CERNYellowReportPageBSMAt14TeV < LHCPhysics

LHCPhysics Web>LHCHXSWG>CERNYellowReportPageBSMAt14TeV (2016-12-08, MarcoPieri) (raw view)
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---+ !BSM Higgs production cross sections at &#8730;s = 14 !TeV (update in CERN Report4 2016)
   
%TOC%

------------

   * Cross sections reported in CERN Report 4. See [[https://twiki.cern.ch/twiki/bin/view/LHCPhysics/CERNYellowReportPageAt7TeV2014][here]]  and here [[https://twiki.cern.ch/twiki/bin/view/LHCPhysics/CERNYellowReportPageAtMH12509_2014][here]] for previous numbers in CERN Report 3.
   * %BLUE% Higgs cross sections and BRs in Spread sheet are available in [[https://twiki.cern.ch/twiki/pub/LHCPhysics/LHCHXSWG/Higgs_XSBR_YR4_update.xlsx][xlsx format]] %ENDCOLOR% %N%
   * %BLUE% You can find figures at our gallery [[LHCHXSWGCrossSectionsFigures][here]].%ENDCOLOR% 

---++ %ICON{led-red}% !BSM Higgs-boson production cross section calculation

   * Please check [[https://twiki.cern.ch/twiki/pub/LHCPhysics/LHCHXSWGCrossSectionsCalc/HXS4BSM_v0.5.pdf][Proposal on how to provide reference "Higgs" cross sections for !BSM applications]] 
   * %BLUE%Full mass scan should be provided for major Higgs production processes:%ENDCOLOR%
      1 Major process: ggF, VBF, WH (also separate W<sup>+</sup>H and W<sup>-</sup>H), ZH (also gg&#8594;ZH)
      1 Associated Higgs with heavy quark: ttH, bbH
      1 Associated Higgs with single top-quark:	tH (bq&#8594;tHq', bg&#8594;WtH, qq&#8594;btH) 
   * %BLUE%Higgs width should be set to zero (NWA).%ENDCOLOR%
   * %BLUE%Separate electroweak correction should be provided.%ENDCOLOR%
   * %BLUE%For relevant processes, and if possible, the contributions proportional to different Higgs couplings should be given separately, together with the corresponding uncertainties.%ENDCOLOR%
   * %BLUE%All other external parameters should be chosen as in the corresponding best SM predictions as well as the evaluation of the uncertainties.%ENDCOLOR%
   * %BLUE%SM width: At each mass point, the corresponding Higgs widths calculated in the SM with the same characteristics above should be provided.%ENDCOLOR%
   * %BLUE%Examples on how to use these predictions in specific cases are provided.%ENDCOLOR%

---+++ 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  | + M<sub>H</sub>=125.09 !GeV|
|   [500,3000] !GeV  |   50 !GeV |  50 points  | | 
   * Total 115 points for M<sub>H</sub>=[10,3000] !GeV.
   * %BLUE%Lower mass limit might depend on stability of the code at low Bjorken-x. To be assessed.%ENDCOLOR%

------------------------------------

---++ gluon-gluon Fusion Process

   * Cross sections are calculated with dFG program at NNLO+NNLL QCD (only) accuracy. Separate NLO EW correction factors 1+&delta;<sub>EW</sub> are also given for M<sub>H</sub>=[100,2500]GeV. 
      * %BLUE%This is an interim recommendation, will be updated when new !N3LO QCD numbers became available%ENDCOLOR%.
   * 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: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>H</sub>, uncertainty estimated in the range 1/2 < &mu;/M<sub>H</sub> < 2 with 1/2 < &mu;<sub>F</sub>/&mu;<sub>R</sub> < 2 constraint.
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  !PDF4LHC15_nnlo_30

<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  |  1+&delta;<sub>EW</sub>  |
|	10.00	|	7.441E+03	|	+49.3	|	-39.1	|	±8.0	|	±7.5	|	±2.8	|	0.0000	|
|	15.00	|	4.576E+03	|	+37.1	|	-30.7	|	±6.0	|	±5.3	|	±2.8	|	0.0000	|
|	20.00	|	2.245E+03	|	+28.7	|	-24.5	|	±4.9	|	±3.9	|	±2.9	|	0.0000	|
|	25.00	|	1.242E+03	|	+23.2	|	-20.0	|	±4.4	|	±3.2	|	±2.9	|	0.0000	|
|	30.00	|	7.726E+02	|	+19.9	|	-16.9	|	±4.2	|	±2.9	|	±3.0	|	0.0000	|
|	35.00	|	5.292E+02	|	+17.5	|	-14.7	|	±4.0	|	±2.6	|	±3.0	|	0.0000	|
|	40.00	|	3.894E+02	|	+15.8	|	-13.3	|	±3.9	|	±2.5	|	±3.0	|	0.0000	|
|	45.00	|	3.022E+02	|	+14.4	|	-12.5	|	±3.8	|	±2.4	|	±3.0	|	0.0000	|
|	50.00	|	2.438E+02	|	+13.2	|	-11.9	|	±3.7	|	±2.3	|	±3.0	|	0.0000	|
|	55.00	|	2.025E+02	|	+12.3	|	-11.4	|	±3.7	|	±2.2	|	±2.9	|	0.0000	|
|	60.00	|	1.720E+02	|	+11.6	|	-10.9	|	±3.6	|	±2.1	|	±2.9	|	0.0000	|
|	65.00	|	1.486E+02	|	+10.9	|	-10.5	|	±3.5	|	±2.1	|	±2.9	|	0.0000	|
|	70.00	|	1.301E+02	|	+10.4	|	-10.2	|	±3.5	|	±2.0	|	±2.8	|	0.0000	|
|	75.00	|	1.151E+02	|	+10.0	|	-9.9	|	±3.4	|	±2.0	|	±2.8	|	0.0000	|
|	80.00	|	1.028E+02	|	+9.6	|	-9.6	|	±3.4	|	±2.0	|	±2.8	|	0.0000	|
|	85.00	|	9.252E+01	|	+9.3	|	-9.4	|	±3.3	|	±1.9	|	±2.7	|	0.0000	|
|	90.00	|	8.378E+01	|	+9.0	|	-9.2	|	±3.3	|	±1.9	|	±2.7	|	0.0000	|
|	95.00	|	7.627E+01	|	+8.7	|	-9.0	|	±3.3	|	±1.9	|	±2.7	|	0.0000	|
|	100.00	|	6.977E+01	|	+8.5	|	-8.8	|	±3.2	|	±1.9	|	±2.6	|	1.0418	|
|	105.00	|	6.410E+01	|	+8.3	|	-8.6	|	±3.2	|	±1.9	|	±2.6	|	1.0436	|
|	110.00	|	5.910E+01	|	+8.1	|	-8.5	|	±3.2	|	±1.9	|	±2.6	|	1.0455	|
|	115.00	|	5.468E+01	|	+7.9	|	-8.4	|	±3.1	|	±1.8	|	±2.6	|	1.0474	|
|	120.00	|	5.076E+01	|	+7.8	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|	1.0494	|
|	125.00	|	4.725E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|	1.0514	|
|	130.00	|	4.411E+01	|	+7.5	|	-8.0	|	±3.1	|	±1.8	|	±2.5	|	1.0534	|
|	135.00	|	4.127E+01	|	+7.4	|	-7.9	|	±3.1	|	±1.8	|	±2.5	|	1.0553	|
|	140.00	|	3.871E+01	|	+7.3	|	-7.8	|	±3.0	|	±1.8	|	±2.5	|	1.0571	|
|	145.00	|	3.639E+01	|	+7.2	|	-7.7	|	±3.0	|	±1.8	|	±2.5	|	1.0587	|
|	150.00	|	3.428E+01	|	+7.1	|	-7.6	|	±3.0	|	±1.8	|	±2.4	|	1.0598	|
|	160.00	|	3.059E+01	|	+6.9	|	-7.5	|	±3.0	|	±1.8	|	±2.4	|	1.0486	|
|	170.00	|	2.748E+01	|	+6.7	|	-7.3	|	±3.0	|	±1.8	|	±2.4	|	1.0206	|
|	180.00	|	2.485E+01	|	+6.5	|	-7.2	|	±2.9	|	±1.7	|	±2.4	|	1.0053	|
|	190.00	|	2.261E+01	|	+6.4	|	-7.1	|	±2.9	|	±1.7	|	±2.3	|	0.9872	|
|	200.00	|	2.070E+01	|	+6.3	|	-7.0	|	±2.9	|	±1.7	|	±2.3	|	0.9793	|
|	210.00	|	1.905E+01	|	+6.2	|	-6.9	|	±2.9	|	±1.7	|	±2.3	|	0.9761	|
|	220.00	|	1.762E+01	|	+6.1	|	-6.8	|	±2.9	|	±1.7	|	±2.3	|	0.9749	|
|	230.00	|	1.637E+01	|	+6.0	|	-6.7	|	±2.9	|	±1.7	|	±2.3	|	0.9749	|
|	240.00	|	1.530E+01	|	+5.9	|	-6.6	|	±2.8	|	±1.7	|	±2.3	|	0.9755	|
|	250.00	|	1.437E+01	|	+5.8	|	-6.5	|	±2.8	|	±1.7	|	±2.2	|	0.9762	|
|	260.00	|	1.356E+01	|	+5.8	|	-6.5	|	±2.8	|	±1.7	|	±2.2	|	0.9772	|
|	270.00	|	1.287E+01	|	+5.7	|	-6.4	|	±2.8	|	±1.7	|	±2.2	|	0.9783	|
|	280.00	|	1.228E+01	|	+5.7	|	-6.3	|	±2.8	|	±1.7	|	±2.2	|	0.9795	|
|	290.00	|	1.179E+01	|	+5.7	|	-6.3	|	±2.8	|	±1.7	|	±2.2	|	0.9805	|
|	300.00	|	1.139E+01	|	+5.7	|	-6.2	|	±2.8	|	±1.7	|	±2.2	|	0.9813	|
|	310.00	|	1.110E+01	|	+5.7	|	-6.1	|	±2.8	|	±1.8	|	±2.2	|	0.9819	|
|	320.00	|	1.092E+01	|	+5.7	|	-6.0	|	±2.8	|	±1.8	|	±2.2	|	0.9820	|
|	330.00	|	1.089E+01	|	+5.7	|	-6.0	|	±2.8	|	±1.8	|	±2.2	|	0.9813	|
|	340.00	|	1.111E+01	|	+5.7	|	-5.9	|	±2.8	|	±1.8	|	±2.2	|	0.9779	|
|	350.00	|	1.197E+01	|	+5.7	|	-5.8	|	±2.8	|	±1.8	|	±2.2	|	0.9595	|
|	360.00	|	1.243E+01	|	+5.7	|	-5.8	|	±2.8	|	±1.8	|	±2.2	|	0.9608	|
|	370.00	|	1.245E+01	|	+5.7	|	-5.7	|	±2.9	|	±1.8	|	±2.2	|	0.9642	|
|	380.00	|	1.219E+01	|	+5.7	|	-5.6	|	±2.9	|	±1.8	|	±2.2	|	0.9677	|
|	390.00	|	1.174E+01	|	+5.7	|	-5.6	|	±2.9	|	±1.9	|	±2.2	|	0.9713	|
|	400.00	|	1.118E+01	|	+5.7	|	-5.5	|	±2.9	|	±1.9	|	±2.2	|	0.9741	|
|	410.00	|	1.056E+01	|	+5.7	|	-5.5	|	±2.9	|	±1.9	|	±2.2	|	0.9771	|
|	420.00	|	9.917E+00	|	+5.7	|	-5.4	|	±2.9	|	±1.9	|	±2.2	|	0.9802	|
|	430.00	|	9.265E+00	|	+5.7	|	-5.4	|	±2.9	|	±1.9	|	±2.2	|	0.9830	|
|	440.00	|	8.624E+00	|	+5.7	|	-5.3	|	±2.9	|	±2.0	|	±2.2	|	0.9853	|
|	450.00	|	8.007E+00	|	+5.6	|	-5.3	|	±3.0	|	±2.0	|	±2.2	|	0.9878	|
|	460.00	|	7.417E+00	|	+5.6	|	-5.2	|	±3.0	|	±2.0	|	±2.2	|	0.9900	|
|	470.00	|	6.861E+00	|	+5.6	|	-5.2	|	±3.0	|	±2.0	|	±2.2	|	0.9921	|
|	480.00	|	6.340E+00	|	+5.6	|	-5.2	|	±3.0	|	±2.0	|	±2.2	|	0.9940	|
|	490.00	|	5.854E+00	|	+5.6	|	-5.1	|	±3.0	|	±2.1	|	±2.2	|	0.9961	|
|	500.00	|	5.401E+00	|	+5.6	|	-5.1	|	±3.0	|	±2.1	|	±2.2	|	0.9981	|
|	550.00	|	3.601E+00	|	+5.5	|	-5.0	|	±3.1	|	±2.2	|	±2.2	|	1.0069	|
|	600.00	|	2.413E+00	|	+5.4	|	-4.9	|	±3.2	|	±2.3	|	±2.3	|	1.0152	|
|	650.00	|	1.636E+00	|	+5.4	|	-4.8	|	±3.4	|	±2.5	|	±2.3	|	1.0226	|
|	700.00	|	1.124E+00	|	+5.4	|	-4.8	|	±3.5	|	±2.6	|	±2.3	|	1.0301	|
|	750.00	|	7.826E-01	|	+5.4	|	-4.7	|	±3.6	|	±2.8	|	±2.3	|	1.0377	|
|	800.00	|	5.527E-01	|	+5.4	|	-4.7	|	±3.8	|	±3.0	|	±2.4	|	1.0454	|
|	850.00	|	3.951E-01	|	+5.4	|	-4.7	|	±4.0	|	±3.2	|	±2.4	|	1.0532	|
|	900.00	|	2.858E-01	|	+5.4	|	-4.7	|	±4.1	|	±3.3	|	±2.4	|	1.0610	|
|	950.00	|	2.093E-01	|	+5.4	|	-4.7	|	±4.3	|	±3.5	|	±2.5	|	1.0695	|
|	1000.00	|	1.547E-01	|	+5.5	|	-4.7	|	±4.5	|	±3.7	|	±2.5	|	1.0783	|
|	1050.00	|	1.156E-01	|	+5.5	|	-4.7	|	±4.7	|	±3.9	|	±2.6	|	1.0890	|
|	1100.00	|	8.707E-02	|	+5.6	|	-4.8	|	±4.9	|	±4.1	|	±2.6	|	1.1004	|
|	1150.00	|	6.617E-02	|	+5.6	|	-4.8	|	±5.1	|	±4.3	|	±2.7	|	1.1122	|
|	1200.00	|	5.068E-02	|	+5.6	|	-4.8	|	±5.3	|	±4.5	|	±2.7	|	1.1242	|
|	1250.00	|	3.909E-02	|	+5.7	|	-4.8	|	±5.5	|	±4.7	|	±2.7	|	1.1364	|
|	1300.00	|	3.037E-02	|	+5.7	|	-4.8	|	±5.7	|	±4.9	|	±2.8	|	1.1475	|
|	1350.00	|	2.374E-02	|	+5.7	|	-4.9	|	±5.9	|	±5.1	|	±2.8	|	1.1586	|
|	1400.00	|	1.867E-02	|	+5.7	|	-4.9	|	±6.1	|	±5.3	|	±2.9	|	1.1700	|
|	1450.00	|	1.477E-02	|	+5.8	|	-4.9	|	±6.3	|	±5.6	|	±2.9	|	1.1816	|
|	1500.00	|	1.174E-02	|	+5.9	|	-5.0	|	±6.5	|	±5.8	|	±3.0	|	1.1937	|
|	1550.00	|	9.382E-03	|	+6.1	|	-5.0	|	±6.7	|	±6.0	|	±3.1	|	1.2069	|
|	1600.00	|	7.529E-03	|	+6.3	|	-5.0	|	±6.9	|	±6.2	|	±3.1	|	1.2206	|
|	1650.00	|	6.074E-03	|	+6.5	|	-5.1	|	±7.1	|	±6.4	|	±3.2	|	1.2347	|
|	1700.00	|	4.920E-03	|	+6.8	|	-5.1	|	±7.4	|	±6.6	|	±3.2	|	1.2493	|
|	1750.00	|	3.998E-03	|	+9.4	|	-1.7	|	±9.1	|	±7.5	|	±5.0	|	1.2644	|
|	1800.00	|	3.261E-03	|	+9.1	|	-2.3	|	±9.0	|	±7.6	|	±4.7	|	1.2798	|
|	1850.00	|	2.672E-03	|	+8.8	|	-2.9	|	±9.0	|	±7.7	|	±4.5	|	1.2955	|
|	1900.00	|	2.196E-03	|	+8.6	|	-3.4	|	±9.0	|	±7.9	|	±4.3	|	1.3117	|
|	1950.00	|	1.810E-03	|	+8.4	|	-3.8	|	±9.0	|	±8.0	|	±4.2	|	1.3283	|
|	2000.00	|	1.497E-03	|	+8.3	|	-4.2	|	±9.1	|	±8.2	|	±4.0	|	1.3453	|
|	2050.00	|	1.241E-03	|	+8.2	|	-4.6	|	±9.2	|	±8.3	|	±4.0	|	1.3627	|
|	2100.00	|	1.032E-03	|	+8.1	|	-4.9	|	±9.4	|	±8.5	|	±3.9	|	1.3806	|
|	2150.00	|	8.606E-04	|	+8.1	|	-5.1	|	±9.6	|	±8.7	|	±3.9	|	1.3989	|
|	2200.00	|	7.200E-04	|	+8.1	|	-5.3	|	±9.8	|	±8.9	|	±3.9	|	1.4176	|
|	2250.00	|	6.032E-04	|	+8.1	|	-5.5	|	±10.0	|	±9.2	|	±3.9	|	1.4367	|
|	2300.00	|	5.064E-04	|	+8.1	|	-5.7	|	±10.2	|	±9.4	|	±4.0	|	1.4563	|
|	2350.00	|	4.264E-04	|	+8.2	|	-5.8	|	±10.5	|	±9.7	|	±4.1	|	1.4763	|
|	2400.00	|	3.601E-04	|	+8.3	|	-5.9	|	±10.7	|	±9.9	|	±4.1	|	1.4968	|
|	2450.00	|	3.045E-04	|	+8.3	|	-6.0	|	±11.0	|	±10.2	|	±4.2	|	1.5177	|
|	2500.00	|	2.577E-04	|	+8.4	|	-6.1	|	±11.3	|	±10.5	|	±4.3	|	1.5390	|
|	2550.00	|	2.184E-04	|	+8.5	|	-6.2	|	±11.6	|	±10.8	|	±4.4	|	0.0000	|
|	2600.00	|	1.860E-04	|	+8.6	|	-6.2	|	±12.0	|	±11.1	|	±4.5	|	0.0000	|
|	2650.00	|	1.583E-04	|	+8.7	|	-6.3	|	±12.3	|	±11.4	|	±4.6	|	0.0000	|
|	2700.00	|	1.350E-04	|	+8.7	|	-6.3	|	±12.6	|	±11.7	|	±4.7	|	0.0000	|
|	2750.00	|	1.151E-04	|	+8.8	|	-6.4	|	±12.9	|	±12.0	|	±4.8	|	0.0000	|
|	2800.00	|	9.881E-05	|	+8.9	|	-6.5	|	±13.3	|	±12.3	|	±4.9	|	0.0000	|
|	2850.00	|	8.442E-05	|	+8.9	|	-6.6	|	±13.6	|	±12.7	|	±4.9	|	0.0000	|
|	2900.00	|	7.282E-05	|	+8.9	|	-6.7	|	±13.9	|	±13.0	|	±5.0	|	0.0000	|
|	2950.00	|	6.233E-05	|	+8.9	|	-6.8	|	±14.3	|	±13.4	|	±5.0	|	0.0000	|
|	3000.00	|	5.374E-05	|	+8.9	|	-6.9	|	±14.6	|	±13.7	|	±5.0	|	0.0000	|
</tr>
</table>

---++ !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: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>W</sub>, uncertainty estimated in the range 1/2 < &mu;/M<sub>W</sub> < 2 (scales have been varied independently by factor 2).
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  !PDF4LHC15_nnlo_30_pdfas

<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  |  1+&delta;<sub>EW</sub>  |
|	10.00	|	1.246E+01	|	+1.0	|	-0.7	|	±2.0	|	±1.8	|	±0.9	|		|
|	15.00	|	1.194E+01	|	+1.0	|	-0.6	|	±2.0	|	±1.8	|	±0.9	|		|
|	20.00	|	1.140E+01	|	+0.9	|	-0.6	|	±2.0	|	±1.8	|	±0.8	|		|
|	25.00	|	1.088E+01	|	+0.9	|	-0.6	|	±2.0	|	±1.8	|	±0.8	|		|
|	30.00	|	1.037E+01	|	+0.9	|	-0.5	|	±2.0	|	±1.8	|	±0.8	|		|
|	35.00	|	9.872E+00	|	+0.8	|	-0.5	|	±2.0	|	±1.8	|	±0.8	|		|
|	40.00	|	9.401E+00	|	+0.8	|	-0.5	|	±1.9	|	±1.8	|	±0.8	|		|
|	45.00	|	8.955E+00	|	+0.8	|	-0.5	|	±1.9	|	±1.8	|	±0.8	|		|
|	50.00	|	8.533E+00	|	+0.8	|	-0.5	|	±1.9	|	±1.8	|	±0.7	|		|
|	55.00	|	8.136E+00	|	+0.7	|	-0.4	|	±1.9	|	±1.8	|	±0.7	|		|
|	60.00	|	7.761E+00	|	+0.7	|	-0.4	|	±1.9	|	±1.8	|	±0.7	|		|
|	65.00	|	7.408E+00	|	+0.7	|	-0.4	|	±1.9	|	±1.8	|	±0.7	|		|
|	70.00	|	7.075E+00	|	+0.7	|	-0.4	|	±1.9	|	±1.8	|	±0.7	|		|
|	75.00	|	6.761E+00	|	+0.7	|	-0.4	|	±1.9	|	±1.8	|	±0.7	|		|
|	80.00	|	6.465E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.7	|		|
|	85.00	|	6.186E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.7	|		|
|	90.00	|	5.922E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|		|
|	95.00	|	5.674E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|		|
|	100.00	|	5.440E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|		|
|	105.00	|	5.219E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|		|
|	110.00	|	5.009E+00	|	+0.5	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|		|
|	115.00	|	4.811E+00	|	+0.5	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|		|
|	120.00	|	4.623E+00	|	+0.5	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	125.00	|	4.445E+00	|	+0.5	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	130.00	|	4.276E+00	|	+0.5	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	135.00	|	4.115E+00	|	+0.5	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	140.00	|	3.963E+00	|	+0.5	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	145.00	|	3.818E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	150.00	|	3.681E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.6	|		|
|	160.00	|	3.425E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	170.00	|	3.193E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	180.00	|	2.981E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	190.00	|	2.788E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	200.00	|	2.611E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	210.00	|	2.449E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	220.00	|	2.301E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	230.00	|	2.164E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	240.00	|	2.038E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|		|
|	250.00	|	1.921E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.8	|	±0.4	|		|
|	260.00	|	1.813E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.8	|	±0.4	|		|
|	270.00	|	1.714E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.8	|	±0.4	|		|
|	280.00	|	1.621E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	290.00	|	1.535E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	300.00	|	1.454E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	310.00	|	1.380E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	320.00	|	1.310E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	330.00	|	1.245E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	340.00	|	1.184E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	350.00	|	1.126E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	360.00	|	1.073E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	370.00	|	1.022E+00	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|		|
|	380.00	|	9.749E-01	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.3	|		|
|	390.00	|	9.303E-01	|	+0.3	|	-0.1	|	±1.9	|	±1.9	|	±0.3	|		|
|	400.00	|	8.884E-01	|	+0.3	|	-0.1	|	±2.0	|	±1.9	|	±0.3	|		|
|	410.00	|	8.488E-01	|	+0.3	|	-0.1	|	±2.0	|	±1.9	|	±0.3	|		|
|	420.00	|	8.115E-01	|	+0.3	|	-0.1	|	±2.0	|	±1.9	|	±0.3	|		|
|	430.00	|	7.763E-01	|	+0.3	|	-0.0	|	±2.0	|	±1.9	|	±0.3	|		|
|	440.00	|	7.430E-01	|	+0.3	|	-0.0	|	±2.0	|	±1.9	|	±0.3	|		|
|	450.00	|	7.115E-01	|	+0.3	|	-0.0	|	±2.0	|	±2.0	|	±0.3	|		|
|	460.00	|	6.817E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|		|
|	470.00	|	6.535E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|		|
|	480.00	|	6.268E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|		|
|	490.00	|	6.014E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|		|
|	500.00	|	5.773E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|		|
|	550.00	|	4.736E-01	|	+0.3	|	-0.2	|	±2.0	|	±2.0	|	±0.2	|		|
|	600.00	|	3.921E-01	|	+0.3	|	-0.2	|	±2.1	|	±2.1	|	±0.2	|		|
|	650.00	|	3.274E-01	|	+0.3	|	-0.3	|	±2.1	|	±2.1	|	±0.2	|		|
|	700.00	|	2.753E-01	|	+0.3	|	-0.3	|	±2.1	|	±2.1	|	±0.2	|		|
|	750.00	|	2.330E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.1	|		|
|	800.00	|	1.984E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.1	|		|
|	850.00	|	1.697E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|		|
|	900.00	|	1.459E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|		|
|	950.00	|	1.259E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|		|
|	1000.00	|	1.091E-01	|	+0.3	|	-0.6	|	±2.4	|	±2.4	|	±0.0	|		|
|	1050.00	|	9.479E-02	|	+0.3	|	-0.6	|	±2.4	|	±2.4	|	±0.0	|		|
|	1100.00	|	8.265E-02	|	+0.3	|	-0.7	|	±2.5	|	±2.5	|	±0.0	|		|
|	1150.00	|	7.227E-02	|	+0.3	|	-0.7	|	±2.5	|	±2.5	|	±0.0	|		|
|	1200.00	|	6.336E-02	|	+0.3	|	-0.8	|	±2.6	|	±2.6	|	±0.0	|		|
|	1250.00	|	5.569E-02	|	+0.3	|	-0.8	|	±2.6	|	±2.6	|	±0.0	|		|
|	1300.00	|	4.906E-02	|	+0.3	|	-0.8	|	±2.7	|	±2.7	|	±0.0	|		|
|	1350.00	|	4.330E-02	|	+0.3	|	-0.9	|	±2.7	|	±2.7	|	±0.1	|		|
|	1400.00	|	3.830E-02	|	+0.4	|	-0.9	|	±2.8	|	±2.8	|	±0.1	|		|
|	1450.00	|	3.393E-02	|	+0.4	|	-1.0	|	±2.8	|	±2.8	|	±0.1	|		|
|	1500.00	|	3.011E-02	|	+0.4	|	-1.0	|	±2.9	|	±2.9	|	±0.1	|		|
|	1550.00	|	2.677E-02	|	+0.4	|	-1.1	|	±2.9	|	±2.9	|	±0.1	|		|
|	1600.00	|	2.383E-02	|	+0.4	|	-1.1	|	±3.0	|	±3.0	|	±0.1	|		|
|	1650.00	|	2.124E-02	|	+0.5	|	-1.2	|	±3.0	|	±3.0	|	±0.1	|		|
|	1700.00	|	1.896E-02	|	+0.5	|	-1.2	|	±3.1	|	±3.1	|	±0.1	|		|
|	1750.00	|	1.694E-02	|	+0.5	|	-1.2	|	±3.1	|	±3.1	|	±0.1	|		|
|	1800.00	|	1.515E-02	|	+0.5	|	-1.3	|	±3.2	|	±3.2	|	±0.2	|		|
|	1850.00	|	1.357E-02	|	+0.5	|	-1.3	|	±3.2	|	±3.2	|	±0.2	|		|
|	1900.00	|	1.217E-02	|	+0.6	|	-1.4	|	±3.3	|	±3.3	|	±0.2	|		|
|	1950.00	|	1.092E-02	|	+0.6	|	-1.4	|	±3.4	|	±3.4	|	±0.2	|		|
|	2000.00	|	9.804E-03	|	+0.6	|	-1.5	|	±3.4	|	±3.4	|	±0.2	|		|
|	2050.00	|	8.812E-03	|	+0.6	|	-1.5	|	±3.5	|	±3.5	|	±0.2	|		|
|	2100.00	|	7.926E-03	|	+0.7	|	-1.6	|	±3.6	|	±3.6	|	±0.2	|		|
|	2150.00	|	7.135E-03	|	+0.7	|	-1.6	|	±3.6	|	±3.6	|	±0.2	|		|
|	2200.00	|	6.428E-03	|	+0.7	|	-1.7	|	±3.7	|	±3.7	|	±0.2	|		|
|	2250.00	|	5.794E-03	|	+0.7	|	-1.7	|	±3.8	|	±3.8	|	±0.2	|		|
|	2300.00	|	5.227E-03	|	+0.7	|	-1.8	|	±3.8	|	±3.8	|	±0.2	|		|
|	2350.00	|	4.717E-03	|	+0.8	|	-1.8	|	±3.9	|	±3.9	|	±0.2	|		|
|	2400.00	|	4.259E-03	|	+0.8	|	-1.8	|	±4.0	|	±4.0	|	±0.2	|		|
|	2450.00	|	3.848E-03	|	+0.8	|	-1.9	|	±4.1	|	±4.1	|	±0.2	|		|
|	2500.00	|	3.478E-03	|	+0.8	|	-1.9	|	±4.2	|	±4.1	|	±0.2	|		|
|	2550.00	|	3.145E-03	|	+0.9	|	-2.0	|	±4.2	|	±4.2	|	±0.2	|		|
|	2600.00	|	2.846E-03	|	+0.9	|	-2.0	|	±4.3	|	±4.3	|	±0.2	|		|
|	2650.00	|	2.575E-03	|	+0.9	|	-2.1	|	±4.4	|	±4.4	|	±0.2	|		|
|	2700.00	|	2.331E-03	|	+1.0	|	-2.1	|	±4.5	|	±4.5	|	±0.2	|		|
|	2750.00	|	2.112E-03	|	+1.0	|	-2.2	|	±4.6	|	±4.6	|	±0.2	|		|
|	2800.00	|	1.914E-03	|	+1.0	|	-2.2	|	±4.7	|	±4.7	|	±0.2	|		|
|	2850.00	|	1.734E-03	|	+1.0	|	-2.3	|	±4.8	|	±4.8	|	±0.2	|		|
|	2900.00	|	1.572E-03	|	+1.0	|	-2.3	|	±4.9	|	±4.9	|	±0.2	|		|
|	2950.00	|	1.426E-03	|	+1.1	|	-2.4	|	±5.0	|	±5.0	|	±0.2	|		|
|	3000.00	|	1.293E-03	|	+1.1	|	-2.4	|	±5.1	|	±5.1	|	±0.2	|		|
</tr>
</table>


---++ 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: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>VH</sub>=(p<sub>V</sub>+p<sub>H</sub>)<sup>2</sup> for QCD part. Uncertainty is estimated in the range 1/3 < &mu;/M<sub>VH</sub> < 3 (&mu;<sub>F</sub> and &mu;<sub>R</sub> are varied independently).
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  !PDF4LHC15_nnlo_mc (QCD part)
   * Photon-induced contribution of O(5%)
      * %RED% NOT included for total cross section %ENDCOLOR% (agrees with CERN Report 3 numbers within 1%). 
 
<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  |  1+&delta;<sub>EW</sub>  |  W<sup>+</sup>H (pb)  |  W<sup>-</sup>H (pb)  | 
|	10.00	|	2.592E+02	|	+1.2	|	-2.1	|	±2.1	|		|		|		|	1.503E+02	|	1.089E+02	|
|	15.00	|	1.609E+02	|	+1.1	|	-1.8	|	±2.0	|		|		|		|	9.357E+01	|	6.731E+01	|
|	20.00	|	1.079E+02	|	+0.7	|	-1.6	|	±2.0	|		|		|		|	6.281E+01	|	4.509E+01	|
|	25.00	|	7.606E+01	|	+1.0	|	-1.6	|	±2.0	|		|		|		|	4.438E+01	|	3.168E+01	|
|	30.00	|	5.555E+01	|	+0.8	|	-1.7	|	±2.0	|		|		|		|	3.255E+01	|	2.300E+01	|
|	35.00	|	4.165E+01	|	+0.7	|	-1.7	|	±2.0	|		|		|		|	2.445E+01	|	1.720E+01	|
|	40.00	|	3.186E+01	|	+0.7	|	-1.4	|	±2.0	|		|		|		|	1.876E+01	|	1.310E+01	|
|	45.00	|	2.484E+01	|	+0.7	|	-1.3	|	±2.0	|		|		|		|	1.464E+01	|	1.020E+01	|
|	50.00	|	1.965E+01	|	+0.7	|	-1.3	|	±1.9	|		|		|		|	1.162E+01	|	8.033E+00	|
|	55.00	|	1.574E+01	|	+0.9	|	-1.1	|	±1.8	|		|		|		|	9.323E+00	|	6.413E+00	|
|	60.00	|	1.279E+01	|	+0.5	|	-1.2	|	±1.8	|		|		|		|	7.597E+00	|	5.194E+00	|
|	65.00	|	1.048E+01	|	+0.5	|	-1.1	|	±1.8	|		|		|		|	6.234E+00	|	4.241E+00	|
|	70.00	|	8.654E+00	|	+0.5	|	-1.0	|	±1.8	|		|		|		|	5.162E+00	|	3.492E+00	|
|	75.00	|	7.222E+00	|	+0.3	|	-1.0	|	±1.8	|		|		|		|	4.320E+00	|	2.902E+00	|
|	80.00	|	6.066E+00	|	+0.4	|	-1.0	|	±1.8	|		|		|		|	3.636E+00	|	2.430E+00	|
|	85.00	|	5.125E+00	|	+0.6	|	-0.9	|	±1.8	|		|		|		|	3.075E+00	|	2.050E+00	|
|	90.00	|	4.360E+00	|	+0.5	|	-0.8	|	±1.8	|		|		|		|	2.619E+00	|	1.741E+00	|
|	95.00	|	3.735E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|		|	2.250E+00	|	1.485E+00	|
|	100.00	|	3.214E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|		|	1.940E+00	|	1.274E+00	|
|	105.00	|	2.781E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|		|	1.682E+00	|	1.099E+00	|
|	110.00	|	2.418E+00	|	+0.4	|	-0.7	|	±1.9	|		|		|		|	1.465E+00	|	9.526E-01	|
|	115.00	|	2.110E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|		|	1.281E+00	|	8.289E-01	|
|	120.00	|	1.848E+00	|	+0.5	|	-0.6	|	±1.8	|		|		|		|	1.124E+00	|	7.243E-01	|
|	125.00	|	1.627E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|		|	9.919E-01	|	6.349E-01	|
|	130.00	|	1.437E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|		|	8.772E-01	|	5.598E-01	|
|	135.00	|	1.272E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|		|	7.781E-01	|	4.941E-01	|
|	140.00	|	1.131E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|		|	6.931E-01	|	4.379E-01	|
|	145.00	|	1.009E+00	|	+0.5	|	-0.8	|	±1.8	|		|		|		|	6.189E-01	|	3.899E-01	|
|	150.00	|	9.016E-01	|	+0.6	|	-0.7	|	±1.8	|		|		|		|	5.542E-01	|	3.474E-01	|
|	160.00	|	7.268E-01	|	+0.5	|	-0.8	|	±1.8	|		|		|		|	4.484E-01	|	2.784E-01	|
|	170.00	|	5.915E-01	|	+0.6	|	-0.9	|	±1.8	|		|		|		|	3.661E-01	|	2.254E-01	|
|	180.00	|	4.862E-01	|	+0.6	|	-0.8	|	±1.9	|		|		|		|	3.019E-01	|	1.843E-01	|
|	190.00	|	4.025E-01	|	+0.7	|	-0.8	|	±1.9	|		|		|		|	2.508E-01	|	1.517E-01	|
|	200.00	|	3.361E-01	|	+0.7	|	-0.9	|	±1.9	|		|		|		|	2.100E-01	|	1.261E-01	|
|	210.00	|	2.826E-01	|	+0.8	|	-0.9	|	±1.9	|		|		|		|	1.771E-01	|	1.055E-01	|
|	220.00	|	2.392E-01	|	+0.8	|	-0.9	|	±1.9	|		|		|		|	1.503E-01	|	8.885E-02	|
|	230.00	|	2.037E-01	|	+0.8	|	-1.0	|	±2.0	|		|		|		|	1.284E-01	|	7.527E-02	|
|	240.00	|	1.743E-01	|	+0.9	|	-1.0	|	±2.0	|		|		|		|	1.102E-01	|	6.408E-02	|
|	250.00	|	1.500E-01	|	+0.9	|	-0.9	|	±2.0	|		|		|		|	9.508E-02	|	5.490E-02	|
|	260.00	|	1.297E-01	|	+0.9	|	-1.0	|	±2.0	|		|		|		|	8.248E-02	|	4.723E-02	|
|	270.00	|	1.127E-01	|	+0.9	|	-1.0	|	±2.0	|		|		|		|	7.186E-02	|	4.085E-02	|
|	280.00	|	9.828E-02	|	+1.0	|	-1.0	|	±2.0	|		|		|		|	6.281E-02	|	3.547E-02	|
|	290.00	|	8.609E-02	|	+1.0	|	-1.0	|	±2.0	|		|		|		|	5.517E-02	|	3.092E-02	|
|	300.00	|	7.567E-02	|	+1.1	|	-1.0	|	±2.1	|		|		|		|	4.861E-02	|	2.706E-02	|
|	310.00	|	6.677E-02	|	+1.1	|	-1.0	|	±2.1	|		|		|		|	4.301E-02	|	2.376E-02	|
|	320.00	|	5.910E-02	|	+1.1	|	-1.0	|	±2.1	|		|		|		|	3.817E-02	|	2.093E-02	|
|	330.00	|	5.247E-02	|	+1.1	|	-1.0	|	±2.2	|		|		|		|	3.397E-02	|	1.850E-02	|
|	340.00	|	4.675E-02	|	+1.1	|	-1.0	|	±2.2	|		|		|		|	3.033E-02	|	1.642E-02	|
|	350.00	|	4.175E-02	|	+1.2	|	-1.0	|	±2.2	|		|		|		|	2.716E-02	|	1.459E-02	|
|	360.00	|	3.738E-02	|	+1.2	|	-1.1	|	±2.3	|		|		|		|	2.437E-02	|	1.301E-02	|
|	370.00	|	3.357E-02	|	+1.2	|	-1.1	|	±2.3	|		|		|		|	2.194E-02	|	1.163E-02	|
|	380.00	|	3.022E-02	|	+1.2	|	-1.1	|	±2.3	|		|		|		|	1.979E-02	|	1.043E-02	|
|	390.00	|	2.726E-02	|	+1.2	|	-1.1	|	±2.4	|		|		|		|	1.789E-02	|	9.370E-03	|
|	400.00	|	2.464E-02	|	+1.2	|	-1.1	|	±2.4	|		|		|		|	1.621E-02	|	8.433E-03	|
|	410.00	|	2.233E-02	|	+1.2	|	-1.1	|	±2.4	|		|		|		|	1.472E-02	|	7.610E-03	|
|	420.00	|	2.026E-02	|	+1.2	|	-1.2	|	±2.4	|		|		|		|	1.338E-02	|	6.879E-03	|
|	430.00	|	1.842E-02	|	+1.3	|	-1.1	|	±2.4	|		|		|		|	1.219E-02	|	6.229E-03	|
|	440.00	|	1.679E-02	|	+1.3	|	-1.3	|	±2.5	|		|		|		|	1.114E-02	|	5.652E-03	|
|	450.00	|	1.532E-02	|	+1.3	|	-1.2	|	±2.5	|		|		|		|	1.018E-02	|	5.139E-03	|
|	460.00	|	1.401E-02	|	+1.3	|	-1.2	|	±2.5	|		|		|		|	9.331E-03	|	4.680E-03	|
|	470.00	|	1.283E-02	|	+1.3	|	-1.3	|	±2.5	|		|		|		|	8.562E-03	|	4.270E-03	|
|	480.00	|	1.176E-02	|	+1.4	|	-1.3	|	±2.5	|		|		|		|	7.863E-03	|	3.898E-03	|
|	490.00	|	1.081E-02	|	+1.3	|	-1.3	|	±2.5	|		|		|		|	7.239E-03	|	3.568E-03	|
|	500.00	|	9.937E-03	|	+1.4	|	-1.4	|	±2.5	|		|		|		|	6.667E-03	|	3.270E-03	|
|	550.00	|	6.667E-03	|	+1.5	|	-1.5	|	±2.8	|		|		|		|	4.513E-03	|	2.154E-03	|
|	600.00	|	4.601E-03	|	+1.5	|	-1.5	|	±3.0	|		|		|		|	3.140E-03	|	1.461E-03	|
|	650.00	|	3.249E-03	|	+1.6	|	-1.6	|	±3.2	|		|		|		|	2.235E-03	|	1.014E-03	|
|	700.00	|	2.342E-03	|	+1.6	|	-1.7	|	±3.3	|		|		|		|	1.622E-03	|	7.196E-04	|
|	750.00	|	1.718E-03	|	+1.7	|	-1.8	|	±3.6	|		|		|		|	1.198E-03	|	5.197E-04	|
|	800.00	|	1.278E-03	|	+1.7	|	-1.8	|	±3.8	|		|		|		|	8.969E-04	|	3.813E-04	|
|	850.00	|	9.639E-04	|	+1.7	|	-1.9	|	±4.0	|		|		|		|	6.802E-04	|	2.837E-04	|
|	900.00	|	7.353E-04	|	+1.8	|	-2.0	|	±4.2	|		|		|		|	5.217E-04	|	2.136E-04	|
|	950.00	|	5.665E-04	|	+1.8	|	-2.0	|	±4.4	|		|		|		|	4.040E-04	|	1.625E-04	|
|	1000.00	|	4.405E-04	|	+1.9	|	-2.1	|	±4.6	|		|		|		|	3.156E-04	|	1.249E-04	|
|	1050.00	|	3.454E-04	|	+1.9	|	-2.2	|	±5.0	|		|		|		|	2.485E-04	|	9.687E-05	|
|	1100.00	|	2.728E-04	|	+1.9	|	-2.2	|	±5.3	|		|		|		|	1.971E-04	|	7.570E-05	|
|	1150.00	|	2.169E-04	|	+2.0	|	-2.3	|	±5.6	|		|		|		|	1.573E-04	|	5.960E-05	|
|	1200.00	|	1.734E-04	|	+2.0	|	-2.3	|	±6.0	|		|		|		|	1.262E-04	|	4.721E-05	|
|	1250.00	|	1.395E-04	|	+2.0	|	-2.4	|	±6.3	|		|		|		|	1.018E-04	|	3.765E-05	|
|	1300.00	|	1.127E-04	|	+2.0	|	-2.4	|	±6.6	|		|		|		|	8.255E-05	|	3.018E-05	|
|	1350.00	|	9.152E-05	|	+2.1	|	-2.5	|	±6.9	|		|		|		|	6.720E-05	|	2.432E-05	|
|	1400.00	|	7.462E-05	|	+2.1	|	-2.5	|	±7.3	|		|		|		|	5.494E-05	|	1.968E-05	|
|	1450.00	|	6.108E-05	|	+2.1	|	-2.6	|	±7.6	|		|		|		|	4.507E-05	|	1.601E-05	|
|	1500.00	|	5.017E-05	|	+2.2	|	-2.6	|	±7.9	|		|		|		|	3.710E-05	|	1.307E-05	|
|	1550.00	|	4.135E-05	|	+2.2	|	-2.7	|	±8.2	|		|		|		|	3.063E-05	|	1.072E-05	|
|	1600.00	|	3.418E-05	|	+2.2	|	-2.7	|	±8.5	|		|		|		|	2.536E-05	|	8.816E-06	|
|	1650.00	|	2.834E-05	|	+2.2	|	-2.8	|	±8.9	|		|		|		|	2.106E-05	|	7.277E-06	|
|	1700.00	|	2.356E-05	|	+2.3	|	-2.8	|	±9.2	|		|		|		|	1.753E-05	|	6.027E-06	|
|	1750.00	|	1.963E-05	|	+2.3	|	-2.9	|	±9.5	|		|		|		|	1.462E-05	|	5.006E-06	|
|	1800.00	|	1.640E-05	|	+2.3	|	-2.9	|	±9.9	|		|		|		|	1.223E-05	|	4.170E-06	|
|	1850.00	|	1.372E-05	|	+2.3	|	-3.0	|	±10.2	|		|		|		|	1.024E-05	|	3.482E-06	|
|	1900.00	|	1.151E-05	|	+2.4	|	-3.1	|	±10.5	|		|		|		|	8.595E-06	|	2.914E-06	|
|	1950.00	|	9.669E-06	|	+2.4	|	-3.1	|	±10.9	|		|		|		|	7.224E-06	|	2.445E-06	|
|	2000.00	|	8.137E-06	|	+2.4	|	-3.1	|	±11.3	|		|		|		|	6.080E-06	|	2.057E-06	|
</tr>
</table>


---++ ZH  Process

   * Cross sections are calculated at NNLO QCD accuracy.
      * Calculations are the same as CERN Report 3. 
      * gg&#8594;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: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>VH</sub>=(p<sub>V</sub>+p<sub>H</sub>)<sup>2</sup> for QCD part. Uncertainty is estimated in the range 1/3 < &mu;/M<sub>VH</sub> < 3 (&mu;<sub>F</sub> and &mu;<sub>R</sub> 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
      * %RED% NOT included for total cross section %ENDCOLOR% (agrees with CERN Report 3 numbers). 

<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  |  1+&delta;<sub>EW</sub>  |  &#963;(gg&#8594;ZH) (pb)  |
|	10.00	|	1.154E+02	|	+0..9	|	-1..5	|	±2.2	|		|		|		|		|
|	15.00	|	7.371E+01	|	+1..3	|	-1..8	|	±2.2	|		|		|		|		|
|	20.00	|	5.058E+01	|	+0..6	|	-1..8	|	±2.2	|		|		|		|		|
|	25.00	|	3.630E+01	|	+0..7	|	-1..6	|	±2.1	|		|		|		|		|
|	30.00	|	2.698E+01	|	+0..5	|	-1..5	|	±2.1	|		|		|		|		|
|	35.00	|	2.055E+01	|	+0..3	|	-1..3	|	±2.1	|		|		|		|		|
|	40.00	|	1.597E+01	|	+0..5	|	-1..1	|	±2.0	|		|		|		|		|
|	45.00	|	1.264E+01	|	+0..6	|	-1..2	|	±2.0	|		|		|		|		|
|	50.00	|	1.014E+01	|	+0..7	|	-1..1	|	±1.9	|		|		|		|		|
|	55.00	|	8.241E+00	|	+0..9	|	-1..0	|	±1.9	|		|		|		|		|
|	60.00	|	6.775E+00	|	+1..1	|	-1..0	|	±1.8	|		|		|		|		|
|	65.00	|	5.628E+00	|	+1..1	|	-1..2	|	±1.8	|		|		|		|		|
|	70.00	|	4.709E+00	|	+1..3	|	-1..2	|	±1.8	|		|		|		|		|
|	75.00	|	3.990E+00	|	+1..2	|	-1..7	|	±1.8	|		|		|		|		|
|	80.00	|	3.386E+00	|	+1..7	|	-1..5	|	±1.8	|		|		|		|		|
|	85.00	|	2.899E+00	|	+2..0	|	-1..8	|	±1.7	|		|		|		|		|
|	90.00	|	2.503E+00	|	+1..8	|	-1..9	|	±1.7	|		|		|		|		|
|	95.00	|	2.168E+00	|	+2..3	|	-2..0	|	±1.7	|		|		|		|		|
|	100.00	|	1.890E+00	|	+2..4	|	-2..3	|	±1.6	|		|		|		|		|
|	105.00	|	1.654E+00	|	+2..6	|	-2..3	|	±1.6	|		|		|		|		|
|	110.00	|	1.454E+00	|	+2..9	|	-2..5	|	±1.6	|		|		|		|		|
|	115.00	|	1.284E+00	|	+3..2	|	-2..6	|	±1.6	|		|		|		|		|
|	120.00	|	1.138E+00	|	+3..4	|	-2..8	|	±1.7	|		|		|		|		|
|	125.00	|	1.014E+00	|	+3..5	|	-3..0	|	±1.6	|		|		|		|		|
|	130.00	|	9.044E-01	|	+3..8	|	-3..1	|	±1.6	|		|		|		|		|
|	135.00	|	8.099E-01	|	+4..0	|	-3..1	|	±1.6	|		|		|		|		|
|	140.00	|	7.278E-01	|	+4..2	|	-3..3	|	±1.6	|		|		|		|		|
|	145.00	|	6.554E-01	|	+4..3	|	-3..5	|	±1.6	|		|		|		|		|
|	150.00	|	5.911E-01	|	+4..5	|	-3..5	|	±1.6	|		|		|		|		|
|	160.00	|	4.844E-01	|	+4..8	|	-3..8	|	±1.6	|		|		|		|		|
|	170.00	|	3.996E-01	|	+4..9	|	-3..9	|	±1.6	|		|		|		|		|
|	180.00	|	3.319E-01	|	+5..1	|	-4..1	|	±1.6	|		|		|		|		|
|	190.00	|	2.770E-01	|	+5..1	|	-4..2	|	±1.5	|		|		|		|		|
|	200.00	|	2.317E-01	|	+5..4	|	-4..2	|	±1.5	|		|		|		|		|
|	210.00	|	1.945E-01	|	+5..2	|	-4..1	|	±1.5	|		|		|		|		|
|	220.00	|	1.636E-01	|	+5..2	|	-4..0	|	±1.5	|		|		|		|		|
|	230.00	|	1.382E-01	|	+4..9	|	-4..0	|	±1.6	|		|		|		|		|
|	240.00	|	1.171E-01	|	+4..7	|	-3..8	|	±1.6	|		|		|		|		|
|	250.00	|	9.940E-02	|	+4..5	|	-3..7	|	±1.6	|		|		|		|		|
|	260.00	|	8.475E-02	|	+4..3	|	-3..5	|	±1.6	|		|		|		|		|
|	270.00	|	7.261E-02	|	+4..0	|	-3..3	|	±1.6	|		|		|		|		|
|	280.00	|	6.247E-02	|	+3..8	|	-3..0	|	±1.6	|		|		|		|		|
|	290.00	|	5.404E-02	|	+3..5	|	-3..0	|	±1.6	|		|		|		|		|
|	300.00	|	4.691E-02	|	+3..3	|	-2..7	|	±1.6	|		|		|		|		|
|	310.00	|	4.093E-02	|	+3..1	|	-2..6	|	±1.6	|		|		|		|		|
|	320.00	|	3.586E-02	|	+2..9	|	-2..5	|	±1.6	|		|		|		|		|
|	330.00	|	3.154E-02	|	+2..7	|	-2..3	|	±1.6	|		|		|		|		|
|	340.00	|	2.788E-02	|	+2..6	|	-2..2	|	±1.7	|		|		|		|		|
|	350.00	|	2.478E-02	|	+2..6	|	-2..2	|	±1.7	|		|		|		|		|
|	360.00	|	2.214E-02	|	+2..6	|	-2..2	|	±1.7	|		|		|		|		|
|	370.00	|	1.987E-02	|	+2..6	|	-2..2	|	±1.8	|		|		|		|		|
|	380.00	|	1.788E-02	|	+2..6	|	-2..3	|	±1.8	|		|		|		|		|
|	390.00	|	1.614E-02	|	+2..7	|	-2..3	|	±1.8	|		|		|		|		|
|	400.00	|	1.461E-02	|	+2..8	|	-2..4	|	±1.8	|		|		|		|		|
|	410.00	|	1.327E-02	|	+2..9	|	-2..5	|	±1.8	|		|		|		|		|
|	420.00	|	1.207E-02	|	+3..0	|	-2..5	|	±1.8	|		|		|		|		|
|	430.00	|	1.101E-02	|	+3..2	|	-2..6	|	±1.9	|		|		|		|		|
|	440.00	|	1.006E-02	|	+3..2	|	-2..8	|	±1.9	|		|		|		|		|
|	450.00	|	9.219E-03	|	+3..4	|	-2..9	|	±1.9	|		|		|		|		|
|	460.00	|	8.466E-03	|	+3..4	|	-3..0	|	±1.9	|		|		|		|		|
|	470.00	|	7.786E-03	|	+3..6	|	-3..2	|	±1.9	|		|		|		|		|
|	480.00	|	7.176E-03	|	+3..7	|	-3..3	|	±1.9	|		|		|		|		|
|	490.00	|	6.621E-03	|	+3..9	|	-3..4	|	±1.9	|		|		|		|		|
|	500.00	|	6.122E-03	|	+4..1	|	-3..6	|	±1.9	|		|		|		|		|
|	550.00	|	4.229E-03	|	+4..9	|	-4..3	|	±2.0	|		|		|		|		|
|	600.00	|	3.012E-03	|	+5..8	|	-5..1	|	±2.1	|		|		|		|		|
|	650.00	|	2.200E-03	|	+6..8	|	-5..8	|	±2.2	|		|		|		|		|
|	700.00	|	1.643E-03	|	+7..6	|	-6..6	|	±2.2	|		|		|		|		|
|	750.00	|	1.247E-03	|	+8..5	|	-7..4	|	±2.3	|		|		|		|		|
|	800.00	|	9.603E-04	|	+9..3	|	-8..0	|	±2.4	|		|		|		|		|
|	850.00	|	7.490E-04	|	+10..0	|	-8..7	|	±2.5	|		|		|		|		|
|	900.00	|	5.900E-04	|	+10..8	|	-9..2	|	±2.6	|		|		|		|		|
|	950.00	|	4.690E-04	|	+11..6	|	-9..8	|	±2.6	|		|		|		|		|
|	1000.00	|	3.761E-04	|	+12..1	|	-10..3	|	±2.8	|		|		|		|		|
|	1050.00	|	3.037E-04	|	+12..6	|	-10..9	|	±3.0	|		|		|		|		|
|	1100.00	|	2.470E-04	|	+13..1	|	-11..4	|	±3.1	|		|		|		|		|
|	1150.00	|	2.016E-04	|	+13..8	|	-11..8	|	±3.3	|		|		|		|		|
|	1200.00	|	1.656E-04	|	+14..3	|	-12..2	|	±3.5	|		|		|		|		|
|	1250.00	|	1.368E-04	|	+14..9	|	-12..7	|	±3.7	|		|		|		|		|
|	1300.00	|	1.134E-04	|	+15..2	|	-13..2	|	±3.9	|		|		|		|		|
|	1350.00	|	9.429E-05	|	+15..6	|	-13..5	|	±4.0	|		|		|		|		|
|	1400.00	|	7.874E-05	|	+16..4	|	-13..8	|	±4.2	|		|		|		|		|
|	1450.00	|	6.595E-05	|	+16..6	|	-14..1	|	±4.4	|		|		|		|		|
|	1500.00	|	5.546E-05	|	+17..1	|	-14..5	|	±4.6	|		|		|		|		|
|	1550.00	|	4.667E-05	|	+17..5	|	-14..8	|	±4.8	|		|		|		|		|
|	1600.00	|	3.953E-05	|	+17..6	|	-15..2	|	±4.9	|		|		|		|		|
|	1650.00	|	3.343E-05	|	+18..2	|	-15..3	|	±5.1	|		|		|		|		|
|	1700.00	|	2.836E-05	|	+18..8	|	-15..5	|	±5.3	|		|		|		|		|
|	1750.00	|	2.415E-05	|	+19..1	|	-15..9	|	±5.5	|		|		|		|		|
|	1800.00	|	2.060E-05	|	+19..3	|	-16..1	|	±5.7	|		|		|		|		|
|	1850.00	|	1.762E-05	|	+19..4	|	-16..5	|	±5.9	|		|		|		|		|
|	1900.00	|	1.507E-05	|	+20..0	|	-16..7	|	±6.1	|		|		|		|		|
|	1950.00	|	1.293E-05	|	+20..3	|	-16..9	|	±6.3	|		|		|		|		|
|	2000.00	|	1.111E-05	|	+20..5	|	-17..3	|	±6.7	|		|		|		|		|
</tr>
</table>


---++ 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: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>top</sub>+M<sub>H</sub>/2, uncertainty estimated in the range 1/2 < &mu;/(M<sub>top</sub>+M<sub>H</sub>/2) < 2 (with 1/2 < &mu;<sub>F</sub>/&mu;<sub>R</sub> < 2 constraint).
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  !PDF4LHC15_nlo_30_pdfas

<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  |  1+&delta;<sub>EW</sub>  |

</tr>
</table>


---++ 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: &mu;<sub>F</sub>=M<sub>H</sub>/4, &mu;<sub>R</sub>=M<sub>H</sub>,
      * 4FS: &mu;<sub>F</sub>=&mu;<sub>R</sub>=(M<sub>H</sub>+2M<sub>b</sub>)/4, 
      * scale with 7-point variation by a factor of 2 in both cases. 
   * Uncertainties
      * 5FS: Linearly added scale + (PDF&#8853;&alpha;<sub>s</sub>) + M<sub>b</sub> + &mu;<sub>b</sub> (PDF and &alpha;<sub>s</sub> 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 M<sub>b</sub>-threshold and evolved upwards, while generating a b-PDF set at high scale.
      * 4FS: !PDF4LHC15_nlo_nf4_100

<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +(QCD Scale+PDF+&alpha;<sub>s</sub>) %  |  -(QCD Scale+PDF+&alpha;<sub>s</sub>) %  |  1+&delta;<sub>EW</sub>  |
|	10.00	|	1.229E+02	|	+92.4	|	-61.0	|		|
|	15.00	|	6.908E+01	|	+67.3	|	-53.3	|		|
|	20.00	|	4.444E+01	|	+54.1	|	-48.0	|		|
|	25.00	|	2.994E+01	|	+45.2	|	-43.9	|		|
|	30.00	|	2.124E+01	|	+40.5	|	-40.8	|		|
|	35.00	|	1.532E+01	|	+35.8	|	-38.1	|		|
|	40.00	|	1.136E+01	|	+34.6	|	-40.2	|		|
|	45.00	|	8.619E+00	|	+32.8	|	-41.3	|		|
|	50.00	|	6.769E+00	|	+31.2	|	-40.6	|		|
|	55.00	|	5.425E+00	|	+30.0	|	-39.3	|		|
|	60.00	|	4.364E+00	|	+28.1	|	-37.9	|		|
|	65.00	|	3.559E+00	|	+27.1	|	-36.3	|		|
|	70.00	|	2.936E+00	|	+26.2	|	-34.9	|		|
|	75.00	|	2.453E+00	|	+25.4	|	-33.4	|		|
|	80.00	|	2.056E+00	|	+24.6	|	-32.0	|		|
|	85.00	|	1.735E+00	|	+24.0	|	-30.8	|		|
|	90.00	|	1.481E+00	|	+23.4	|	-29.7	|		|
|	95.00	|	1.264E+00	|	+22.6	|	-28.6	|		|
|	100.00	|	1.090E+00	|	+22.3	|	-27.7	|		|
|	105.00	|	9.433E-01	|	+21.8	|	-26.9	|		|
|	110.00	|	8.216E-01	|	+21.3	|	-26.1	|		|
|	115.00	|	7.171E-01	|	+20.7	|	-25.3	|		|
|	120.00	|	6.288E-01	|	+20.4	|	-24.7	|		|
|	125.00	|	5.529E-01	|	+20.0	|	-24.0	|		|
|	130.00	|	4.878E-01	|	+21.4	|	-23.5	|		|
|	135.00	|	4.329E-01	|	+19.4	|	-23.0	|		|
|	140.00	|	3.853E-01	|	+19.3	|	-22.5	|		|
|	145.00	|	3.439E-01	|	+19.1	|	-22.1	|		|
|	150.00	|	3.080E-01	|	+18.8	|	-21.6	|		|
|	160.00	|	2.488E-01	|	+18.4	|	-20.8	|		|
|	170.00	|	2.025E-01	|	+17.9	|	-19.9	|		|
|	180.00	|	1.667E-01	|	+17.5	|	-19.2	|		|
|	190.00	|	1.381E-01	|	+17.1	|	-18.7	|		|
|	200.00	|	1.156E-01	|	+16.7	|	-18.1	|		|
|	210.00	|	9.698E-02	|	+16.6	|	-17.6	|		|
|	220.00	|	8.201E-02	|	+16.3	|	-17.3	|		|
|	230.00	|	6.983E-02	|	+16.1	|	-17.1	|		|
|	240.00	|	5.973E-02	|	+15.9	|	-16.9	|		|
|	250.00	|	5.135E-02	|	+15.6	|	-16.7	|		|
|	260.00	|	4.430E-02	|	+15.4	|	-16.4	|		|
|	270.00	|	3.843E-02	|	+15.2	|	-16.2	|		|
|	280.00	|	3.342E-02	|	+15.0	|	-16.0	|		|
|	290.00	|	2.926E-02	|	+15.0	|	-15.9	|		|
|	300.00	|	2.563E-02	|	+14.9	|	-15.8	|		|
|	310.00	|	2.252E-02	|	+14.8	|	-15.7	|		|
|	320.00	|	1.990E-02	|	+15.0	|	-15.6	|		|
|	330.00	|	1.759E-02	|	+14.6	|	-15.5	|		|
|	340.00	|	1.564E-02	|	+14.6	|	-15.4	|		|
|	350.00	|	1.390E-02	|	+14.6	|	-15.3	|		|
|	360.00	|	1.239E-02	|	+14.3	|	-15.2	|		|
|	370.00	|	1.109E-02	|	+14.0	|	-15.2	|		|
|	380.00	|	9.944E-03	|	+14.2	|	-15.1	|		|
|	390.00	|	8.934E-03	|	+14.3	|	-15.1	|		|
|	400.00	|	8.021E-03	|	+14.1	|	-14.9	|		|
|	410.00	|	7.241E-03	|	+14.2	|	-14.9	|		|
|	420.00	|	6.548E-03	|	+14.3	|	-14.8	|		|
|	430.00	|	5.927E-03	|	+14.3	|	-14.7	|		|
|	440.00	|	5.373E-03	|	+14.3	|	-14.7	|		|
|	450.00	|	4.883E-03	|	+14.2	|	-14.7	|		|
|	460.00	|	4.449E-03	|	+14.2	|	-14.6	|		|
|	470.00	|	4.045E-03	|	+14.1	|	-14.6	|		|
|	480.00	|	3.694E-03	|	+14.4	|	-14.6	|		|
|	490.00	|	3.369E-03	|	+14.2	|	-14.5	|		|
|	500.00	|	3.088E-03	|	+14.4	|	-14.5	|		|
|	550.00	|	2.016E-03	|	+14.1	|	-14.4	|		|
|	600.00	|	1.355E-03	|	+14.5	|	-14.5	|		|
|	650.00	|	9.318E-04	|	+14.8	|	-14.6	|		|
|	700.00	|	6.540E-04	|	+15.2	|	-14.7	|		|
|	750.00	|	4.674E-04	|	+15.6	|	-14.9	|		|
|	800.00	|	3.391E-04	|	+16.0	|	-14.8	|		|
|	850.00	|	2.495E-04	|	+16.4	|	-15.0	|		|
|	900.00	|	1.858E-04	|	+16.8	|	-15.3	|		|
|	950.00	|	1.402E-04	|	+17.3	|	-15.7	|		|
|	1000.00	|	1.067E-04	|	+17.8	|	-15.9	|		|
|	1050.00	|	8.200E-05	|	+18.1	|	-16.3	|		|
|	1100.00	|	6.359E-05	|	+18.3	|	-16.7	|		|
|	1150.00	|	4.958E-05	|	+18.5	|	-17.2	|		|
|	1200.00	|	3.901E-05	|	+18.6	|	-17.6	|		|
|	1250.00	|	3.088E-05	|	+18.8	|	-18.2	|		|
|	1300.00	|	2.458E-05	|	+18.9	|	-18.6	|		|
|	1350.00	|	1.969E-05	|	+19.1	|	-19.2	|		|
|	1400.00	|	1.586E-05	|	+19.5	|	-19.9	|		|
|	1450.00	|	1.283E-05	|	+19.8	|	-20.7	|		|
|	1500.00	|	1.043E-05	|	+20.2	|	-21.5	|		|
|	1550.00	|	8.512E-06	|	+20.6	|	-22.2	|		|
|	1600.00	|	6.968E-06	|	+21.1	|	-23.0	|		|
|	1650.00	|	5.736E-06	|	+21.7	|	-23.7	|		|
|	1700.00	|	4.733E-06	|	+22.5	|	-24.2	|		|
|	1750.00	|	3.920E-06	|	+23.3	|	-24.8	|		|
|	1800.00	|	3.235E-06	|	+24.1	|	-25.3	|		|
|	1850.00	|	2.714E-06	|	+25.0	|	-25.9	|		|
|	1900.00	|	2.270E-06	|	+25.9	|	-26.4	|		|
|	1950.00	|	1.901E-06	|	+26.5	|	-27.0	|		|
|	2000.00	|	1.598E-06	|	+27.2	|	-27.6	|		|
|	2050.00	|	1.347E-06	|	+27.9	|	-28.2	|		|
|	2100.00	|	1.137E-06	|	+28.5	|	-28.8	|		|
|	2150.00	|	9.613E-07	|	+29.1	|	-29.5	|		|
|	2200.00	|	8.154E-07	|	+29.8	|	-30.1	|		|
|	2250.00	|	6.927E-07	|	+30.4	|	-30.8	|		|
|	2300.00	|	5.899E-07	|	+31.1	|	-31.6	|		|
|	2350.00	|	5.028E-07	|	+31.7	|	-32.6	|		|
|	2400.00	|	4.373E-07	|	+32.4	|	-33.4	|		|
|	2450.00	|	3.676E-07	|	+33.4	|	-34.6	|		|
|	2500.00	|	3.108E-07	|	+34.4	|	-35.8	|		|
|	2550.00	|	2.705E-07	|	+35.3	|	-36.7	|		|
|	2600.00	|	2.325E-07	|	+36.4	|	-37.7	|		|
|	2650.00	|	1.966E-07	|	+38.0	|	-39.3	|		|
|	2700.00	|	1.636E-07	|	+39.1	|	-40.8	|		|
|	2750.00	|	1.493E-07	|	+39.1	|	-40.9	|		|
|	2800.00	|	1.229E-07	|	+41.0	|	-43.0	|		|
|	2850.00	|	1.113E-07	|	+41.2	|	-43.1	|		|
|	2900.00	|	9.641E-08	|	+42.4	|	-44.1	|		|
|	2950.00	|	8.285E-08	|	+43.7	|	-45.2	|		|
|	3000.00	|	7.259E-08	|	+44.9	|	-45.9	|		|
</tr>
</table>


---++ tH  Process (t-ch)

   * Cross sections are calculated at NLO QCD accuracy in 5FS. 
   * Program: !MadGraph5_aMC@NLO
   * QCD scales: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=(M<sub>top</sub>+M<sub>H</sub>)/4, uncertainty estimated in the range 1/2 < &mu;/{(M<sub>top</sub>+M<sub>H</sub>)/4} < 2 (with 1/2 < &mu;<sub>F</sub>/&mu;<sub>R</sub> < 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.

<table>
<tr>
|  m<sub>H</sub> (!GeV)  | Cross Section (pb) | +(QCD Scale + FS) % | -(QCD Scale + FS) % | &pm;(PDF+&alpha;<sub>s</sub>) % | &pm;PDF % | &pm;&alpha;<sub>s</sub> % |  1+&delta;<sub>EW</sub>  |  tH (pb)  |  tbarH (pb)  | 
|	10.00	|	2.128E+00	|	+8.0	|	-11.8	|	±2.5	|	±2.3	|	±0.9	|		|	1.347E+00	|	7.890E-01	|
|	15.00	|	1.474E+00	|	+8.2	|	-12.6	|	±2.5	|	±2.4	|	±0.9	|		|	9.350E-01	|	5.380E-01	|
|	20.00	|	1.084E+00	|	+8.5	|	-12.8	|	±2.6	|	±2.4	|	±0.9	|		|	6.900E-01	|	3.930E-01	|
|	30.00	|	6.543E-01	|	+8.7	|	-12.5	|	±2.7	|	±2.5	|	±0.9	|		|	4.198E-01	|	2.347E-01	|
|	45.00	|	3.632E-01	|	+8.8	|	-11.9	|	±2.8	|	±2.6	|	±1.0	|		|	2.352E-01	|	1.281E-01	|
|	70.00	|	1.837E-01	|	+8.4	|	-10.9	|	±3.1	|	±2.9	|	±1.0	|		|	1.120E-01	|	6.370E-02	|
|	100.00	|	1.135E-01	|	+7.3	|	-12.9	|	±3.4	|	±3.3	|	±1.1	|		|	7.430E-02	|	3.910E-02	|
|	150.00	|	7.781E-02	|	+5.7	|	-16.3	|	±3.8	|	±3.6	|	±1.2	|		|	5.074E-02	|	2.689E-02	|
|	200.00	|	6.363E-02	|	+4.8	|	-18.0	|	±3.9	|	±3.7	|	±1.3	|		|	4.156E-02	|	2.205E-02	|
|	300.00	|	4.622E-02	|	+3.8	|	-19.9	|	±4.1	|	±3.9	|	±1.3	|		|	3.036E-02	|	1.594E-02	|
|	450.00	|	2.889E-02	|	+3.0	|	-21.9	|	±4.5	|	±4.3	|	±1.3	|		|	1.921E-02	|	9.690E-03	|
|	700.00	|	1.349E-02	|	+2.3	|	-24.8	|	±5.1	|	±4.9	|	±1.4	|		|	9.150E-03	|	4.340E-03	|
|	1000.00	|	5.750E-03	|	+2.0	|	-27.9	|	±6.0	|	±5.7	|	±1.6	|		|	3.980E-03	|	1.780E-03	|
|	1500.00	|	1.570E-03	|	+2.0	|	-31.9	|	±7.7	|	±7.4	|	±1.9	|		|	1.120E-03	|	4.600E-04	|
|	2000.00	|	4.760E-04	|	+2.3	|	-35.3	|	±9.9	|	±9.6	|	±2.4	|		|	3.450E-04	|	1.300E-04	|
|	3000.00	|	4.990E-05	|	+3.3	|	-41.0	|	±15.4	|	±14.9	|	±3.9	|		|	3.750E-05	|	1.240E-05	|
</tr>
</table>

---++ tH  Process (s-ch)

   * Cross sections are calculated at NLO QCD accuracy in 5FS. 
   * Program: !MadGraph5_aMC@NLO
   * QCD scales: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=(M<sub>top</sub>+M<sub>H</sub>)/2, uncertainty estimated in the range 1/2 < &mu;/{(M<sub>top</sub>+M<sub>H</sub>)/2} < 2 (with 1/2 < &mu;<sub>F</sub>/&mu;<sub>R</sub> < 2 constraint).
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  
      * !PDF4LHC15_nlo_30_pdfas (5FS) 

<table>
<tr>
|  m<sub>H</sub> (!GeV)  | Cross Section (pb) | +QCD Scale % | -QCD Scale % | &pm;(PDF+&alpha;<sub>s</sub>) % | &pm;PDF % | &pm;&alpha;<sub>s</sub> % |  1+&delta;<sub>EW</sub>  |  tH (pb)  |  tbarH (pb)  | 
|	10.00	|	1.153E-01	|	+2.4	|	-2.0	|	±1.9	|	±1.8	|	±0.6	|		|	7.140E-02	|	4.380E-02	|
|	15.00	|	8.183E-02	|	+2.4	|	-1.9	|	±1.9	|	±1.8	|	±0.5	|		|	5.082E-02	|	3.105E-02	|
|	20.00	|	6.175E-02	|	+2.4	|	-1.9	|	±1.9	|	±1.8	|	±0.5	|		|	3.847E-02	|	2.324E-02	|
|	30.00	|	3.870E-02	|	+2.3	|	-1.9	|	±1.9	|	±1.8	|	±0.5	|		|	2.426E-02	|	1.446E-02	|
|	45.00	|	2.205E-02	|	+2.2	|	-1.8	|	±1.9	|	±1.9	|	±0.4	|		|	1.390E-02	|	8.130E-03	|
|	70.00	|	1.054E-02	|	+2.2	|	-1.7	|	±2.0	|	±2.0	|	±0.4	|		|	6.716E-03	|	3.820E-03	|
|	100.00	|	5.248E-03	|	+2.3	|	-1.6	|	±2.1	|	±2.0	|	±0.3	|		|	3.389E-03	|	1.865E-03	|
|	150.00	|	2.139E-03	|	+2.3	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|		|	1.403E-03	|	7.370E-04	|
|	200.00	|	1.062E-03	|	+2.3	|	-1.9	|	±2.4	|	±2.4	|	±0.1	|		|	7.050E-04	|	3.550E-04	|
|	300.00	|	3.630E-04	|	+2.3	|	-2.0	|	±2.7	|	±2.7	|	±0.0	|		|	2.470E-04	|	1.160E-04	|
|	450.00	|	1.110E-04	|	+2.0	|	-2.0	|	±3.2	|	±3.2	|	±0.2	|		|	7.800E-05	|	3.400E-05	|
|	700.00	|	2.610E-05	|	+2.0	|	-2.3	|	±3.9	|	±3.9	|	±0.4	|		|	1.880E-05	|	7.300E-06	|
|	1000.00	|	6.590E-06	|	+2.0	|	-2.6	|	±4.8	|	±4.7	|	±0.6	|		|	4.880E-06	|	1.720E-06	|
|	1500.00	|	9.860E-07	|	+2.3	|	-3.1	|	±6.0	|	±5.9	|	±1.0	|		|	7.450E-07	|	2.390E-07	|
|	2000.00	|	1.850E-07	|	+2.6	|	-3.7	|	±7.0	|	±6.9	|	±1.3	|		|	1.420E-07	|	4.400E-08	|
|	3000.00	|	8.700E-09	|	+3.6	|	-4.8	|	±10.7	|	±10.5	|	±2.1	|		|	6.580E-09	|	2.120E-09	|
</tr>
</table>

-- Main.ReiTanaka - 2016-03-01
Topic revision: r17 - 2016-12-08 - MarcoPieri
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