
|
|
|
45.00 |
1.156E+01 |
+0.4 |
-1.2 |
±2.0 |
|
|
|
|
50.00 |
9.264E+00 |
+0.6 |
-1.1 |
±1.9 |
|
|
|
|
55.00 |
7.527E+00 |
+0.8 |
-1.1 |
±1.9 |
|
|
|
|
60.00 |
6.183E+00 |
+0.8 |
-1.3 |
±1.8 |
|
|
|
|
65.00 |
5.119E+00 |
+0.9 |
-1.0 |
±1.8 |
|
|
|
|
70.00 |
4.279E+00 |
+1.4 |
-1.2 |
±1.8 |
|
|
|
|
75.00 |
3.611E+00 |
+1.5 |
-1.3 |
±1.7 |
|
|
|
|
80.00 |
3.073E+00 |
+1.5 |
-1.6 |
±1.7 |
|
|
|
|
85.00 |
2.628E+00 |
+1.7 |
-1.8 |
±1.7 |
|
|
|
|
90.00 |
2.261E+00 |
+2.1 |
-1.8 |
±1.7 |
|
|
|
|
95.00 |
1.959E+00 |
+2.1 |
-2.0 |
±1.7 |
|
|
|
|
100.00 |
1.704E+00 |
+2.5 |
-2.1 |
±1.7 |
|
|
|
|
105.00 |
1.490E+00 |
+2.6 |
-2.2 |
±1.7 |
|
|
|
|
110.00 |
1.309E+00 |
+2.8 |
-2.4 |
±1.7 |
|
|
|
|
115.00 |
1.155E+00 |
+3.1 |
-2.4 |
±1.7 |
|
|
|
|
120.00 |
1.024E+00 |
+3.2 |
-2.7 |
±1.6 |
|
|
|
|
125.00 |
9.095E-01 |
+3.5 |
-2.8 |
±1.6 |
|
|
|
|
130.00 |
8.118E-01 |
+3.6 |
-2.9 |
±1.6 |
|
|
|
|
135.00 |
7.262E-01 |
+3.7 |
-3.2 |
±1.6 |
|
|
|
|
140.00 |
6.514E-01 |
+3.9 |
-3.2 |
±1.6 |
|
|
|
|
145.00 |
5.856E-01 |
+4.1 |
-3.3 |
±1.6 |
|
|
|
|
150.00 |
5.279E-01 |
+4.2 |
-3.5 |
±1.6 |
|
|
|
|
160.00 |
4.318E-01 |
+4.6 |
-3.6 |
±1.6 |
|
|
|
|
170.00 |
3.560E-01 |
+4.8 |
-3.9 |
±1.6 |
|
|
|
|
180.00 |
2.951E-01 |
+4.9 |
-3.9 |
±1.5 |
|
|
|
|
190.00 |
2.455E-01 |
+5.2 |
-4.0 |
±1.5 |
|
|
|
|
200.00 |
2.054E-01 |
+5.1 |
-4.0 |
±1.5 |
|
|
|
|
210.00 |
1.722E-01 |
+5.2 |
-4.0 |
±1.5 |
|
|
|
|
220.00 |
1.449E-01 |
+4.9 |
-4.0 |
±1.5 |
|
|
|
|
230.00 |
1.223E-01 |
+4.8 |
-3.9 |
±1.6 |
|
|
|
|
240.00 |
1.034E-01 |
+4.6 |
-3.8 |
±1.6 |
|
|
|
|
250.00 |
8.773E-02 |
+4.4 |
-3.5 |
±1.6 |
|
|
|
|
260.00 |
7.478E-02 |
+4.2 |
-3.4 |
±1.6 |
|
|
|
|
270.00 |
6.406E-02 |
+3.8 |
-3.3 |
±1.6 |
|
|
|
|
280.00 |
5.507E-02 |
+3.7 |
-3.0 |
±1.7 |
|
|
|
|
290.00 |
4.761E-02 |
+3.4 |
-2.9 |
±1.7 |
|
|
|
|
300.00 |
4.132E-02 |
+3.2 |
-2.7 |
±1.7 |
|
|
|
|
310.00 |
3.601E-02 |
+3.0 |
-2.5 |
±1.7 |
|
|
|
|
320.00 |
3.154E-02 |
+2.8 |
-2.5 |
±1.7 |
|
|
|
|
330.00 |
2.771E-02 |
+2.7 |
-2.3 |
±1.7 |
|
|
|
|
340.00 |
2.447E-02 |
+2.6 |
-2.2 |
±1.8 |
|
|
|
|
350.00 |
2.173E-02 |
+2.6 |
-2.2 |
±1.8 |
|
|
|
|
360.00 |
1.940E-02 |
+2.5 |
-2.3 |
±1.8 |
|
|
|
|
370.00 |
1.738E-02 |
+2.5 |
-2.2 |
±1.8 |
|
|
|
|
380.00 |
1.562E-02 |
+2.6 |
-2.3 |
±1.8 |
|
|
|
|
390.00 |
1.409E-02 |
+2.6 |
-2.3 |
±1.9 |
|
|
|
|
400.00 |
1.273E-02 |
+2.8 |
-2.3 |
±1.9 |
|
|
|
|
410.00 |
1.154E-02 |
+2.9 |
-2.5 |
±1.9 |
|
|
|
|
420.00 |
1.049E-02 |
+3.0 |
-2.5 |
±1.9 |
|
|
|
|
430.00 |
9.558E-03 |
+3.0 |
-2.7 |
±1.9 |
|
|
|
|
440.00 |
8.722E-03 |
+3.2 |
-2.8 |
±2.0 |
|
|
|
|
450.00 |
7.980E-03 |
+3.3 |
-2.9 |
±2.0 |
|
|
|
|
460.00 |
7.317E-03 |
+3.4 |
-3.0 |
±2.0 |
|
|
|
|
470.00 |
6.719E-03 |
+3.5 |
-3.2 |
±2.0 |
|
|
|
|
480.00 |
6.179E-03 |
+3.7 |
-3.2 |
±2.0 |
|
|
|
|
490.00 |
5.695E-03 |
+3.9 |
-3.4 |
±2.1 |
|
|
|
|
500.00 |
5.256E-03 |
+4.1 |
-3.5 |
±2.1 |
|
|
|
|
550.00 |
3.601E-03 |
+4.8 |
-4.3 |
±2.2 |
|
|
|
|
600.00 |
2.544E-03 |
+5.7 |
-5.0 |
±2.2 |
|
|
|
|
650.00 |
1.844E-03 |
+6.6 |
-5.8 |
±2.3 |
|
|
|
|
700.00 |
1.364E-03 |
+7.5 |
-6.5 |
±2.4 |
|
|
|
|
750.00 |
1.027E-03 |
+8.4 |
-7.2 |
±2.5 |
|
|
|
|
800.00 |
7.842E-04 |
+9.1 |
-7.9 |
±2.6 |
|
|
|
|
850.00 |
6.061E-04 |
+10.0 |
-8.5 |
±2.7 |
|
|
|
|
900.00 |
4.743E-04 |
+10.6 |
-9.2 |
±2.7 |
|
|
|
|
950.00 |
3.740E-04 |
+11.4 |
-9.7 |
±2.8 |
|
|
|
|
1000.00 |
2.977E-04 |
+11.9 |
-10.4 |
±3.0 |
|
|
|
|
1050.00 |
2.385E-04 |
+12.7 |
-10.7 |
±3.2 |
|
|
|
|
1100.00 |
1.922E-04 |
+13.4 |
-11.2 |
±3.4 |
|
|
|
|
1150.00 |
1.559E-04 |
+13.8 |
-11.7 |
±3.6 |
|
|
|
|
1200.00 |
1.273E-04 |
+14.3 |
-12.3 |
±3.8 |
|
|
|
|
1250.00 |
1.043E-04 |
+14.8 |
-12.7 |
±4.0 |
|
|
|
|
1300.00 |
8.583E-05 |
+15.4 |
-13.1 |
±4.2 |
|
|
|
|
1350.00 |
7.083E-05 |
+16.0 |
-13.4 |
±4.4 |
|
|
|
|
1400.00 |
5.875E-05 |
+16.4 |
-13.9 |
±4.6 |
|
|
|
|
1450.00 |
4.885E-05 |
+16.8 |
-14.1 |
±4.8 |
|
|
|
|
1500.00 |
4.078E-05 |
+17.1 |
-14.5 |
±5.0 |
|
|
|
|
1550.00 |
3.404E-05 |
+17.8 |
-14.6 |
±5.2 |
|
|
|
|
1600.00 |
2.865E-05 |
+17.9 |
-15.2 |
±5.4 |
|
|
|
|
1650.00 |
2.408E-05 |
+18.4 |
-15.4 |
±5.6 |
|
|
|
|
1700.00 |
2.031E-05 |
+18.8 |
-15.7 |
±5.8 |
|
|
|
|
1750.00 |
1.718E-05 |
+19.1 |
-16.1 |
±6.1 |
|
|
|
|
1800.00 |
1.455E-05 |
+19.5 |
-16.3 |
±6.3 |
|
|
|
|
1850.00 |
1.234E-05 |
+20.0 |
-16.6 |
±6.5 |
|
|
|
|
1900.00 |
1.050E-05 |
+20.2 |
-16.9 |
±6.7 |
|
|
|
|
1950.00 |
8.934E-06 |
+20.6 |
-17.1 |
±6.9 |
|
|
|
|
2000.00 |
7.639E-06 |
+20.7 |
-17.5 |
±7.4 |
|
|
|
|
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 |
2.669E+01 |
+7.8 |
-9.9 |
±3.2 |
±2.6 |
±1.8 |
0.980 |
30.00 |
8.867E+00 |
+7.2 |
-9.7 |
±3.3 |
±2.7 |
±1.8 |
1.003 |
70.00 |
2.113E+00 |
+6.4 |
-9.4 |
±3.4 |
±2.8 |
±1.9 |
1.018 |
100.00 |
9.146E-01 |
+6.1 |
-9.3 |
±3.5 |
±2.9 |
±1.9 |
1.020 |
120.00 |
5.598E-01 |
+5.9 |
-9.3 |
±3.6 |
±3.0 |
±2.0 |
1.018 |
125.00 |
4.987E-01 |
+5.8 |
-9.2 |
±3.6 |
±3.0 |
±2.0 |
1.017 |
130.00 |
4.465E-01 |
+5.8 |
-9.3 |
±3.6 |
±3.0 |
±2.0 |
1.017 |
150.00 |
2.925E-01 |
+5.8 |
-9.3 |
±3.7 |
±3.1 |
±2.0 |
1.008 |
200.00 |
1.222E-01 |
+6.0 |
-9.6 |
±4.0 |
±3.5 |
±2.1 |
0.999 |
250.00 |
6.398E-02 |
+6.5 |
-10.0 |
±4.4 |
±3.9 |
±2.1 |
0.991 |
300.00 |
3.948E-02 |
+7.1 |
-10.6 |
±4.9 |
±4.4 |
±2.2 |
0.989 |
400.00 |
1.985E-02 |
+7.9 |
-11.4 |
±5.8 |
±5.3 |
±2.2 |
0.995 |
500.00 |
1.162E-02 |
+8.7 |
-12.0 |
±6.5 |
±6.0 |
±2.3 |
1.039 |
750.00 |
3.650E-03 |
+9.9 |
-13.0 |
±8.0 |
±7.6 |
±2.6 |
1.132 |
1000.00 |
1.263E-03 |
+10.6 |
-13.6 |
±9.5 |
±9.0 |
±2.9 |
1.211 |
1500.00 |
1.860E-04 |
+11.4 |
-14.4 |
±12.6 |
±12.0 |
±3.6 |
1.400 |
2000.00 |
3.308E-05 |
+12.4 |
-15.2 |
±16.1 |
±15.4 |
±4.6 |
1.642 |
2500.00 |
6.711E-06 |
+13.5 |
-16.0 |
±20.0 |
±19.1 |
±5.8 |
1.934 |
3000.00 |
1.466E-06 |
+14.6 |
-16.9 |
±24.2 |
±23.1 |
±7.2 |
2.314 |
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 |
1.138E+02 |
+91.9 |
-60.4 |
|
15.00 |
6.297E+01 |
+66.3 |
-52.8 |
|
20.00 |
4.011E+01 |
+53.4 |
-47.4 |
|
25.00 |
2.729E+01 |
+44.4 |
-43.4 |
|
30.00 |
1.931E+01 |
+39.8 |
-40.3 |
|
35.00 |
1.388E+01 |
+35.3 |
-37.6 |
|
40.00 |
1.029E+01 |
+34.1 |
-39.8 |
|
45.00 |
7.846E+00 |
+32.9 |
-40.9 |
|
50.00 |
6.102E+00 |
+31.2 |
-40.2 |
|
55.00 |
4.849E+00 |
+29.4 |
-39.0 |
|
60.00 |
3.914E+00 |
+28.5 |
-37.5 |
|
65.00 |
3.189E+00 |
+27.1 |
-36.1 |
|
70.00 |
2.633E+00 |
+26.2 |
-34.5 |
|
75.00 |
2.194E+00 |
+27.2 |
-33.1 |
|
80.00 |
1.838E+00 |
+24.8 |
-31.7 |
|
85.00 |
1.549E+00 |
+24.1 |
-30.5 |
|
90.00 |
1.317E+00 |
+23.4 |
-29.4 |
|
95.00 |
1.126E+00 |
+22.8 |
-28.4 |
|
100.00 |
9.669E-01 |
+22.2 |
-27.5 |
|
105.00 |
8.379E-01 |
+21.8 |
-26.6 |
|
110.00 |
7.262E-01 |
+21.2 |
-25.8 |
|
115.00 |
6.325E-01 |
+20.8 |
-25.1 |
|
120.00 |
5.534E-01 |
+20.3 |
-24.4 |
|
125.00 |
4.879E-01 |
+20.1 |
-23.9 |
|
130.00 |
4.304E-01 |
+19.9 |
-23.3 |
|
135.00 |
3.818E-01 |
+19.7 |
-22.8 |
|
140.00 |
3.383E-01 |
+19.4 |
-22.3 |
|
145.00 |
3.018E-01 |
+19.1 |
-21.8 |
|
150.00 |
2.693E-01 |
+18.9 |
-21.4 |
|
160.00 |
2.175E-01 |
+18.3 |
-20.4 |
|
170.00 |
1.769E-01 |
+18.0 |
-19.7 |
|
180.00 |
1.451E-01 |
+17.5 |
-19.1 |
|
190.00 |
1.200E-01 |
+17.1 |
-18.5 |
|
200.00 |
1.000E-01 |
+17.0 |
-18.0 |
|
210.00 |
8.397E-02 |
+16.7 |
-17.7 |
|
220.00 |
7.092E-02 |
+16.4 |
-17.5 |
|
230.00 |
6.021E-02 |
+16.1 |
-17.2 |
|
240.00 |
5.133E-02 |
+15.8 |
-17.0 |
|
250.00 |
4.410E-02 |
+15.6 |
-16.7 |
|
260.00 |
3.799E-02 |
+15.4 |
-16.5 |
|
270.00 |
3.287E-02 |
+15.3 |
-16.3 |
|
280.00 |
2.854E-02 |
+15.2 |
-16.2 |
|
290.00 |
2.491E-02 |
+15.2 |
-16.1 |
|
300.00 |
2.180E-02 |
+15.1 |
-15.9 |
|
310.00 |
1.915E-02 |
+15.0 |
-15.8 |
|
320.00 |
1.689E-02 |
+14.9 |
-15.7 |
|
330.00 |
1.491E-02 |
+14.7 |
-15.6 |
|
340.00 |
1.321E-02 |
+14.6 |
-15.6 |
|
350.00 |
1.174E-02 |
+14.6 |
-15.5 |
|
360.00 |
1.045E-02 |
+14.5 |
-15.4 |
|
370.00 |
9.324E-03 |
+14.5 |
-15.3 |
|
380.00 |
8.351E-03 |
+14.6 |
-15.2 |
|
390.00 |
7.492E-03 |
+14.6 |
-15.1 |
|
400.00 |
6.731E-03 |
+14.6 |
-15.0 |
|
410.00 |
6.046E-03 |
+14.5 |
-15.0 |
|
420.00 |
5.470E-03 |
+14.5 |
-15.0 |
|
430.00 |
4.941E-03 |
+14.4 |
-14.9 |
|
440.00 |
4.472E-03 |
+14.4 |
-14.9 |
|
450.00 |
4.057E-03 |
+14.5 |
-14.9 |
|
460.00 |
3.690E-03 |
+14.6 |
-14.8 |
|
470.00 |
3.352E-03 |
+14.6 |
-14.8 |
|
480.00 |
3.055E-03 |
+14.6 |
-14.8 |
|
490.00 |
2.784E-03 |
+14.4 |
-14.7 |
|
500.00 |
2.547E-03 |
+14.5 |
-14.8 |
|
550.00 |
1.651E-03 |
+14.7 |
-14.7 |
|
600.00 |
1.101E-03 |
+15.1 |
-14.9 |
|
650.00 |
7.518E-04 |
+15.5 |
-15.0 |
|
700.00 |
5.251E-04 |
+15.8 |
-15.1 |
|
750.00 |
3.723E-04 |
+16.2 |
-15.0 |
|
800.00 |
2.692E-04 |
+16.8 |
-15.3 |
|
850.00 |
1.967E-04 |
+17.3 |
-15.7 |
|
900.00 |
1.457E-04 |
+17.7 |
-16.0 |
|
950.00 |
1.091E-04 |
+18.2 |
-16.2 |
|
1000.00 |
8.258E-05 |
+18.4 |
-16.7 |
|
1050.00 |
6.299E-05 |
+18.6 |
-17.2 |
|
1100.00 |
4.856E-05 |
+18.8 |
-17.5 |
|
1150.00 |
3.773E-05 |
+18.9 |
-18.1 |
|
1200.00 |
2.950E-05 |
+19.1 |
-18.6 |
|
1250.00 |
2.322E-05 |
+19.3 |
-19.2 |
|
1300.00 |
1.863E-05 |
+19.7 |
-20.1 |
|
1350.00 |
1.465E-05 |
+20.1 |
-20.9 |
|
1400.00 |
1.172E-05 |
+20.5 |
-21.7 |
|
1450.00 |
9.329E-06 |
+20.8 |
-22.5 |
|
1500.00 |
7.618E-06 |
+21.5 |
-23.4 |
|
1550.00 |
6.179E-06 |
+22.2 |
-24.0 |
|
1600.00 |
5.038E-06 |
+23.1 |
-24.6 |
|
1650.00 |
4.120E-06 |
+24.0 |
-25.2 |
|
1700.00 |
3.380E-06 |
+24.8 |
-25.8 |
|
1750.00 |
2.787E-06 |
+25.7 |
-26.4 |
|
1800.00 |
2.303E-06 |
+26.6 |
-27.0 |
|
1850.00 |
1.910E-06 |
+27.3 |
-27.7 |
|
1900.00 |
1.586E-06 |
+28.0 |
-28.3 |
|
1950.00 |
1.332E-06 |
+28.7 |
-28.9 |
|
2000.00 |
1.105E-06 |
+29.4 |
-29.7 |
|
2050.00 |
9.255E-07 |
+30.1 |
-30.4 |
|
2100.00 |
7.769E-07 |
+30.7 |
-31.1 |
|
2150.00 |
6.532E-07 |
+31.4 |
-32.0 |
|
2200.00 |
5.511E-07 |
+32.1 |
-33.1 |
|
2250.00 |
4.742E-07 |
+32.9 |
-34.0 |
|
2300.00 |
3.941E-07 |
+34.1 |
-35.3 |
|
2350.00 |
3.343E-07 |
+35.1 |
-36.4 |
|
2400.00 |
2.837E-07 |
+36.2 |
-37.6 |
|
2450.00 |
2.415E-07 |
+37.1 |
-38.7 |
|
2500.00 |
2.059E-07 |
+38.3 |
-39.8 |
|
2550.00 |
1.748E-07 |
+39.4 |
-41.1 |
|
2600.00 |
1.466E-07 |
+41.0 |
-42.8 |
|
2650.00 |
1.265E-07 |
+41.6 |
-43.6 |
|
2700.00 |
1.090E-07 |
+42.9 |
-44.6 |
|
2750.00 |
9.444E-08 |
+44.0 |
-45.4 |
|
2800.00 |
8.022E-08 |
+46.1 |
-46.7 |
|
2850.00 |
6.968E-08 |
+46.8 |
-47.3 |
|
2900.00 |
5.972E-08 |
+48.3 |
-48.3 |
|
2950.00 |
5.178E-08 |
+49.6 |
-49.2 |
|
3000.00 |
4.467E-08 |
+51.1 |
-50.1 |
|
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) |
10.00 |
1.848E+00 |
+8.2 |
-12.5 |
±2.6 |
±2.4 |
±0.9 |
|
1.174E+00 |
6.740E-01 |
15.00 |
1.274E+00 |
+8.5 |
-13.0 |
±2.6 |
±2.4 |
±0.9 |
|
8.130E-01 |
4.620E-01 |
20.00 |
9.350E-01 |
+8.6 |
-13.2 |
±2.7 |
±2.5 |
±0.9 |
|
5.998E-01 |
3.368E-01 |
30.00 |
5.613E-01 |
+8.9 |
-13.1 |
±2.7 |
±2.6 |
±1.0 |
|
3.616E-01 |
1.993E-01 |
45.00 |
3.095E-01 |
+9.0 |
-12.4 |
±2.9 |
±2.7 |
±1.0 |
|
2.013E-01 |
1.081E-01 |
70.00 |
1.542E-01 |
+8.5 |
-10.6 |
±3.2 |
±3.0 |
±1.0 |
|
1.013E-01 |
5.290E-02 |
100.00 |
9.414E-02 |
+7.5 |
-13.0 |
±3.6 |
±3.4 |
±1.1 |
|
6.211E-02 |
3.216E-02 |
150.00 |
6.389E-02 |
+5.8 |
-16.4 |
±3.9 |
±3.7 |
±1.2 |
|
4.185E-02 |
2.190E-02 |
200.00 |
5.191E-02 |
+4.9 |
-18.3 |
±4.0 |
±3.8 |
±1.3 |
|
3.409E-02 |
1.787E-02 |
300.00 |
3.743E-02 |
+3.9 |
-20.4 |
±4.3 |
±4.1 |
±1.3 |
|
2.470E-02 |
1.275E-02 |
450.00 |
2.301E-02 |
+3.1 |
-22.6 |
±4.6 |
±4.4 |
±1.4 |
|
1.535E-02 |
7.640E-03 |
700.00 |
1.041E-02 |
+2.4 |
-25.5 |
±5.3 |
±5.1 |
±1.5 |
|
7.090E-03 |
3.310E-03 |
1000.00 |
4.270E-03 |
+2.1 |
-28.3 |
±6.3 |
±6.0 |
±1.6 |
|
2.970E-03 |
1.300E-03 |
1500.00 |
1.100E-03 |
+2.1 |
-32.4 |
±8.2 |
±7.9 |
±2.1 |
|
7.800E-04 |
3.100E-04 |
2000.00 |
3.110E-04 |
+2.4 |
-36.1 |
±10.7 |
±10.4 |
±2.7 |
|
2.270E-04 |
8.400E-05 |
3000.00 |
2.820E-05 |
+3.6 |
-42.0 |
±17.1 |
±16.5 |
±4.5 |
|
2.140E-05 |
6.800E-06 |
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) |
10.00 |
1.041E-01 |
+2.4 |
-1.9 |
±1.9 |
±1.8 |
±0.5 |
|
6.490E-02 |
3.930E-02 |
15.00 |
7.410E-02 |
+2.4 |
-1.9 |
±1.9 |
±1.8 |
±0.5 |
|
4.624E-02 |
2.779E-02 |
20.00 |
5.568E-02 |
+2.3 |
-1.9 |
±1.9 |
±1.9 |
±0.5 |
|
3.489E-02 |
2.080E-02 |
30.00 |
3.487E-02 |
+2.3 |
-1.8 |
±1.9 |
±1.9 |
±0.5 |
|
2.195E-02 |
1.290E-02 |
45.00 |
1.980E-02 |
+2.2 |
-1.8 |
±2.0 |
±1.9 |
±0.4 |
|
1.258E-02 |
7.240E-03 |
70.00 |
9.420E-03 |
+2.2 |
-1.6 |
±2.0 |
±2.0 |
±0.4 |
|
6.056E-03 |
3.386E-03 |
100.00 |
4.678E-03 |
+2.4 |
-1.7 |
±2.1 |
±2.1 |
±0.3 |
|
3.032E-03 |
1.642E-03 |
150.00 |
1.888E-03 |
+2.4 |
-1.8 |
±2.3 |
±2.3 |
±0.2 |
|
1.245E-03 |
6.420E-04 |
200.00 |
9.290E-04 |
+2.4 |
-2.0 |
±2.5 |
±2.5 |
±0.1 |
|
6.220E-04 |
3.070E-04 |
300.00 |
3.140E-04 |
+2.3 |
-2.1 |
±2.8 |
±2.8 |
±0.0 |
|
2.150E-04 |
9.900E-05 |
450.00 |
9.390E-05 |
+2.1 |
-2.1 |
±3.3 |
±3.3 |
±0.2 |
|
6.610E-05 |
2.790E-05 |
700.00 |
2.130E-05 |
+2.0 |
-2.4 |
±4.1 |
±4.1 |
±0.5 |
|
1.540E-05 |
5.800E-06 |
1000.00 |
5.170E-06 |
+2.1 |
-2.8 |
±5.0 |
±5.0 |
±0.7 |
|
3.840E-06 |
1.330E-06 |
1500.00 |
7.140E-07 |
+2.5 |
-3.3 |
±6.3 |
±6.2 |
±1.0 |
|
5.420E-07 |
1.710E-07 |
2000.00 |
1.240E-07 |
+2.9 |
-3.9 |
±7.4 |
±7.2 |
±1.4 |
|
9.500E-08 |
2.900E-08 |
3000.00 |
4.800E-09 |
+3.9 |
-5.2 |
±12.8 |
±12.8 |
±2.3 |
|
3.590E-09 |
1.210E-09 |
--
ReiTanaka - 2016-03-01
This topic: LHCPhysics
> LHCHXSWG > CERNYellowReportPageBSMAt13TeV
Topic revision: r22 - 2018-04-05 - MassimilianoGrazzini