CERNYellowReportPageBSMAt7TeV < LHCPhysics

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---+ !BSM Higgs production cross sections at &#8730;s = 7 !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	|	4.101E+03	|	+47.3	|	-36.8	|	±6.2	|	±5.6	|	±2.7	|	0.0000	|
|	15.00	|	2.370E+03	|	+33.4	|	-27.3	|	±4.9	|	±4.0	|	±2.8	|	0.0000	|
|	20.00	|	1.092E+03	|	+24.9	|	-20.9	|	±4.3	|	±3.1	|	±2.9	|	0.0000	|
|	25.00	|	5.717E+02	|	+20.3	|	-16.9	|	±4.0	|	±2.6	|	±3.0	|	0.0000	|
|	30.00	|	3.402E+02	|	+18.0	|	-14.6	|	±3.9	|	±2.5	|	±3.0	|	0.0000	|
|	35.00	|	2.243E+02	|	+15.8	|	-13.3	|	±3.8	|	±2.3	|	±3.0	|	0.0000	|
|	40.00	|	1.598E+02	|	+14.1	|	-12.6	|	±3.7	|	±2.2	|	±3.0	|	0.0000	|
|	45.00	|	1.206E+02	|	+12.8	|	-11.8	|	±3.7	|	±2.1	|	±3.0	|	0.0000	|
|	50.00	|	9.490E+01	|	+11.8	|	-11.3	|	±3.6	|	±2.1	|	±3.0	|	0.0000	|
|	55.00	|	7.710E+01	|	+11.1	|	-10.8	|	±3.6	|	±2.0	|	±2.9	|	0.0000	|
|	60.00	|	6.414E+01	|	+10.5	|	-10.4	|	±3.5	|	±2.0	|	±2.9	|	0.0000	|
|	65.00	|	5.438E+01	|	+9.9	|	-10.0	|	±3.5	|	±2.0	|	±2.8	|	0.0000	|
|	70.00	|	4.679E+01	|	+9.5	|	-9.7	|	±3.4	|	±1.9	|	±2.8	|	0.0000	|
|	75.00	|	4.073E+01	|	+9.2	|	-9.5	|	±3.4	|	±1.9	|	±2.8	|	0.0000	|
|	80.00	|	3.580E+01	|	+8.9	|	-9.2	|	±3.3	|	±1.9	|	±2.8	|	0.0000	|
|	85.00	|	3.172E+01	|	+8.6	|	-9.0	|	±3.3	|	±1.9	|	±2.7	|	0.0000	|
|	90.00	|	2.830E+01	|	+8.4	|	-8.8	|	±3.3	|	±1.9	|	±2.7	|	0.0000	|
|	95.00	|	2.539E+01	|	+8.2	|	-8.7	|	±3.3	|	±1.9	|	±2.7	|	0.0000	|
|	100.00	|	2.291E+01	|	+8.0	|	-8.5	|	±3.3	|	±1.9	|	±2.7	|	1.0418	|
|	105.00	|	2.077E+01	|	+7.8	|	-8.4	|	±3.2	|	±1.9	|	±2.6	|	1.0436	|
|	110.00	|	1.891E+01	|	+7.7	|	-8.3	|	±3.2	|	±1.9	|	±2.6	|	1.0455	|
|	115.00	|	1.727E+01	|	+7.5	|	-8.2	|	±3.2	|	±1.8	|	±2.6	|	1.0474	|
|	120.00	|	1.583E+01	|	+7.4	|	-8.0	|	±3.2	|	±1.8	|	±2.6	|	1.0494	|
|	125.00	|	1.456E+01	|	+7.3	|	-7.9	|	±3.2	|	±1.8	|	±2.6	|	1.0514	|
|	130.00	|	1.343E+01	|	+7.1	|	-7.8	|	±3.2	|	±1.8	|	±2.6	|	1.0534	|
|	135.00	|	1.242E+01	|	+7.0	|	-7.7	|	±3.2	|	±1.8	|	±2.6	|	1.0553	|
|	140.00	|	1.152E+01	|	+6.9	|	-7.7	|	±3.2	|	±1.8	|	±2.6	|	1.0571	|
|	145.00	|	1.071E+01	|	+6.8	|	-7.6	|	±3.1	|	±1.8	|	±2.6	|	1.0587	|
|	150.00	|	9.973E+00	|	+6.8	|	-7.5	|	±3.1	|	±1.8	|	±2.5	|	1.0598	|
|	160.00	|	8.707E+00	|	+6.6	|	-7.4	|	±3.1	|	±1.9	|	±2.5	|	1.0486	|
|	170.00	|	7.664E+00	|	+6.4	|	-7.2	|	±3.2	|	±1.9	|	±2.5	|	1.0206	|
|	180.00	|	6.790E+00	|	+6.3	|	-7.1	|	±3.2	|	±1.9	|	±2.5	|	1.0053	|
|	190.00	|	6.056E+00	|	+6.2	|	-7.0	|	±3.2	|	±1.9	|	±2.5	|	0.9872	|
|	200.00	|	5.436E+00	|	+6.2	|	-6.9	|	±3.2	|	±1.9	|	±2.5	|	0.9793	|
|	210.00	|	4.908E+00	|	+6.1	|	-6.8	|	±3.2	|	±1.9	|	±2.5	|	0.9761	|
|	220.00	|	4.456E+00	|	+6.1	|	-6.7	|	±3.2	|	±2.0	|	±2.5	|	0.9749	|
|	230.00	|	4.067E+00	|	+6.1	|	-6.6	|	±3.2	|	±2.0	|	±2.5	|	0.9749	|
|	240.00	|	3.734E+00	|	+6.0	|	-6.5	|	±3.2	|	±2.0	|	±2.5	|	0.9755	|
|	250.00	|	3.446E+00	|	+6.0	|	-6.4	|	±3.3	|	±2.1	|	±2.5	|	0.9762	|
|	260.00	|	3.196E+00	|	+6.0	|	-6.4	|	±3.3	|	±2.1	|	±2.5	|	0.9772	|
|	270.00	|	2.982E+00	|	+6.0	|	-6.3	|	±3.3	|	±2.2	|	±2.5	|	0.9783	|
|	280.00	|	2.798E+00	|	+5.9	|	-6.3	|	±3.4	|	±2.2	|	±2.5	|	0.9795	|
|	290.00	|	2.643E+00	|	+5.9	|	-6.2	|	±3.4	|	±2.3	|	±2.6	|	0.9805	|
|	300.00	|	2.513E+00	|	+5.9	|	-6.1	|	±3.5	|	±2.3	|	±2.6	|	0.9813	|
|	310.00	|	2.410E+00	|	+5.9	|	-6.1	|	±3.5	|	±2.4	|	±2.6	|	0.9819	|
|	320.00	|	2.335E+00	|	+5.9	|	-6.0	|	±3.5	|	±2.4	|	±2.6	|	0.9820	|
|	330.00	|	2.292E+00	|	+5.9	|	-5.9	|	±3.6	|	±2.5	|	±2.6	|	0.9813	|
|	340.00	|	2.302E+00	|	+5.9	|	-5.9	|	±3.6	|	±2.5	|	±2.6	|	0.9779	|
|	350.00	|	2.444E+00	|	+5.9	|	-5.8	|	±3.7	|	±2.6	|	±2.6	|	0.9595	|
|	360.00	|	2.503E+00	|	+6.0	|	-5.7	|	±3.7	|	±2.6	|	±2.6	|	0.9608	|
|	370.00	|	2.470E+00	|	+6.0	|	-5.7	|	±3.8	|	±2.7	|	±2.7	|	0.9642	|
|	380.00	|	2.382E+00	|	+6.0	|	-5.6	|	±3.9	|	±2.8	|	±2.7	|	0.9677	|
|	390.00	|	2.261E+00	|	+6.0	|	-5.6	|	±3.9	|	±2.8	|	±2.7	|	0.9713	|
|	400.00	|	2.122E+00	|	+6.0	|	-5.5	|	±4.0	|	±2.9	|	±2.7	|	0.9741	|
|	410.00	|	1.976E+00	|	+6.0	|	-5.5	|	±4.0	|	±3.0	|	±2.7	|	0.9771	|
|	420.00	|	1.827E+00	|	+6.0	|	-5.5	|	±4.1	|	±3.0	|	±2.7	|	0.9802	|
|	430.00	|	1.682E+00	|	+6.0	|	-5.4	|	±4.1	|	±3.1	|	±2.7	|	0.9830	|
|	440.00	|	1.543E+00	|	+6.0	|	-5.4	|	±4.2	|	±3.2	|	±2.8	|	0.9853	|
|	450.00	|	1.412E+00	|	+6.0	|	-5.4	|	±4.3	|	±3.3	|	±2.8	|	0.9878	|
|	460.00	|	1.290E+00	|	+6.0	|	-5.4	|	±4.3	|	±3.3	|	±2.8	|	0.9900	|
|	470.00	|	1.177E+00	|	+6.0	|	-5.3	|	±4.4	|	±3.4	|	±2.8	|	0.9921	|
|	480.00	|	1.072E+00	|	+6.0	|	-5.3	|	±4.5	|	±3.5	|	±2.8	|	0.9940	|
|	490.00	|	9.756E-01	|	+6.0	|	-5.3	|	±4.5	|	±3.5	|	±2.8	|	0.9961	|
|	500.00	|	8.875E-01	|	+6.0	|	-5.3	|	±4.6	|	±3.6	|	±2.8	|	0.9981	|
|	550.00	|	5.523E-01	|	+6.1	|	-5.2	|	±5.0	|	±4.0	|	±2.9	|	1.0069	|
|	600.00	|	3.460E-01	|	+6.2	|	-5.2	|	±5.3	|	±4.4	|	±3.0	|	1.0152	|
|	650.00	|	2.195E-01	|	+6.2	|	-5.3	|	±5.7	|	±4.8	|	±3.1	|	1.0226	|
|	700.00	|	1.413E-01	|	+6.3	|	-5.3	|	±6.2	|	±5.2	|	±3.2	|	1.0301	|
|	750.00	|	9.229E-02	|	+6.4	|	-5.4	|	±6.6	|	±5.7	|	±3.3	|	1.0377	|
|	800.00	|	6.113E-02	|	+6.5	|	-5.5	|	±7.0	|	±6.1	|	±3.4	|	1.0454	|
|	850.00	|	4.107E-02	|	+6.6	|	-5.5	|	±7.5	|	±6.6	|	±3.5	|	1.0532	|
|	900.00	|	2.791E-02	|	+6.7	|	-5.6	|	±7.9	|	±7.0	|	±3.7	|	1.0610	|
|	950.00	|	1.922E-02	|	+6.8	|	-5.7	|	±8.4	|	±7.5	|	±3.8	|	1.0695	|
|	1000.00	|	1.335E-02	|	+7.0	|	-5.8	|	±8.9	|	±7.9	|	±3.9	|	1.0783	|
|	1050.00	|	9.376E-03	|	+7.1	|	-5.9	|	±9.3	|	±8.4	|	±4.1	|	1.0890	|
|	1100.00	|	6.648E-03	|	+7.2	|	-5.9	|	±9.9	|	±8.9	|	±4.2	|	1.1004	|
|	1150.00	|	4.749E-03	|	+7.3	|	-6.0	|	±10.4	|	±9.4	|	±4.3	|	1.1122	|
|	1200.00	|	3.423E-03	|	+7.4	|	-6.1	|	±10.9	|	±9.9	|	±4.5	|	1.1242	|
|	1250.00	|	2.484E-03	|	+7.5	|	-6.2	|	±11.5	|	±10.5	|	±4.7	|	1.1364	|
|	1300.00	|	1.815E-03	|	+7.6	|	-6.3	|	±12.0	|	±11.0	|	±4.8	|	1.1475	|
|	1350.00	|	1.334E-03	|	+7.7	|	-6.4	|	±12.6	|	±11.6	|	±5.0	|	1.1586	|
|	1400.00	|	9.864E-04	|	+7.8	|	-6.5	|	±13.2	|	±12.2	|	±5.2	|	1.1700	|
|	1450.00	|	7.333E-04	|	+7.9	|	-6.6	|	±13.8	|	±12.8	|	±5.3	|	1.1816	|
|	1500.00	|	5.478E-04	|	+8.0	|	-6.7	|	±14.5	|	±13.4	|	±5.5	|	1.1937	|
|	1550.00	|	4.112E-04	|	+8.1	|	-6.8	|	±15.1	|	±14.0	|	±5.7	|	1.2069	|
|	1600.00	|	3.100E-04	|	+8.1	|	-7.0	|	±15.8	|	±14.7	|	±5.9	|	1.2206	|
|	1650.00	|	2.346E-04	|	+8.1	|	-7.1	|	±16.5	|	±15.3	|	±6.1	|	1.2347	|
|	1700.00	|	1.782E-04	|	+8.2	|	-7.2	|	±17.3	|	±16.0	|	±6.4	|	1.2493	|
|	1750.00	|	1.359E-04	|	+8.2	|	-7.7	|	±9.0	|	±3.3	|	±8.4	|	1.2644	|
|	1800.00	|	1.039E-04	|	+8.2	|	-7.8	|	±10.6	|	±6.6	|	±8.3	|	1.2798	|
|	1850.00	|	7.973E-05	|	+8.3	|	-7.9	|	±12.7	|	±9.7	|	±8.2	|	1.2955	|
|	1900.00	|	6.133E-05	|	+8.3	|	-8.0	|	±14.9	|	±12.4	|	±8.2	|	1.3117	|
|	1950.00	|	4.730E-05	|	+8.4	|	-8.1	|	±17.1	|	±14.9	|	±8.3	|	1.3283	|
|	2000.00	|	3.656E-05	|	+8.4	|	-8.2	|	±19.1	|	±17.2	|	±8.3	|	1.3453	|
|	2050.00	|	2.832E-05	|	+8.4	|	-8.3	|	±21.0	|	±19.2	|	±8.4	|	1.3627	|
|	2100.00	|	2.199E-05	|	+8.5	|	-8.4	|	±22.7	|	±21.1	|	±8.6	|	1.3806	|
|	2150.00	|	1.711E-05	|	+8.5	|	-8.4	|	±24.4	|	±22.7	|	±8.8	|	1.3989	|
|	2200.00	|	1.333E-05	|	+8.6	|	-8.5	|	±25.9	|	±24.3	|	±9.0	|	1.4176	|
|	2250.00	|	1.042E-05	|	+8.6	|	-8.6	|	±27.3	|	±25.7	|	±9.2	|	1.4367	|
|	2300.00	|	8.135E-06	|	+8.6	|	-8.6	|	±28.6	|	±27.0	|	±9.5	|	1.4563	|
|	2350.00	|	6.371E-06	|	+8.7	|	-8.7	|	±29.8	|	±28.2	|	±9.8	|	1.4763	|
|	2400.00	|	4.991E-06	|	+8.7	|	-8.7	|	±31.1	|	±29.4	|	±10.1	|	1.4968	|
|	2450.00	|	3.916E-06	|	+8.8	|	-8.8	|	±32.3	|	±30.5	|	±10.5	|	1.5177	|
|	2500.00	|	3.075E-06	|	+8.8	|	-8.8	|	±33.5	|	±31.7	|	±10.8	|	1.5390	|
|	2550.00	|	2.412E-06	|	+8.8	|	-8.8	|	±34.7	|	±32.8	|	±11.2	|	0.0000	|
|	2600.00	|	1.897E-06	|	+8.9	|	-8.9	|	±35.9	|	±34.0	|	±11.6	|	0.0000	|
|	2650.00	|	1.496E-06	|	+8.9	|	-8.9	|	±37.3	|	±35.3	|	±12.0	|	0.0000	|
|	2700.00	|	1.181E-06	|	+9.0	|	-9.0	|	±38.7	|	±36.6	|	±12.4	|	0.0000	|
|	2750.00	|	9.285E-07	|	+9.0	|	-9.0	|	±40.2	|	±38.1	|	±12.9	|	0.0000	|
|	2800.00	|	7.321E-07	|	+9.0	|	-9.0	|	±41.8	|	±39.7	|	±13.3	|	0.0000	|
|	2850.00	|	5.788E-07	|	+9.1	|	-9.1	|	±43.6	|	±41.4	|	±13.7	|	0.0000	|
|	2900.00	|	4.549E-07	|	+9.1	|	-9.1	|	±45.6	|	±43.4	|	±14.1	|	0.0000	|
|	2950.00	|	3.594E-07	|	+9.2	|	-9.2	|	±47.8	|	±45.5	|	±14.5	|	0.0000	|
|	3000.00	|	2.823E-07	|	+9.2	|	-9.2	|	±50.1	|	±47.9	|	±15.0	|	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	|	4.452E+00	|	+0.9	|	-0.5	|	±2.0	|	±1.8	|	±0.7	|	|
|	15.00	|	4.224E+00	|	+0.8	|	-0.4	|	±2.0	|	±1.8	|	±0.7	|	|
|	20.00	|	3.994E+00	|	+0.8	|	-0.4	|	±2.0	|	±1.8	|	±0.7	|	|
|	25.00	|	3.768E+00	|	+0.7	|	-0.4	|	±2.0	|	±1.8	|	±0.7	|	|
|	30.00	|	3.555E+00	|	+0.6	|	-0.4	|	±1.9	|	±1.8	|	±0.6	|	|
|	35.00	|	3.350E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|	|
|	40.00	|	3.157E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|	|
|	45.00	|	2.977E+00	|	+0.6	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|	|
|	50.00	|	2.808E+00	|	+0.5	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|	|
|	55.00	|	2.651E+00	|	+0.5	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|	|
|	60.00	|	2.504E+00	|	+0.5	|	-0.3	|	±1.9	|	±1.8	|	±0.6	|	|
|	65.00	|	2.367E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|	|
|	70.00	|	2.240E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.8	|	±0.5	|	|
|	75.00	|	2.120E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	80.00	|	2.009E+00	|	+0.4	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	85.00	|	1.905E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	90.00	|	1.807E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	95.00	|	1.716E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	100.00	|	1.631E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	105.00	|	1.550E+00	|	+0.3	|	-0.2	|	±1.9	|	±1.9	|	±0.5	|	|
|	110.00	|	1.475E+00	|	+0.2	|	-0.2	|	±1.9	|	±1.9	|	±0.4	|	|
|	115.00	|	1.405E+00	|	+0.2	|	-0.2	|	±1.9	|	±1.9	|	±0.4	|	|
|	120.00	|	1.339E+00	|	+0.2	|	-0.2	|	±1.9	|	±1.9	|	±0.4	|	|
|	125.00	|	1.276E+00	|	+0.2	|	-0.2	|	±1.9	|	±1.9	|	±0.4	|	|
|	130.00	|	1.217E+00	|	+0.2	|	-0.2	|	±1.9	|	±1.9	|	±0.4	|	|
|	135.00	|	1.162E+00	|	+0.2	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|	|
|	140.00	|	1.110E+00	|	+0.2	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|	|
|	145.00	|	1.061E+00	|	+0.2	|	-0.1	|	±1.9	|	±1.9	|	±0.4	|	|
|	150.00	|	1.014E+00	|	+0.2	|	-0.1	|	±2.0	|	±1.9	|	±0.4	|	|
|	160.00	|	9.285E-01	|	+0.2	|	-0.1	|	±2.0	|	±1.9	|	±0.4	|	|
|	170.00	|	8.518E-01	|	+0.2	|	-0.1	|	±2.0	|	±1.9	|	±0.3	|	|
|	180.00	|	7.830E-01	|	+0.2	|	-0.1	|	±2.0	|	±1.9	|	±0.3	|	|
|	190.00	|	7.210E-01	|	+0.2	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|	|
|	200.00	|	6.650E-01	|	+0.2	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|	|
|	210.00	|	6.143E-01	|	+0.2	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|	|
|	220.00	|	5.684E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|	|
|	230.00	|	5.266E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|	|
|	240.00	|	4.886E-01	|	+0.3	|	-0.1	|	±2.0	|	±2.0	|	±0.3	|	|
|	250.00	|	4.539E-01	|	+0.3	|	-0.2	|	±2.0	|	±2.0	|	±0.2	|	|
|	260.00	|	4.222E-01	|	+0.3	|	-0.2	|	±2.1	|	±2.0	|	±0.2	|	|
|	270.00	|	3.932E-01	|	+0.3	|	-0.2	|	±2.1	|	±2.1	|	±0.2	|	|
|	280.00	|	3.666E-01	|	+0.3	|	-0.2	|	±2.1	|	±2.1	|	±0.2	|	|
|	290.00	|	3.421E-01	|	+0.3	|	-0.2	|	±2.1	|	±2.1	|	±0.2	|	|
|	300.00	|	3.196E-01	|	+0.3	|	-0.3	|	±2.1	|	±2.1	|	±0.2	|	|
|	310.00	|	2.989E-01	|	+0.3	|	-0.3	|	±2.1	|	±2.1	|	±0.2	|	|
|	320.00	|	2.798E-01	|	+0.3	|	-0.3	|	±2.1	|	±2.1	|	±0.2	|	|
|	330.00	|	2.621E-01	|	+0.3	|	-0.3	|	±2.2	|	±2.1	|	±0.2	|	|
|	340.00	|	2.457E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.2	|	|
|	350.00	|	2.306E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.1	|	|
|	360.00	|	2.166E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.1	|	|
|	370.00	|	2.035E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.1	|	|
|	380.00	|	1.914E-01	|	+0.3	|	-0.4	|	±2.2	|	±2.2	|	±0.1	|	|
|	390.00	|	1.802E-01	|	+0.3	|	-0.5	|	±2.2	|	±2.2	|	±0.1	|	|
|	400.00	|	1.697E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|	|
|	410.00	|	1.599E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|	|
|	420.00	|	1.508E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|	|
|	430.00	|	1.423E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|	|
|	440.00	|	1.343E-01	|	+0.3	|	-0.5	|	±2.3	|	±2.3	|	±0.1	|	|
|	450.00	|	1.269E-01	|	+0.3	|	-0.6	|	±2.3	|	±2.3	|	±0.1	|	|
|	460.00	|	1.199E-01	|	+0.3	|	-0.6	|	±2.4	|	±2.4	|	±0.1	|	|
|	470.00	|	1.134E-01	|	+0.3	|	-0.6	|	±2.4	|	±2.4	|	±0.1	|	|
|	480.00	|	1.073E-01	|	+0.3	|	-0.6	|	±2.4	|	±2.4	|	±0.0	|	|
|	490.00	|	1.015E-01	|	+0.3	|	-0.6	|	±2.4	|	±2.4	|	±0.0	|	|
|	500.00	|	9.616E-02	|	+0.3	|	-0.7	|	±2.4	|	±2.4	|	±0.0	|	|
|	550.00	|	7.372E-02	|	+0.3	|	-0.7	|	±2.5	|	±2.5	|	±0.0	|	|
|	600.00	|	5.706E-02	|	+0.3	|	-0.8	|	±2.6	|	±2.6	|	±0.0	|	|
|	650.00	|	4.453E-02	|	+0.3	|	-0.9	|	±2.7	|	±2.7	|	±0.1	|	|
|	700.00	|	3.501E-02	|	+0.3	|	-1.0	|	±2.8	|	±2.8	|	±0.1	|	|
|	750.00	|	2.769E-02	|	+0.4	|	-1.1	|	±2.9	|	±2.9	|	±0.1	|	|
|	800.00	|	2.203E-02	|	+0.4	|	-1.2	|	±3.0	|	±3.0	|	±0.1	|	|
|	850.00	|	1.761E-02	|	+0.5	|	-1.3	|	±3.1	|	±3.1	|	±0.1	|	|
|	900.00	|	1.414E-02	|	+0.5	|	-1.4	|	±3.2	|	±3.2	|	±0.2	|	|
|	950.00	|	1.139E-02	|	+0.5	|	-1.4	|	±3.3	|	±3.3	|	±0.2	|	|
|	1000.00	|	9.209E-03	|	+0.6	|	-1.5	|	±3.5	|	±3.5	|	±0.2	|	|
|	1050.00	|	7.468E-03	|	+0.6	|	-1.6	|	±3.6	|	±3.6	|	±0.2	|	|
|	1100.00	|	6.072E-03	|	+0.7	|	-1.7	|	±3.7	|	±3.7	|	±0.2	|	|
|	1150.00	|	4.949E-03	|	+0.7	|	-1.8	|	±3.9	|	±3.9	|	±0.2	|	|
|	1200.00	|	4.043E-03	|	+0.8	|	-1.9	|	±4.0	|	±4.0	|	±0.2	|	|
|	1250.00	|	3.308E-03	|	+0.8	|	-2.0	|	±4.2	|	±4.2	|	±0.2	|	|
|	1300.00	|	2.712E-03	|	+0.9	|	-2.1	|	±4.4	|	±4.4	|	±0.2	|	|
|	1350.00	|	2.226E-03	|	+0.9	|	-2.2	|	±4.5	|	±4.5	|	±0.2	|	|
|	1400.00	|	1.830E-03	|	+1.0	|	-2.3	|	±4.7	|	±4.7	|	±0.2	|	|
|	1450.00	|	1.506E-03	|	+1.0	|	-2.4	|	±4.9	|	±4.9	|	±0.2	|	|
|	1500.00	|	1.240E-03	|	+1.1	|	-2.5	|	±5.2	|	±5.1	|	±0.2	|	|
|	1550.00	|	1.023E-03	|	+1.1	|	-2.6	|	±5.4	|	±5.4	|	±0.2	|	|
|	1600.00	|	8.438E-04	|	+1.2	|	-2.7	|	±5.6	|	±5.6	|	±0.2	|	|
|	1650.00	|	6.967E-04	|	+1.2	|	-2.8	|	±5.9	|	±5.9	|	±0.1	|	|
|	1700.00	|	5.756E-04	|	+1.3	|	-2.9	|	±6.1	|	±6.1	|	±0.1	|	|
|	1750.00	|	4.757E-04	|	+1.4	|	-3.0	|	±6.4	|	±6.4	|	±0.1	|	|
|	1800.00	|	3.933E-04	|	+1.4	|	-3.1	|	±6.7	|	±6.7	|	±0.1	|	|
|	1850.00	|	3.253E-04	|	+1.5	|	-3.2	|	±7.0	|	±7.0	|	±0.1	|	|
|	1900.00	|	2.690E-04	|	+1.5	|	-3.3	|	±7.4	|	±7.4	|	±0.0	|	|
|	1950.00	|	2.226E-04	|	+1.6	|	-3.4	|	±7.7	|	±7.7	|	±0.0	|	|
|	2000.00	|	1.841E-04	|	+1.7	|	-3.5	|	±8.1	|	±8.1	|	±0.0	|	|
|	2050.00	|	1.523E-04	|	+1.7	|	-3.6	|	±8.5	|	±8.5	|	±0.0	|	|
|	2100.00	|	1.260E-04	|	+1.8	|	-3.7	|	±8.9	|	±8.9	|	±0.1	|	|
|	2150.00	|	1.042E-04	|	+1.9	|	-3.8	|	±9.3	|	±9.3	|	±0.1	|	|
|	2200.00	|	8.614E-05	|	+2.0	|	-3.9	|	±9.7	|	±9.7	|	±0.1	|	|
|	2250.00	|	7.121E-05	|	+2.0	|	-4.1	|	±10.2	|	±10.2	|	±0.2	|	|
|	2300.00	|	5.884E-05	|	+2.1	|	-4.2	|	±10.7	|	±10.7	|	±0.2	|	|
|	2350.00	|	4.860E-05	|	+2.2	|	-4.3	|	±11.2	|	±11.2	|	±0.3	|	|
|	2400.00	|	4.012E-05	|	+2.3	|	-4.4	|	±11.7	|	±11.7	|	±0.3	|	|
|	2450.00	|	3.311E-05	|	+2.4	|	-4.5	|	±12.2	|	±12.2	|	±0.4	|	|
|	2500.00	|	2.730E-05	|	+2.4	|	-4.7	|	±12.8	|	±12.8	|	±0.4	|	|
|	2550.00	|	2.250E-05	|	+2.5	|	-4.8	|	±13.4	|	±13.4	|	±0.4	|	|
|	2600.00	|	1.854E-05	|	+2.6	|	-4.9	|	±14.0	|	±14.0	|	±0.5	|	|
|	2650.00	|	1.526E-05	|	+2.7	|	-5.0	|	±14.7	|	±14.7	|	±0.6	|	|
|	2700.00	|	1.255E-05	|	+2.8	|	-5.2	|	±15.4	|	±15.3	|	±0.6	|	|
|	2750.00	|	1.032E-05	|	+2.9	|	-5.3	|	±16.0	|	±16.0	|	±0.7	|	|
|	2800.00	|	8.471E-06	|	+3.0	|	-5.4	|	±16.8	|	±16.8	|	±0.7	|	|
|	2850.00	|	6.950E-06	|	+3.0	|	-5.5	|	±17.5	|	±17.5	|	±0.8	|	|
|	2900.00	|	5.698E-06	|	+3.2	|	-5.7	|	±18.3	|	±18.3	|	±0.8	|	|
|	2950.00	|	4.666E-06	|	+3.3	|	-5.8	|	±19.1	|	±19.1	|	±0.9	|	|
|	3000.00	|	3.818E-06	|	+3.4	|	-5.9	|	±20.0	|	±19.9	|	±1.0	|	|
</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	|	1.191E+02	|	+0.9	|	-1.2	|	±2.0	|		|		|		|	7.139E+01	|	4.775E+01	|
|	15.00	|	7.322E+01	|	+0.8	|	-1.1	|	±2.0	|		|		|		|	4.406E+01	|	2.916E+01	|
|	20.00	|	4.865E+01	|	+0.4	|	-1.0	|	±2.0	|		|		|		|	2.940E+01	|	1.925E+01	|
|	25.00	|	3.394E+01	|	+0.5	|	-1.0	|	±2.0	|		|		|		|	2.057E+01	|	1.337E+01	|
|	30.00	|	2.451E+01	|	+0.6	|	-0.8	|	±2.0	|		|		|		|	1.489E+01	|	9.618E+00	|
|	35.00	|	1.822E+01	|	+0.5	|	-0.7	|	±2.0	|		|		|		|	1.112E+01	|	7.101E+00	|
|	40.00	|	1.383E+01	|	+0.5	|	-0.8	|	±2.0	|		|		|		|	8.473E+00	|	5.357E+00	|
|	45.00	|	1.069E+01	|	+0.4	|	-0.8	|	±2.0	|		|		|		|	6.569E+00	|	4.121E+00	|
|	50.00	|	8.385E+00	|	+0.5	|	-0.6	|	±2.0	|		|		|		|	5.164E+00	|	3.221E+00	|
|	55.00	|	6.671E+00	|	+0.5	|	-0.7	|	±2.0	|		|		|		|	4.120E+00	|	2.551E+00	|
|	60.00	|	5.366E+00	|	+0.5	|	-0.7	|	±2.0	|		|		|		|	3.327E+00	|	2.039E+00	|
|	65.00	|	4.364E+00	|	+0.4	|	-0.8	|	±2.0	|		|		|		|	2.713E+00	|	1.651E+00	|
|	70.00	|	3.581E+00	|	+0.4	|	-0.8	|	±2.0	|		|		|		|	2.232E+00	|	1.349E+00	|
|	75.00	|	2.962E+00	|	+0.4	|	-0.8	|	±2.0	|		|		|		|	1.851E+00	|	1.111E+00	|
|	80.00	|	2.468E+00	|	+0.5	|	-0.7	|	±2.0	|		|		|		|	1.546E+00	|	9.215E-01	|
|	85.00	|	2.071E+00	|	+0.5	|	-0.7	|	±2.1	|		|		|		|	1.301E+00	|	7.701E-01	|
|	90.00	|	1.751E+00	|	+0.5	|	-0.8	|	±2.1	|		|		|		|	1.103E+00	|	6.476E-01	|
|	95.00	|	1.487E+00	|	+0.5	|	-0.8	|	±2.1	|		|		|		|	9.391E-01	|	5.480E-01	|
|	100.00	|	1.270E+00	|	+0.6	|	-0.8	|	±2.1	|		|		|		|	8.040E-01	|	4.658E-01	|
|	105.00	|	1.090E+00	|	+0.6	|	-0.8	|	±2.1	|		|		|		|	6.923E-01	|	3.981E-01	|
|	110.00	|	9.408E-01	|	+0.5	|	-0.9	|	±2.1	|		|		|		|	5.987E-01	|	3.421E-01	|
|	115.00	|	8.146E-01	|	+0.6	|	-0.8	|	±2.1	|		|		|		|	5.196E-01	|	2.950E-01	|
|	120.00	|	7.089E-01	|	+0.6	|	-0.9	|	±2.0	|		|		|		|	4.533E-01	|	2.556E-01	|
|	125.00	|	6.191E-01	|	+0.7	|	-0.9	|	±2.1	|		|		|		|	3.967E-01	|	2.224E-01	|
|	130.00	|	5.427E-01	|	+0.6	|	-0.9	|	±2.1	|		|		|		|	3.486E-01	|	1.941E-01	|
|	135.00	|	4.773E-01	|	+0.7	|	-0.9	|	±2.2	|		|		|		|	3.072E-01	|	1.701E-01	|
|	140.00	|	4.212E-01	|	+0.7	|	-0.9	|	±2.2	|		|		|		|	2.717E-01	|	1.495E-01	|
|	145.00	|	3.727E-01	|	+0.8	|	-0.9	|	±2.2	|		|		|		|	2.410E-01	|	1.317E-01	|
|	150.00	|	3.310E-01	|	+0.7	|	-0.9	|	±2.2	|		|		|		|	2.145E-01	|	1.165E-01	|
|	160.00	|	2.629E-01	|	+0.7	|	-1.0	|	±2.3	|		|		|		|	1.711E-01	|	9.176E-02	|
|	170.00	|	2.109E-01	|	+0.9	|	-1.0	|	±2.3	|		|		|		|	1.378E-01	|	7.308E-02	|
|	180.00	|	1.707E-01	|	+0.9	|	-0.9	|	±2.4	|		|		|		|	1.120E-01	|	5.872E-02	|
|	190.00	|	1.394E-01	|	+0.9	|	-1.0	|	±2.4	|		|		|		|	9.185E-02	|	4.759E-02	|
|	200.00	|	1.148E-01	|	+0.9	|	-1.0	|	±2.5	|		|		|		|	7.589E-02	|	3.887E-02	|
|	210.00	|	9.509E-02	|	+0.9	|	-1.1	|	±2.5	|		|		|		|	6.312E-02	|	3.197E-02	|
|	220.00	|	7.928E-02	|	+1.0	|	-1.1	|	±2.6	|		|		|		|	5.282E-02	|	2.646E-02	|
|	230.00	|	6.652E-02	|	+1.0	|	-1.1	|	±2.6	|		|		|		|	4.447E-02	|	2.205E-02	|
|	240.00	|	5.610E-02	|	+1.1	|	-1.1	|	±2.6	|		|		|		|	3.764E-02	|	1.846E-02	|
|	250.00	|	4.758E-02	|	+1.1	|	-1.2	|	±2.7	|		|		|		|	3.203E-02	|	1.555E-02	|
|	260.00	|	4.053E-02	|	+1.1	|	-1.2	|	±2.7	|		|		|		|	2.737E-02	|	1.316E-02	|
|	270.00	|	3.470E-02	|	+1.1	|	-1.3	|	±2.7	|		|		|		|	2.351E-02	|	1.119E-02	|
|	280.00	|	2.982E-02	|	+1.1	|	-1.3	|	±2.8	|		|		|		|	2.027E-02	|	9.551E-03	|
|	290.00	|	2.574E-02	|	+1.2	|	-1.4	|	±2.8	|		|		|		|	1.755E-02	|	8.187E-03	|
|	300.00	|	2.228E-02	|	+1.2	|	-1.5	|	±2.9	|		|		|		|	1.524E-02	|	7.044E-03	|
|	310.00	|	1.936E-02	|	+1.2	|	-1.5	|	±3.0	|		|		|		|	1.328E-02	|	6.084E-03	|
|	320.00	|	1.688E-02	|	+1.2	|	-1.5	|	±3.1	|		|		|		|	1.161E-02	|	5.271E-03	|
|	330.00	|	1.476E-02	|	+1.3	|	-1.5	|	±3.2	|		|		|		|	1.018E-02	|	4.581E-03	|
|	340.00	|	1.295E-02	|	+1.3	|	-1.6	|	±3.3	|		|		|		|	8.959E-03	|	3.994E-03	|
|	350.00	|	1.139E-02	|	+1.3	|	-1.6	|	±3.4	|		|		|		|	7.900E-03	|	3.492E-03	|
|	360.00	|	1.005E-02	|	+1.3	|	-1.7	|	±3.4	|		|		|		|	6.987E-03	|	3.062E-03	|
|	370.00	|	8.882E-03	|	+1.4	|	-1.7	|	±3.5	|		|		|		|	6.191E-03	|	2.691E-03	|
|	380.00	|	7.871E-03	|	+1.4	|	-1.7	|	±3.5	|		|		|		|	5.500E-03	|	2.371E-03	|
|	390.00	|	6.991E-03	|	+1.4	|	-1.7	|	±3.6	|		|		|		|	4.897E-03	|	2.094E-03	|
|	400.00	|	6.224E-03	|	+1.4	|	-1.8	|	±3.7	|		|		|		|	4.370E-03	|	1.854E-03	|
|	410.00	|	5.550E-03	|	+1.4	|	-1.8	|	±3.8	|		|		|		|	3.906E-03	|	1.644E-03	|
|	420.00	|	4.959E-03	|	+1.4	|	-1.8	|	±3.9	|		|		|		|	3.497E-03	|	1.462E-03	|
|	430.00	|	4.440E-03	|	+1.5	|	-1.9	|	±4.0	|		|		|		|	3.138E-03	|	1.302E-03	|
|	440.00	|	3.983E-03	|	+1.5	|	-1.9	|	±4.1	|		|		|		|	2.821E-03	|	1.162E-03	|
|	450.00	|	3.577E-03	|	+1.5	|	-1.9	|	±4.2	|		|		|		|	2.539E-03	|	1.038E-03	|
|	460.00	|	3.219E-03	|	+1.5	|	-2.0	|	±4.3	|		|		|		|	2.289E-03	|	9.296E-04	|
|	470.00	|	2.900E-03	|	+1.6	|	-2.0	|	±4.4	|		|		|		|	2.067E-03	|	8.333E-04	|
|	480.00	|	2.618E-03	|	+1.6	|	-2.1	|	±4.5	|		|		|		|	1.869E-03	|	7.486E-04	|
|	490.00	|	2.365E-03	|	+1.6	|	-2.1	|	±4.6	|		|		|		|	1.692E-03	|	6.732E-04	|
|	500.00	|	2.140E-03	|	+1.6	|	-2.1	|	±4.7	|		|		|		|	1.533E-03	|	6.065E-04	|
|	550.00	|	1.323E-03	|	+1.7	|	-2.2	|	±5.3	|		|		|		|	9.561E-04	|	3.670E-04	|
|	600.00	|	8.402E-04	|	+1.8	|	-2.4	|	±5.9	|		|		|		|	6.116E-04	|	2.286E-04	|
|	650.00	|	5.455E-04	|	+1.8	|	-2.5	|	±6.5	|		|		|		|	3.996E-04	|	1.459E-04	|
|	700.00	|	3.609E-04	|	+1.9	|	-2.6	|	±7.0	|		|		|		|	2.658E-04	|	9.508E-05	|
|	750.00	|	2.425E-04	|	+2.0	|	-2.8	|	±7.6	|		|		|		|	1.794E-04	|	6.307E-05	|
|	800.00	|	1.652E-04	|	+2.1	|	-2.9	|	±8.2	|		|		|		|	1.227E-04	|	4.250E-05	|
|	850.00	|	1.138E-04	|	+2.2	|	-3.0	|	±8.7	|		|		|		|	8.477E-05	|	2.903E-05	|
|	900.00	|	7.923E-05	|	+2.2	|	-3.1	|	±9.3	|		|		|		|	5.915E-05	|	2.008E-05	|
|	950.00	|	5.563E-05	|	+2.3	|	-3.3	|	±9.9	|		|		|		|	4.160E-05	|	1.403E-05	|
|	1000.00	|	3.936E-05	|	+2.3	|	-3.4	|	±10.5	|		|		|		|	2.946E-05	|	9.901E-06	|
|	1050.00	|	2.804E-05	|	+2.5	|	-3.5	|	±17.6	|		|		|		|	2.099E-05	|	7.047E-06	|
|	1100.00	|	2.009E-05	|	+2.6	|	-3.6	|	±24.7	|		|		|		|	1.504E-05	|	5.054E-06	|
|	1150.00	|	1.447E-05	|	+2.6	|	-3.7	|	±31.8	|		|		|		|	1.082E-05	|	3.650E-06	|
|	1200.00	|	1.046E-05	|	+2.7	|	-3.8	|	±38.8	|		|		|		|	7.810E-06	|	2.653E-06	|
|	1250.00	|	7.598E-06	|	+2.8	|	-3.9	|	±45.8	|		|		|		|	5.659E-06	|	1.939E-06	|
|	1300.00	|	5.535E-06	|	+2.9	|	-4.0	|	±52.7	|		|		|		|	4.110E-06	|	1.425E-06	|
|	1350.00	|	4.044E-06	|	+3.0	|	-4.2	|	±59.6	|		|		|		|	2.992E-06	|	1.052E-06	|
|	1400.00	|	2.962E-06	|	+3.0	|	-4.3	|	±66.4	|		|		|		|	2.182E-06	|	7.800E-07	|
|	1450.00	|	2.174E-06	|	+3.1	|	-4.5	|	±73.1	|		|		|		|	1.593E-06	|	5.808E-07	|
|	1500.00	|	1.598E-06	|	+3.2	|	-4.6	|	±79.4	|		|		|		|	1.164E-06	|	4.340E-07	|
|	1550.00	|	1.177E-06	|	+3.3	|	-4.7	|	±86.5	|		|		|		|	8.512E-07	|	3.254E-07	|
|	1600.00	|	8.670E-07	|	+3.5	|	-4.8	|	±92.8	|		|		|		|	6.222E-07	|	2.448E-07	|
|	1650.00	|	6.393E-07	|	+3.6	|	-5.0	|	±98.9	|		|		|		|	4.546E-07	|	1.847E-07	|
|	1700.00	|	4.715E-07	|	+3.7	|	-5.1	|	±104.8	|		|		|		|	3.318E-07	|	1.397E-07	|
|	1750.00	|	3.477E-07	|	+3.8	|	-5.3	|	±110.5	|		|		|		|	2.418E-07	|	1.059E-07	|
|	1800.00	|	2.564E-07	|	+3.9	|	-5.4	|	±115.8	|		|		|		|	1.759E-07	|	8.052E-08	|
|	1850.00	|	1.890E-07	|	+4.1	|	-5.5	|	±120.9	|		|		|		|	1.276E-07	|	6.135E-08	|
|	1900.00	|	1.392E-07	|	+4.2	|	-5.7	|	±125.6	|		|		|		|	9.233E-08	|	4.683E-08	|
|	1950.00	|	1.023E-07	|	+4.3	|	-5.8	|	±129.9	|		|		|		|	6.652E-08	|	3.582E-08	|
|	2000.00	|	7.514E-08	|	+4.5	|	-6.0	|	±133.8	|		|		|		|	4.769E-08	|	2.745E-08	|
</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	|	5.145E+01	|	+0.8	|	-0.9	|	±2.1	|		|		|		|		|
|	15.00	|	3.242E+01	|	+0.7	|	-0.9	|	±2.1	|		|		|		|		|
|	20.00	|	2.200E+01	|	+0.4	|	-0.9	|	±2.1	|		|		|		|		|
|	25.00	|	1.564E+01	|	+0.4	|	-0.9	|	±2.1	|		|		|		|		|
|	30.00	|	1.150E+01	|	+0.3	|	-0.7	|	±2.1	|		|		|		|		|
|	35.00	|	8.665E+00	|	+0.4	|	-0.8	|	±2.1	|		|		|		|		|
|	40.00	|	6.674E+00	|	+0.5	|	-0.8	|	±2.1	|		|		|		|		|
|	45.00	|	5.225E+00	|	+0.6	|	-0.8	|	±2.1	|		|		|		|		|
|	50.00	|	4.153E+00	|	+0.7	|	-0.9	|	±2.0	|		|		|		|		|
|	55.00	|	3.340E+00	|	+0.7	|	-0.9	|	±2.0	|		|		|		|		|
|	60.00	|	2.716E+00	|	+0.8	|	-1.0	|	±2.0	|		|		|		|		|
|	65.00	|	2.230E+00	|	+0.9	|	-1.0	|	±2.0	|		|		|		|		|
|	70.00	|	1.849E+00	|	+1.1	|	-1.2	|	±1.9	|		|		|		|		|
|	75.00	|	1.544E+00	|	+1.2	|	-1.2	|	±1.9	|		|		|		|		|
|	80.00	|	1.299E+00	|	+1.3	|	-1.4	|	±1.9	|		|		|		|		|
|	85.00	|	1.100E+00	|	+1.5	|	-1.3	|	±1.9	|		|		|		|		|
|	90.00	|	9.384E-01	|	+1.6	|	-1.4	|	±1.9	|		|		|		|		|
|	95.00	|	8.038E-01	|	+1.8	|	-1.5	|	±1.8	|		|		|		|		|
|	100.00	|	6.925E-01	|	+1.9	|	-1.7	|	±1.8	|		|		|		|		|
|	105.00	|	5.995E-01	|	+2.0	|	-1.7	|	±1.8	|		|		|		|		|
|	110.00	|	5.216E-01	|	+2.2	|	-1.8	|	±1.8	|		|		|		|		|
|	115.00	|	4.556E-01	|	+2.4	|	-2.0	|	±1.8	|		|		|		|		|
|	120.00	|	3.992E-01	|	+2.6	|	-2.0	|	±1.7	|		|		|		|		|
|	125.00	|	3.514E-01	|	+2.6	|	-2.1	|	±1.7	|		|		|		|		|
|	130.00	|	3.103E-01	|	+2.8	|	-2.3	|	±1.7	|		|		|		|		|
|	135.00	|	2.750E-01	|	+2.9	|	-2.4	|	±1.7	|		|		|		|		|
|	140.00	|	2.442E-01	|	+3.1	|	-2.5	|	±1.8	|		|		|		|		|
|	145.00	|	2.177E-01	|	+3.2	|	-2.7	|	±1.8	|		|		|		|		|
|	150.00	|	1.942E-01	|	+3.4	|	-2.7	|	±1.8	|		|		|		|		|
|	160.00	|	1.561E-01	|	+3.6	|	-3.0	|	±1.9	|		|		|		|		|
|	170.00	|	1.265E-01	|	+3.7	|	-3.2	|	±1.9	|		|		|		|		|
|	180.00	|	1.031E-01	|	+3.9	|	-3.4	|	±1.9	|		|		|		|		|
|	190.00	|	8.462E-02	|	+4.0	|	-3.5	|	±2.0	|		|		|		|		|
|	200.00	|	6.979E-02	|	+4.0	|	-3.5	|	±2.0	|		|		|		|		|
|	210.00	|	5.780E-02	|	+4.1	|	-3.5	|	±2.1	|		|		|		|		|
|	220.00	|	4.809E-02	|	+4.1	|	-3.5	|	±2.1	|		|		|		|		|
|	230.00	|	4.015E-02	|	+4.0	|	-3.4	|	±2.2	|		|		|		|		|
|	240.00	|	3.365E-02	|	+3.8	|	-3.3	|	±2.2	|		|		|		|		|
|	250.00	|	2.831E-02	|	+3.6	|	-3.3	|	±2.3	|		|		|		|		|
|	260.00	|	2.392E-02	|	+3.4	|	-3.2	|	±2.3	|		|		|		|		|
|	270.00	|	2.030E-02	|	+3.3	|	-3.0	|	±2.4	|		|		|		|		|
|	280.00	|	1.731E-02	|	+3.1	|	-2.9	|	±2.4	|		|		|		|		|
|	290.00	|	1.482E-02	|	+2.9	|	-2.8	|	±2.4	|		|		|		|		|
|	300.00	|	1.274E-02	|	+2.8	|	-2.7	|	±2.5	|		|		|		|		|
|	310.00	|	1.100E-02	|	+2.7	|	-2.6	|	±2.5	|		|		|		|		|
|	320.00	|	9.530E-03	|	+2.5	|	-2.5	|	±2.6	|		|		|		|		|
|	330.00	|	8.289E-03	|	+2.4	|	-2.5	|	±2.6	|		|		|		|		|
|	340.00	|	7.237E-03	|	+2.4	|	-2.4	|	±2.7	|		|		|		|		|
|	350.00	|	6.347E-03	|	+2.3	|	-2.4	|	±2.7	|		|		|		|		|
|	360.00	|	5.586E-03	|	+2.4	|	-2.4	|	±2.8	|		|		|		|		|
|	370.00	|	4.934E-03	|	+2.4	|	-2.5	|	±2.8	|		|		|		|		|
|	380.00	|	4.370E-03	|	+2.4	|	-2.5	|	±2.9	|		|		|		|		|
|	390.00	|	3.880E-03	|	+2.5	|	-2.6	|	±2.9	|		|		|		|		|
|	400.00	|	3.454E-03	|	+2.6	|	-2.7	|	±3.0	|		|		|		|		|
|	410.00	|	3.082E-03	|	+2.6	|	-2.7	|	±3.0	|		|		|		|		|
|	420.00	|	2.756E-03	|	+2.8	|	-2.8	|	±3.0	|		|		|		|		|
|	430.00	|	2.470E-03	|	+2.8	|	-2.9	|	±3.1	|		|		|		|		|
|	440.00	|	2.218E-03	|	+2.9	|	-3.0	|	±3.1	|		|		|		|		|
|	450.00	|	1.995E-03	|	+3.0	|	-3.1	|	±3.1	|		|		|		|		|
|	460.00	|	1.798E-03	|	+3.1	|	-3.2	|	±3.2	|		|		|		|		|
|	470.00	|	1.623E-03	|	+3.3	|	-3.3	|	±3.2	|		|		|		|		|
|	480.00	|	1.467E-03	|	+3.4	|	-3.4	|	±3.3	|		|		|		|		|
|	490.00	|	1.329E-03	|	+3.5	|	-3.5	|	±3.3	|		|		|		|		|
|	500.00	|	1.205E-03	|	+3.6	|	-3.6	|	±3.3	|		|		|		|		|
|	550.00	|	7.547E-04	|	+4.3	|	-4.1	|	±3.6	|		|		|		|		|
|	600.00	|	4.868E-04	|	+5.1	|	-4.8	|	±3.8	|		|		|		|		|
|	650.00	|	3.218E-04	|	+5.8	|	-5.4	|	±4.1	|		|		|		|		|
|	700.00	|	2.171E-04	|	+6.6	|	-6.1	|	±4.4	|		|		|		|		|
|	750.00	|	1.490E-04	|	+7.4	|	-6.7	|	±4.6	|		|		|		|		|
|	800.00	|	1.038E-04	|	+8.2	|	-7.4	|	±4.9	|		|		|		|		|
|	850.00	|	7.328E-05	|	+9.0	|	-8.0	|	±5.1	|		|		|		|		|
|	900.00	|	5.229E-05	|	+9.9	|	-8.6	|	±5.4	|		|		|		|		|
|	950.00	|	3.771E-05	|	+10.6	|	-9.3	|	±5.7	|		|		|		|		|
|	1000.00	|	2.741E-05	|	+11.4	|	-9.9	|	±5.9	|		|		|		|		|
|	1050.00	|	2.009E-05	|	+12.2	|	-10.5	|	±6.5	|		|		|		|		|
|	1100.00	|	1.482E-05	|	+13.0	|	-11.1	|	±7.1	|		|		|		|		|
|	1150.00	|	1.101E-05	|	+13.8	|	-11.7	|	±7.6	|		|		|		|		|
|	1200.00	|	8.219E-06	|	+14.5	|	-12.3	|	±8.2	|		|		|		|		|
|	1250.00	|	6.167E-06	|	+15.3	|	-12.8	|	±8.7	|		|		|		|		|
|	1300.00	|	4.646E-06	|	+16.1	|	-13.3	|	±9.3	|		|		|		|		|
|	1350.00	|	3.516E-06	|	+16.8	|	-13.9	|	±9.9	|		|		|		|		|
|	1400.00	|	2.671E-06	|	+17.7	|	-14.4	|	±10.4	|		|		|		|		|
|	1450.00	|	2.036E-06	|	+18.5	|	-15.0	|	±11.0	|		|		|		|		|
|	1500.00	|	1.556E-06	|	+19.1	|	-15.5	|	±11.6	|		|		|		|		|
|	1550.00	|	1.193E-06	|	+19.9	|	-16.0	|	±12.1	|		|		|		|		|
|	1600.00	|	9.170E-07	|	+20.6	|	-16.5	|	±12.7	|		|		|		|		|
|	1650.00	|	7.066E-07	|	+21.3	|	-17.0	|	±13.2	|		|		|		|		|
|	1700.00	|	5.456E-07	|	+21.9	|	-17.5	|	±13.8	|		|		|		|		|
|	1750.00	|	4.220E-07	|	+22.8	|	-18.0	|	±14.4	|		|		|		|		|
|	1800.00	|	3.269E-07	|	+23.5	|	-18.4	|	±14.9	|		|		|		|		|
|	1850.00	|	2.537E-07	|	+24.3	|	-18.8	|	±15.5	|		|		|		|		|
|	1900.00	|	1.972E-07	|	+25.0	|	-19.3	|	±16.1	|		|		|		|		|
|	1950.00	|	1.534E-07	|	+25.6	|	-19.8	|	±16.6	|		|		|		|		|
|	2000.00	|	1.195E-07	|	+26.5	|	-20.3	|	±17.8	|		|		|		|		|
</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	|	5.391E+01	|	+82.2	|	-54.9	|
|	15.00	|	2.900E+01	|	+58.5	|	-47.4	|
|	20.00	|	1.807E+01	|	+49.3	|	-42.5	|
|	25.00	|	1.189E+01	|	+42.7	|	-38.7	|
|	30.00	|	8.222E+00	|	+38.5	|	-35.9	|
|	35.00	|	5.786E+00	|	+35.2	|	-33.5	|
|	40.00	|	4.217E+00	|	+33.5	|	-36.1	|
|	45.00	|	3.160E+00	|	+32.4	|	-37.3	|
|	50.00	|	2.422E+00	|	+30.6	|	-36.8	|
|	55.00	|	1.894E+00	|	+29.4	|	-35.7	|
|	60.00	|	1.503E+00	|	+28.0	|	-34.3	|
|	65.00	|	1.210E+00	|	+27.4	|	-32.9	|
|	70.00	|	9.787E-01	|	+26.4	|	-31.6	|
|	75.00	|	8.024E-01	|	+25.8	|	-30.3	|
|	80.00	|	6.602E-01	|	+24.8	|	-29.1	|
|	85.00	|	5.501E-01	|	+24.3	|	-28.0	|
|	90.00	|	4.604E-01	|	+23.9	|	-27.0	|
|	95.00	|	3.876E-01	|	+23.1	|	-26.0	|
|	100.00	|	3.289E-01	|	+22.7	|	-25.3	|
|	105.00	|	2.805E-01	|	+22.1	|	-24.4	|
|	110.00	|	2.402E-01	|	+21.8	|	-23.8	|
|	115.00	|	2.069E-01	|	+21.5	|	-23.3	|
|	120.00	|	1.782E-01	|	+21.0	|	-22.8	|
|	125.00	|	1.552E-01	|	+20.7	|	-22.4	|
|	130.00	|	1.351E-01	|	+20.3	|	-22.1	|
|	135.00	|	1.183E-01	|	+20.1	|	-21.7	|
|	140.00	|	1.038E-01	|	+19.8	|	-21.4	|
|	145.00	|	9.117E-02	|	+19.4	|	-21.1	|
|	150.00	|	8.073E-02	|	+19.3	|	-20.8	|
|	160.00	|	6.348E-02	|	+19.0	|	-20.3	|
|	170.00	|	5.043E-02	|	+18.6	|	-19.9	|
|	180.00	|	4.052E-02	|	+18.3	|	-19.6	|
|	190.00	|	3.286E-02	|	+18.0	|	-19.3	|
|	200.00	|	2.678E-02	|	+17.8	|	-19.0	|
|	210.00	|	2.202E-02	|	+17.6	|	-18.7	|
|	220.00	|	1.821E-02	|	+17.6	|	-18.5	|
|	230.00	|	1.515E-02	|	+17.6	|	-18.3	|
|	240.00	|	1.268E-02	|	+17.4	|	-18.0	|
|	250.00	|	1.067E-02	|	+17.3	|	-17.9	|
|	260.00	|	9.011E-03	|	+17.5	|	-17.8	|
|	270.00	|	7.650E-03	|	+17.3	|	-17.7	|
|	280.00	|	6.537E-03	|	+17.2	|	-17.6	|
|	290.00	|	5.581E-03	|	+17.1	|	-17.5	|
|	300.00	|	4.802E-03	|	+17.2	|	-17.4	|
|	310.00	|	4.146E-03	|	+17.4	|	-17.4	|
|	320.00	|	3.588E-03	|	+17.4	|	-17.4	|
|	330.00	|	3.115E-03	|	+17.5	|	-17.4	|
|	340.00	|	2.712E-03	|	+17.6	|	-17.4	|
|	350.00	|	2.370E-03	|	+17.7	|	-17.4	|
|	360.00	|	2.077E-03	|	+17.9	|	-17.4	|
|	370.00	|	1.822E-03	|	+18.0	|	-17.3	|
|	380.00	|	1.602E-03	|	+18.1	|	-17.3	|
|	390.00	|	1.413E-03	|	+18.3	|	-17.4	|
|	400.00	|	1.249E-03	|	+18.4	|	-17.4	|
|	410.00	|	1.105E-03	|	+18.5	|	-17.3	|
|	420.00	|	9.824E-04	|	+18.7	|	-17.3	|
|	430.00	|	8.738E-04	|	+18.9	|	-17.4	|
|	440.00	|	7.790E-04	|	+19.0	|	-17.5	|
|	450.00	|	6.948E-04	|	+19.2	|	-17.5	|
|	460.00	|	6.218E-04	|	+19.3	|	-17.7	|
|	470.00	|	5.567E-04	|	+19.4	|	-17.7	|
|	480.00	|	4.992E-04	|	+19.5	|	-17.7	|
|	490.00	|	4.490E-04	|	+19.9	|	-17.9	|
|	500.00	|	4.039E-04	|	+20.0	|	-17.9	|
|	550.00	|	2.427E-04	|	+20.7	|	-18.5	|
|	600.00	|	1.505E-04	|	+21.0	|	-19.2	|
|	650.00	|	9.547E-05	|	+21.2	|	-20.3	|
|	700.00	|	6.203E-05	|	+21.7	|	-21.4	|
|	750.00	|	4.109E-05	|	+22.4	|	-22.9	|
|	800.00	|	2.764E-05	|	+23.1	|	-24.4	|
|	850.00	|	1.889E-05	|	+24.4	|	-25.9	|
|	900.00	|	1.307E-05	|	+26.0	|	-27.0	|
|	950.00	|	9.154E-06	|	+27.7	|	-28.1	|
|	1000.00	|	6.472E-06	|	+29.2	|	-29.3	|
|	1050.00	|	4.623E-06	|	+30.6	|	-30.5	|
|	1100.00	|	3.332E-06	|	+31.9	|	-31.8	|
|	1150.00	|	2.420E-06	|	+33.2	|	-33.1	|
|	1200.00	|	1.771E-06	|	+34.5	|	-35.2	|
|	1250.00	|	1.304E-06	|	+36.2	|	-37.2	|
|	1300.00	|	9.644E-07	|	+38.1	|	-39.3	|
|	1350.00	|	7.191E-07	|	+40.0	|	-41.5	|
|	1400.00	|	5.379E-07	|	+42.2	|	-43.7	|
|	1450.00	|	4.047E-07	|	+44.1	|	-45.8	|
|	1500.00	|	2.995E-07	|	+46.8	|	-48.1	|
|	1550.00	|	2.317E-07	|	+49.1	|	-49.4	|
|	1600.00	|	1.779E-07	|	+51.6	|	-51.0	|
|	1650.00	|	1.346E-07	|	+54.6	|	-53.1	|
|	1700.00	|	1.043E-07	|	+57.3	|	-54.7	|
|	1750.00	|	7.913E-08	|	+60.3	|	-56.8	|
|	1800.00	|	6.096E-08	|	+60.9	|	-58.5	|
|	1850.00	|	4.702E-08	|	+61.4	|	-60.3	|
|	1900.00	|	3.635E-08	|	+61.8	|	-63.2	|
|	1950.00	|	2.820E-08	|	+63.8	|	-65.4	|
|	2000.00	|	2.190E-08	|	+67.2	|	-67.8	|
|	2050.00	|	1.703E-08	|	+70.7	|	-70.5	|
|	2100.00	|	1.311E-08	|	+74.9	|	-73.7	|
|	2150.00	|	1.035E-08	|	+78.3	|	-75.8	|
|	2200.00	|	8.084E-09	|	+82.4	|	-78.7	|
|	2250.00	|	6.318E-09	|	+86.7	|	-81.7	|
|	2300.00	|	4.946E-09	|	+91.2	|	-84.8	|
|	2350.00	|	3.875E-09	|	+95.8	|	-88.0	|
|	2400.00	|	3.036E-09	|	+98.0	|	-91.2	|
|	2450.00	|	2.382E-09	|	+100.2	|	-94.5	|
|	2500.00	|	1.865E-09	|	+104.3	|	-98.1	|
|	2550.00	|	1.455E-09	|	+110.0	|	-102.0	|
|	2600.00	|	1.154E-09	|	+112.5	|	-104.5	|
|	2650.00	|	9.065E-10	|	+114.4	|	-107.5	|
|	2700.00	|	7.107E-10	|	+119.0	|	-111.5	|
|	2750.00	|	5.606E-10	|	+124.9	|	-114.8	|
|	2800.00	|	4.401E-10	|	+131.4	|	-118.3	|
|	2850.00	|	3.459E-10	|	+138.2	|	-121.7	|
|	2900.00	|	2.718E-10	|	+145.3	|	-125.2	|
|	2950.00	|	2.135E-10	|	+152.8	|	-128.7	|
|	3000.00	|	1.677E-10	|	+160.5	|	-132.3	|
</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)  | 

</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)  | 

</tr>
</table>

-- Main.ReiTanaka - 2016-03-01
This topic: LHCPhysics > LHCHXSWG > CERNYellowReportPageBSMAt7TeV
Topic revision: r16 - 2016-12-08 - MarcoPieri
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