(r7) CERNYellowReportPageBSMAt7TeV < LHCPhysics

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---+ SM Higgs production cross sections at &#8730;s = 13 !TeV (update in CERN Report4 2016)
   
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------------

   * Cross sections reported in CERN Report 4.
   * %BLUE% SM Higgs cross sections and BRs in Spread sheet is available in [[https://twiki.cern.ch/twiki/pub/LHCPhysics/CERNYellowReportPageAt8TeV2014/Higgs_XSBR_YR4_update.xlsx][xlsx format]] (update 2016.02.14) %ENDCOLOR% %N%
   * %BLUE% You can find figures at our gallery [[LHCHXSWGCrossSectionsFigures][here]].%ENDCOLOR% 
 
---++ Mass range and step for SM-like Higgs boson:

| *Higgs Mass range* | *step size* |  *# of points*  |  *addendum*  |
|   [120,124] !GeV  |   0.5 !GeV |   9 points  | | 
|   [124,126] !GeV  |	  0.1 !GeV |   20 points  | + M<sub>H</sub>=125.09 !GeV|
|   [126,130] !GeV  |   0.5 !GeV |   8 points  | | 
   * Total 38 points for M<sub>H</sub>=[120,130] !GeV.


---++ gluon-gluon Fusion Process

   * Cross sections are calculated with dFG program at NNLO+NNLL QCD and NLO EW accuracies. 
   * Calculations are the same as CERN Report 3 (i.e. top, bottom and charm quark effects are taken into account), except it is in NWA (CPS in CERN Report 3).  
   * Program: dFG
   * QCD scales: &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> %  |
|	120.00	|	4.738E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	120.50	|	4.704E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	121.00	|	4.670E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	121.50	|	4.637E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	122.00	|	4.604E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	122.50	|	4.571E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	123.00	|	4.539E+01	|	+7.7	|	-8.2	|	±3.1	|	±1.8	|	±2.5	|
|	123.50	|	4.507E+01	|	+7.7	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.00	|	4.476E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.10	|	4.470E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.20	|	4.463E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.30	|	4.457E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.40	|	4.451E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.50	|	4.445E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.60	|	4.438E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.70	|	4.432E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.80	|	4.426E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	124.90	|	4.420E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.00	|	4.414E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.09	|	4.408E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.10	|	4.408E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.20	|	4.402E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.30	|	4.396E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.40	|	4.390E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.50	|	4.383E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.60	|	4.377E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.70	|	4.371E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.80	|	4.365E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	125.90	|	4.359E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	126.00	|	4.353E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	126.50	|	4.324E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	127.00	|	4.294E+01	|	+7.6	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	127.50	|	4.265E+01	|	+7.5	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	128.00	|	4.236E+01	|	+7.5	|	-8.1	|	±3.1	|	±1.8	|	±2.5	|
|	128.50	|	4.207E+01	|	+7.5	|	-8.0	|	±3.1	|	±1.8	|	±2.5	|
|	129.00	|	4.179E+01	|	+7.5	|	-8.0	|	±3.1	|	±1.8	|	±2.5	|
|	129.50	|	4.151E+01	|	+7.5	|	-8.0	|	±3.1	|	±1.8	|	±2.5	|
|	130.00	|	4.123E+01	|	+7.5	|	-8.0	|	±3.1	|	±1.8	|	±2.5	|
</tr>
</table>

---++ !VBF  Process

   * Cross sections are calculated at (approx.) NNLO QCD and NLO EW accuracies. 
   * Calculations are the same as CERN Report 3, except it is in NWA (CPS in CERN Report 3).  
   * Program: NNLO QCD (!VBF@NNLO) and NLO EW (HAWK).
   * QCD scales: &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 (keeping  &mu;<sub>F</sub>=&mu;<sub>R</sub> or without constraint, i.e. &mu;<sub>F</sub> and &mu;<sub>R</sub> are varied independently?).
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  !PDF4LHC15_nnlo_100 or !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> %  |
|	120.00	|	3.935E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	120.50	|	3.919E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	121.00	|	3.904E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	121.50	|	3.888E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	122.00	|	3.873E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	122.50	|	3.858E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	123.00	|	3.842E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	123.50	|	3.827E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.00	|	3.812E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.10	|	3.809E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.20	|	3.806E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.30	|	3.803E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.40	|	3.800E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.50	|	3.797E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.60	|	3.794E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.70	|	3.791E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.80	|	3.788E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	124.90	|	3.785E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.00	|	3.782E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.09	|	3.779E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.10	|	3.779E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.20	|	3.776E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.30	|	3.773E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.40	|	3.770E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.50	|	3.767E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.60	|	3.764E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.70	|	3.761E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.80	|	3.758E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	125.90	|	3.755E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	126.00	|	3.752E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	126.50	|	3.738E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	127.00	|	3.723E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	127.50	|	3.708E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	128.00	|	3.694E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	128.50	|	3.680E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	129.00	|	3.665E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	129.50	|	3.651E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
|	130.00	|	3.637E+00	|	+0.4	|	-0.3	|	±2.1	|		|		|
</tr>
</table>


---++ WH  Process

   * Cross sections are calculated at NNLO QCD and NLO EW accuracies. 
   * Calculations are the same as CERN Report 3, except photon-induced contribution (see below).
   * Program: NNLO QCD (!VBF@NNLO) and NLO EW (HAWK).
   * 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 and &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>VH</sub>+M<sub>H</sub> for EW 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) and NNPDF2.3QED (EW part).
   * Photon-induced contribution of O(5%) (%RED%still under discussion and subject to change%ENDCOLOR%). 
      * NOT included for total cross section. 
      * Included in cross sections for dedicated WH&#8594;l&nu;H (l=e,&mu; or &tau;) process (%RED%we strongly recommend to use these numbers for dedicated analyses%ENDCOLOR%).
 
<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> %  |  W<sup>+</sup>H (pb)  |  W<sup>-</sup>H (pb)  | 
|	120.00	|	1.565E+00	|	+0.5	|	-0.6	|	±1.8	|		|		|	9.560E-01	|	6.092E-01	|
|	120.50	|	1.545E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	9.442E-01	|	6.007E-01	|
|	121.00	|	1.525E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	9.323E-01	|	5.924E-01	|
|	121.50	|	1.505E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|	9.204E-01	|	5.845E-01	|
|	122.00	|	1.485E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|	9.086E-01	|	5.764E-01	|
|	122.50	|	1.466E+00	|	+0.5	|	-0.8	|	±1.9	|		|		|	8.968E-01	|	5.693E-01	|
|	123.00	|	1.446E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.840E-01	|	5.618E-01	|
|	123.50	|	1.427E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.722E-01	|	5.545E-01	|
|	124.00	|	1.408E+00	|	+0.6	|	-0.6	|	±1.9	|		|		|	8.612E-01	|	5.465E-01	|
|	124.10	|	1.404E+00	|	+0.5	|	-0.6	|	±1.9	|		|		|	8.590E-01	|	5.454E-01	|
|	124.20	|	1.401E+00	|	+0.5	|	-0.6	|	±1.9	|		|		|	8.568E-01	|	5.440E-01	|
|	124.30	|	1.398E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.548E-01	|	5.429E-01	|
|	124.40	|	1.394E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.527E-01	|	5.415E-01	|
|	124.50	|	1.390E+00	|	+0.6	|	-0.6	|	±1.9	|		|		|	8.500E-01	|	5.395E-01	|
|	124.60	|	1.387E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.487E-01	|	5.386E-01	|
|	124.70	|	1.383E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.463E-01	|	5.372E-01	|
|	124.80	|	1.380E+00	|	+0.5	|	-0.8	|	±1.9	|		|		|	8.441E-01	|	5.360E-01	|
|	124.90	|	1.376E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.418E-01	|	5.345E-01	|
|	125.00	|	1.373E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.399E-01	|	5.327E-01	|
|	125.09	|	1.369E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.380E-01	|	5.313E-01	|
|	125.10	|	1.369E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.377E-01	|	5.313E-01	|
|	125.20	|	1.365E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.355E-01	|	5.297E-01	|
|	125.30	|	1.362E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.334E-01	|	5.282E-01	|
|	125.40	|	1.358E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.313E-01	|	5.272E-01	|
|	125.50	|	1.355E+00	|	+0.5	|	-0.7	|	±1.9	|		|		|	8.291E-01	|	5.259E-01	|
|	125.60	|	1.351E+00	|	+0.5	|	-0.6	|	±1.9	|		|		|	8.270E-01	|	5.243E-01	|
|	125.70	|	1.347E+00	|	+0.5	|	-0.6	|	±1.9	|		|		|	8.243E-01	|	5.231E-01	|
|	125.80	|	1.344E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.224E-01	|	5.217E-01	|
|	125.90	|	1.341E+00	|	+0.5	|	-0.8	|	±1.9	|		|		|	8.212E-01	|	5.202E-01	|
|	126.00	|	1.337E+00	|	+0.6	|	-0.8	|	±1.9	|		|		|	8.184E-01	|	5.187E-01	|
|	126.50	|	1.320E+00	|	+0.6	|	-0.7	|	±1.9	|		|		|	8.080E-01	|	5.123E-01	|
|	127.00	|	1.304E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	7.987E-01	|	5.051E-01	|
|	127.50	|	1.287E+00	|	+0.6	|	-0.7	|	±1.8	|		|		|	7.879E-01	|	4.988E-01	|
|	128.00	|	1.271E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	7.785E-01	|	4.923E-01	|
|	128.50	|	1.255E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	7.686E-01	|	4.863E-01	|
|	129.00	|	1.239E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	7.593E-01	|	4.801E-01	|
|	129.50	|	1.224E+00	|	+0.5	|	-0.7	|	±1.8	|		|		|	7.500E-01	|	4.738E-01	|
|	130.00	|	1.209E+00	|	+0.4	|	-0.7	|	±1.8	|		|		|	7.413E-01	|	4.676E-01	|
</tr>
</table>

---+++ WH&#8594;l&nu;H (l=e,&mu; or &tau;) Process

<table>
<tr>
| |  W<sup>+</sup>H&#8594;l<sup>+</sup>&nu;H  |||||||  W<sup>-</sup>H&#8594;l<sup>-</sup>&nu;H  |||||||
|  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> %  |  &sigma;<sub>&gamma;</sub>  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF %  |  &pm;&alpha;<sub>s</sub> %  |  &sigma;<sub>&gamma;</sub>  | 
|	120.00	|	1.099E-01	|	+0.6	|	-0.6	|	±1.8	|		|		|	6.140E-03	|	7.042E-02	|	+0.4	|	-0.6	|	±1.9	|		|		|	4.300E-03	|
|	120.50	|	1.086E-01	|	+0.5	|	-0.7	|	±1.8	|		|		|	6.120E-03	|	6.949E-02	|	+0.5	|	-0.6	|	±1.9	|		|		|	4.290E-03	|
|	121.00	|	1.073E-01	|	+0.5	|	-0.7	|	±1.8	|		|		|	6.110E-03	|	6.859E-02	|	+0.5	|	-0.6	|	±1.9	|		|		|	4.290E-03	|
|	121.50	|	1.060E-01	|	+0.4	|	-0.8	|	±1.8	|		|		|	6.100E-03	|	6.772E-02	|	+0.5	|	-0.6	|	±1.9	|		|		|	4.280E-03	|
|	122.00	|	1.047E-01	|	+0.3	|	-0.8	|	±1.8	|		|		|	6.090E-03	|	6.683E-02	|	+0.6	|	-0.6	|	±1.9	|		|		|	4.270E-03	|
|	122.50	|	1.034E-01	|	+0.5	|	-0.8	|	±1.8	|		|		|	6.070E-03	|	6.605E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.260E-03	|
|	123.00	|	1.020E-01	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.050E-03	|	6.521E-02	|	+0.5	|	-0.6	|	±2.0	|		|		|	4.240E-03	|
|	123.50	|	1.007E-01	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.040E-03	|	6.441E-02	|	+0.5	|	-0.7	|	±2.0	|		|		|	4.230E-03	|
|	124.00	|	9.950E-02	|	+0.6	|	-0.6	|	±1.8	|		|		|	6.030E-03	|	6.354E-02	|	+0.6	|	-0.6	|	±2.0	|		|		|	4.230E-03	|
|	124.10	|	9.926E-02	|	+0.5	|	-0.6	|	±1.8	|		|		|	6.030E-03	|	6.343E-02	|	+0.5	|	-0.7	|	±2.0	|		|		|	4.230E-03	|
|	124.20	|	9.902E-02	|	+0.5	|	-0.6	|	±1.8	|		|		|	6.030E-03	|	6.326E-02	|	+0.5	|	-0.6	|	±2.0	|		|		|	4.220E-03	|
|	124.30	|	9.880E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.020E-03	|	6.314E-02	|	+0.5	|	-0.6	|	±2.0	|		|		|	4.220E-03	|
|	124.40	|	9.857E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.020E-03	|	6.299E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.220E-03	|
|	124.50	|	9.828E-02	|	+0.6	|	-0.6	|	±1.8	|		|		|	6.020E-03	|	6.277E-02	|	+0.6	|	-0.6	|	±2.0	|		|		|	4.210E-03	|
|	124.60	|	9.813E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	6.020E-03	|	6.267E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.210E-03	|
|	124.70	|	9.786E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.010E-03	|	6.251E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.210E-03	|
|	124.80	|	9.762E-02	|	+0.6	|	-0.8	|	±1.8	|		|		|	6.010E-03	|	6.238E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.210E-03	|
|	124.90	|	9.738E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.010E-03	|	6.222E-02	|	+0.3	|	-0.7	|	±2.0	|		|		|	4.210E-03	|
|	125.00	|	9.717E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	6.010E-03	|	6.203E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.210E-03	|
|	125.09	|	9.695E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	6.000E-03	|	6.187E-02	|	+0.4	|	-0.6	|	±2.0	|		|		|	4.200E-03	|
|	125.10	|	9.692E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.000E-03	|	6.187E-02	|	+0.4	|	-0.6	|	±2.0	|		|		|	4.210E-03	|
|	125.20	|	9.668E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.000E-03	|	6.169E-02	|	+0.5	|	-0.6	|	±2.0	|		|		|	4.200E-03	|
|	125.30	|	9.645E-02	|	+0.6	|	-0.8	|	±1.8	|		|		|	6.000E-03	|	6.153E-02	|	+0.5	|	-0.6	|	±2.0	|		|		|	4.200E-03	|
|	125.40	|	9.622E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	6.000E-03	|	6.142E-02	|	+0.5	|	-0.8	|	±2.0	|		|		|	4.200E-03	|
|	125.50	|	9.598E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	5.990E-03	|	6.128E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.200E-03	|
|	125.60	|	9.575E-02	|	+0.5	|	-0.6	|	±1.8	|		|		|	5.990E-03	|	6.111E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.200E-03	|
|	125.70	|	9.545E-02	|	+0.6	|	-0.6	|	±1.8	|		|		|	5.990E-03	|	6.096E-02	|	+0.3	|	-0.7	|	±2.0	|		|		|	4.190E-03	|
|	125.80	|	9.524E-02	|	+0.7	|	-0.7	|	±1.8	|		|		|	5.980E-03	|	6.081E-02	|	+0.4	|	-0.8	|	±2.0	|		|		|	4.190E-03	|
|	125.90	|	9.511E-02	|	+0.6	|	-0.8	|	±1.8	|		|		|	5.980E-03	|	6.065E-02	|	+0.4	|	-0.7	|	±2.0	|		|		|	4.190E-03	|
|	126.00	|	9.481E-02	|	+0.6	|	-0.8	|	±1.8	|		|		|	5.980E-03	|	6.049E-02	|	+0.5	|	-0.7	|	±2.0	|		|		|	4.190E-03	|
|	126.50	|	9.367E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	5.970E-03	|	5.977E-02	|	+0.5	|	-0.7	|	±2.0	|		|		|	4.170E-03	|
|	127.00	|	9.264E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	5.950E-03	|	5.899E-02	|	+0.5	|	-0.6	|	±1.9	|		|		|	4.170E-03	|
|	127.50	|	9.146E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	5.940E-03	|	5.830E-02	|	+0.5	|	-0.6	|	±1.9	|		|		|	4.160E-03	|
|	128.00	|	9.042E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	5.930E-03	|	5.758E-02	|	+0.4	|	-0.6	|	±1.9	|		|		|	4.150E-03	|
|	128.50	|	8.934E-02	|	+0.6	|	-0.7	|	±1.8	|		|		|	5.920E-03	|	5.691E-02	|	+0.4	|	-0.7	|	±1.9	|		|		|	4.130E-03	|
|	129.00	|	8.831E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	5.900E-03	|	5.624E-02	|	+0.4	|	-0.7	|	±1.9	|		|		|	4.130E-03	|
|	129.50	|	8.729E-02	|	+0.5	|	-0.7	|	±1.8	|		|		|	5.890E-03	|	5.554E-02	|	+0.5	|	-0.7	|	±1.9	|		|		|	4.120E-03	|
|	130.00	|	8.634E-02	|	+0.4	|	-0.8	|	±1.8	|		|		|	5.880E-03	|	5.486E-02	|	+0.5	|	-0.6	|	±1.9	|		|		|	4.110E-03	|
</tr>
</table>


---++ ZH  Process

   * Cross sections are calculated at NNLO QCD (!VH@NNLO) and NLO EW (HAWK) accuracies. 
      * gg&#8594;ZH (box-diagram) occurs as a part of NNLO QCD correction and included in the total cross section. 
   * Calculations are the same as CERN Report 3, except photon-induced contribution (see below).
   * 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 and &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>VH</sub>+M<sub>H</sub> for EW 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) and NNPDF2.3QED (EW part).
   * Photon-induced contribution of O(1%) or below (%RED%still under discussion and subject to change%ENDCOLOR%). 
      * NOT included for total cross section. 
      * Included in cross sections for dedicated ZH&#8594;llH (l=e,&mu; or &tau;) process (%RED%we strongly recommend to use these numbers for dedicated analyses%ENDCOLOR%).

<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> %  |  &#963;(gg&#8594;ZH) (pb)  |
|	120.00	|	9.939E-01	|	+3.4	|	-3.0	|	±1.6	|		|		|	1.299E-01	|
|	120.50	|	9.829E-01	|	+3.4	|	-3.0	|	±1.6	|		|		|	1.292E-01	|
|	121.00	|	9.705E-01	|	+3.5	|	-3.0	|	±1.6	|		|		|	1.281E-01	|
|	121.50	|	9.591E-01	|	+3.6	|	-3.0	|	±1.6	|		|		|	1.269E-01	|
|	122.00	|	9.485E-01	|	+3.6	|	-3.0	|	±1.6	|		|		|	1.271E-01	|
|	122.50	|	9.371E-01	|	+3.6	|	-3.0	|	±1.6	|		|		|	1.265E-01	|
|	123.00	|	9.266E-01	|	+3.6	|	-3.1	|	±1.6	|		|		|	1.254E-01	|
|	123.50	|	9.157E-01	|	+3.5	|	-3.1	|	±1.6	|		|		|	1.250E-01	|
|	124.00	|	9.051E-01	|	+3.6	|	-3.1	|	±1.6	|		|		|	1.242E-01	|
|	124.10	|	9.037E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	1.242E-01	|
|	124.20	|	9.008E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	1.241E-01	|
|	124.30	|	8.988E-01	|	+3.7	|	-3.1	|	±1.6	|		|		|	1.239E-01	|
|	124.40	|	8.964E-01	|	+3.7	|	-3.0	|	±1.6	|		|		|	1.236E-01	|
|	124.50	|	8.943E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	1.235E-01	|
|	124.60	|	8.921E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	1.233E-01	|
|	124.70	|	8.902E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.235E-01	|
|	124.80	|	8.884E-01	|	+3.7	|	-3.1	|	±1.6	|		|		|	1.230E-01	|
|	124.90	|	8.858E-01	|	+3.9	|	-3.1	|	±1.6	|		|		|	1.227E-01	|
|	125.00	|	8.839E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.227E-01	|
|	125.09	|	8.824E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	1.227E-01	|
|	125.10	|	8.820E-01	|	+3.9	|	-3.0	|	±1.6	|		|		|	1.226E-01	|
|	125.20	|	8.800E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.223E-01	|
|	125.30	|	8.785E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.224E-01	|
|	125.40	|	8.768E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.223E-01	|
|	125.50	|	8.744E-01	|	+3.7	|	-3.1	|	±1.6	|		|		|	1.221E-01	|
|	125.60	|	8.729E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.224E-01	|
|	125.70	|	8.705E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	1.218E-01	|
|	125.80	|	8.691E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	1.219E-01	|
|	125.90	|	8.669E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.218E-01	|
|	126.00	|	8.651E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	1.218E-01	|
|	126.50	|	8.550E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	1.211E-01	|
|	127.00	|	8.447E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	1.203E-01	|
|	127.50	|	8.350E-01	|	+3.8	|	-3.2	|	±1.6	|		|		|	1.197E-01	|
|	128.00	|	8.256E-01	|	+3.9	|	-3.1	|	±1.6	|		|		|	1.190E-01	|
|	128.50	|	8.163E-01	|	+3.9	|	-3.2	|	±1.6	|		|		|	1.180E-01	|
|	129.00	|	8.073E-01	|	+3.8	|	-3.2	|	±1.6	|		|		|	1.177E-01	|
|	129.50	|	7.978E-01	|	+3.9	|	-3.2	|	±1.6	|		|		|	1.171E-01	|
|	130.00	|	7.897E-01	|	+3.9	|	-3.2	|	±1.6	|		|		|	1.164E-01	|
</tr>
</table>

---+++ ZH&#8594;llH, &nu;&nu;H (l=e,&mu; or &tau;) Process

<table>
<tr>
| |  ZH&#8594;l<sup>+</sup>l<sup>-</sup>H  ||||||||  ZH&#8594;&nu;&nu;H  ||||||||
|  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> %  |  gg&#8594;ZH (pb)  |  &sigma;<sub>&gamma;</sub>  |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF %  |  &pm;&alpha;<sub>s</sub> %  |  gg&#8594;ZH (pb)  |  &sigma;<sub>&gamma;</sub>  | 
|	120.00	|	3.363E-02	|	+3.4	|	-3.0	|	±1.6	|		|		|	4.380E-03	|	2.200E-04	|	1.997E-01	|	+3.4	|	-3.0	|	±1.6	|		|		|	2.600E-02	|	0.000E+00	|
|	120.50	|	3.326E-02	|	+3.4	|	-3.0	|	±1.6	|		|		|	4.360E-03	|	2.200E-04	|	1.975E-01	|	+3.4	|	-3.0	|	±1.6	|		|		|	2.585E-02	|	0.000E+00	|
|	121.00	|	3.284E-02	|	+3.5	|	-3.0	|	±1.6	|		|		|	4.320E-03	|	2.200E-04	|	1.950E-01	|	+3.5	|	-3.0	|	±1.6	|		|		|	2.564E-02	|	0.000E+00	|
|	121.50	|	3.246E-02	|	+3.6	|	-3.0	|	±1.6	|		|		|	4.280E-03	|	2.200E-04	|	1.927E-01	|	+3.6	|	-3.0	|	±1.6	|		|		|	2.540E-02	|	0.000E+00	|
|	122.00	|	3.210E-02	|	+3.6	|	-3.0	|	±1.6	|		|		|	4.290E-03	|	2.200E-04	|	1.906E-01	|	+3.6	|	-3.0	|	±1.6	|		|		|	2.545E-02	|	0.000E+00	|
|	122.50	|	3.172E-02	|	+3.6	|	-3.0	|	±1.6	|		|		|	4.270E-03	|	2.200E-04	|	1.883E-01	|	+3.6	|	-3.0	|	±1.6	|		|		|	2.531E-02	|	0.000E+00	|
|	123.00	|	3.136E-02	|	+3.6	|	-3.1	|	±1.6	|		|		|	4.230E-03	|	2.200E-04	|	1.862E-01	|	+3.6	|	-3.1	|	±1.6	|		|		|	2.510E-02	|	0.000E+00	|
|	123.50	|	3.100E-02	|	+3.5	|	-3.1	|	±1.6	|		|		|	4.220E-03	|	2.200E-04	|	1.840E-01	|	+3.5	|	-3.1	|	±1.6	|		|		|	2.502E-02	|	0.000E+00	|
|	124.00	|	3.064E-02	|	+3.6	|	-3.1	|	±1.6	|		|		|	4.190E-03	|	2.200E-04	|	1.819E-01	|	+3.6	|	-3.1	|	±1.6	|		|		|	2.486E-02	|	0.000E+00	|
|	124.10	|	3.059E-02	|	+3.7	|	-3.2	|	±1.6	|		|		|	4.190E-03	|	2.200E-04	|	1.816E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	2.487E-02	|	0.000E+00	|
|	124.20	|	3.050E-02	|	+3.8	|	-3.0	|	±1.6	|		|		|	4.190E-03	|	2.200E-04	|	1.810E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	2.482E-02	|	0.000E+00	|
|	124.30	|	3.043E-02	|	+3.7	|	-3.1	|	±1.6	|		|		|	4.180E-03	|	2.200E-04	|	1.806E-01	|	+3.7	|	-3.1	|	±1.6	|		|		|	2.480E-02	|	0.000E+00	|
|	124.40	|	3.035E-02	|	+3.7	|	-3.0	|	±1.6	|		|		|	4.170E-03	|	2.200E-04	|	1.801E-01	|	+3.7	|	-3.0	|	±1.6	|		|		|	2.474E-02	|	0.000E+00	|
|	124.50	|	3.028E-02	|	+3.8	|	-3.0	|	±1.6	|		|		|	4.170E-03	|	2.200E-04	|	1.797E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	2.471E-02	|	0.000E+00	|
|	124.60	|	3.020E-02	|	+3.8	|	-3.0	|	±1.6	|		|		|	4.160E-03	|	2.200E-04	|	1.793E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	2.467E-02	|	0.000E+00	|
|	124.70	|	3.014E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.170E-03	|	2.200E-04	|	1.789E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.470E-02	|	0.000E+00	|
|	124.80	|	3.008E-02	|	+3.7	|	-3.1	|	±1.6	|		|		|	4.150E-03	|	2.200E-04	|	1.785E-01	|	+3.7	|	-3.1	|	±1.6	|		|		|	2.461E-02	|	0.000E+00	|
|	124.90	|	2.999E-02	|	+3.9	|	-3.1	|	±1.6	|		|		|	4.140E-03	|	2.200E-04	|	1.780E-01	|	+3.9	|	-3.1	|	±1.6	|		|		|	2.458E-02	|	0.000E+00	|
|	125.00	|	2.993E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.140E-03	|	2.200E-04	|	1.776E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.457E-02	|	0.000E+00	|
|	125.09	|	2.987E-02	|	+3.8	|	-3.0	|	±1.6	|		|		|	4.140E-03	|	2.100E-04	|	1.773E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	2.455E-02	|	0.000E+00	|
|	125.10	|	2.986E-02	|	+3.9	|	-3.0	|	±1.6	|		|		|	4.140E-03	|	2.100E-04	|	1.772E-01	|	+3.9	|	-3.0	|	±1.6	|		|		|	2.454E-02	|	0.000E+00	|
|	125.20	|	2.979E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.130E-03	|	2.100E-04	|	1.768E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.447E-02	|	0.000E+00	|
|	125.30	|	2.974E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.130E-03	|	2.100E-04	|	1.765E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.448E-02	|	0.000E+00	|
|	125.40	|	2.968E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.130E-03	|	2.100E-04	|	1.762E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.446E-02	|	0.000E+00	|
|	125.50	|	2.960E-02	|	+3.7	|	-3.1	|	±1.6	|		|		|	4.120E-03	|	2.100E-04	|	1.757E-01	|	+3.7	|	-3.1	|	±1.6	|		|		|	2.444E-02	|	0.000E+00	|
|	125.60	|	2.955E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.130E-03	|	2.100E-04	|	1.754E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.448E-02	|	0.000E+00	|
|	125.70	|	2.947E-02	|	+3.8	|	-3.0	|	±1.6	|		|		|	4.110E-03	|	2.100E-04	|	1.749E-01	|	+3.8	|	-3.0	|	±1.6	|		|		|	2.436E-02	|	0.000E+00	|
|	125.80	|	2.943E-02	|	+3.7	|	-3.2	|	±1.6	|		|		|	4.110E-03	|	2.100E-04	|	1.746E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	2.440E-02	|	0.000E+00	|
|	125.90	|	2.935E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.110E-03	|	2.100E-04	|	1.742E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.436E-02	|	0.000E+00	|
|	126.00	|	2.929E-02	|	+3.8	|	-3.1	|	±1.6	|		|		|	4.110E-03	|	2.100E-04	|	1.738E-01	|	+3.8	|	-3.1	|	±1.6	|		|		|	2.437E-02	|	0.000E+00	|
|	126.50	|	2.895E-02	|	+3.7	|	-3.2	|	±1.6	|		|		|	4.090E-03	|	2.100E-04	|	1.718E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	2.423E-02	|	0.000E+00	|
|	127.00	|	2.861E-02	|	+3.7	|	-3.2	|	±1.6	|		|		|	4.060E-03	|	2.100E-04	|	1.697E-01	|	+3.7	|	-3.2	|	±1.6	|		|		|	2.407E-02	|	0.000E+00	|
|	127.50	|	2.827E-02	|	+3.8	|	-3.2	|	±1.6	|		|		|	4.040E-03	|	2.100E-04	|	1.678E-01	|	+3.8	|	-3.2	|	±1.6	|		|		|	2.394E-02	|	0.000E+00	|
|	128.00	|	2.796E-02	|	+3.9	|	-3.1	|	±1.6	|		|		|	4.020E-03	|	2.100E-04	|	1.659E-01	|	+3.9	|	-3.1	|	±1.6	|		|		|	2.381E-02	|	0.000E+00	|
|	128.50	|	2.765E-02	|	+3.9	|	-3.2	|	±1.6	|		|		|	3.980E-03	|	2.100E-04	|	1.640E-01	|	+3.9	|	-3.2	|	±1.6	|		|		|	2.362E-02	|	0.000E+00	|
|	129.00	|	2.735E-02	|	+3.8	|	-3.2	|	±1.6	|		|		|	3.970E-03	|	2.100E-04	|	1.622E-01	|	+3.8	|	-3.2	|	±1.6	|		|		|	2.355E-02	|	0.000E+00	|
|	129.50	|	2.703E-02	|	+3.9	|	-3.2	|	±1.6	|		|		|	3.950E-03	|	2.100E-04	|	1.603E-01	|	+3.9	|	-3.2	|	±1.6	|		|		|	2.344E-02	|	0.000E+00	|
|	130.00	|	2.675E-02	|	+3.9	|	-3.2	|	±1.6	|		|		|	3.930E-03	|	2.100E-04	|	1.587E-01	|	+3.9	|	-3.2	|	±1.6	|		|		|	2.329E-02	|	0.000E+00	|
</tr>
</table>


---++ ttH  Process
 
   * Cross sections are calculated at NLO QCD and NLO EW accuracies. 
   * Calculations are the same as CERN Report 3, except NLO EW corrections are adopted now.
   * Program: !MadGraph5_aMC@NLO (Sherpa+OpenLoops as cross ceck)
   * QCD scales: &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> %  |
|	120.00	|	5.697E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	120.50	|	5.625E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	121.00	|	5.568E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	121.50	|	5.502E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	122.00	|	5.438E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	122.50	|	5.375E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	123.00	|	5.315E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	123.50	|	5.259E-01	|	+5.9	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.00	|	5.193E-01	|	+5.9	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.10	|	5.179E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.20	|	5.167E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.30	|	5.161E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	124.40	|	5.143E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.50	|	5.132E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.60	|	5.122E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	124.70	|	5.115E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	124.80	|	5.100E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	124.90	|	5.086E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.00	|	5.071E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.09	|	5.065E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.10	|	5.060E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	125.20	|	5.052E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.30	|	5.043E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.40	|	5.033E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	125.50	|	5.023E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	125.60	|	5.007E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.70	|	4.993E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.80	|	4.982E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	125.90	|	4.971E-01	|	+5.9	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	126.00	|	4.964E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	126.50	|	4.909E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	127.00	|	4.851E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	127.50	|	4.799E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	128.00	|	4.742E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	128.50	|	4.689E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	129.00	|	4.639E-01	|	+5.8	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
|	129.50	|	4.586E-01	|	+5.8	|	-9.2	|	±3.6	|	±3.0	|	±2.0	|
|	130.00	|	4.539E-01	|	+5.8	|	-9.3	|	±3.6	|	±3.0	|	±2.0	|
</tr>
</table>


---++ bbH  Process 
   * The cross  sections are the Santander matched numbers with 5FS (NNLO) and 4FS (NLO).
   * %RED% 4FS includes Y<sub>t</sub>*Y<sub>b</sub> term (O(10%) negative correction) in addition to Y<sub>b</sub><sup>2</sup>. 

<table>
<tr>
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +(QCD Scale+PDF+&alpha;<sub>s</sub>) %  |  -(QCD Scale+PDF+&alpha;<sub>s</sub>) %  |
|	120.00	|	5.534E-01	|	+20.3	|	-24.4	|
|	120.50	|	5.471E-01	|	+20.3	|	-24.4	|
|	121.00	|	5.414E-01	|	+20.4	|	-24.3	|
|	121.50	|	5.343E-01	|	+20.5	|	-24.3	|
|	122.00	|	5.268E-01	|	+20.4	|	-24.3	|
|	122.50	|	5.200E-01	|	+20.2	|	-24.2	|
|	123.00	|	5.124E-01	|	+21.2	|	-24.1	|
|	123.50	|	5.066E-01	|	+20.1	|	-24.0	|
|	124.00	|	4.999E-01	|	+20.1	|	-24.0	|
|	124.10	|	4.985E-01	|	+20.1	|	-24.0	|
|	124.20	|	4.976E-01	|	+20.3	|	-24.1	|
|	124.30	|	4.955E-01	|	+20.2	|	-24.1	|
|	124.40	|	4.950E-01	|	+20.3	|	-24.1	|
|	124.50	|	4.930E-01	|	+20.0	|	-23.9	|
|	124.60	|	4.918E-01	|	+20.1	|	-24.0	|
|	124.70	|	4.919E-01	|	+20.6	|	-24.1	|
|	124.80	|	4.899E-01	|	+20.2	|	-24.0	|
|	124.90	|	4.891E-01	|	+20.3	|	-24.1	|
|	125.00	|	4.880E-01	|	+20.2	|	-23.9	|
|	125.09	|	4.863E-01	|	+20.1	|	-23.9	|
|	125.10	|	4.860E-01	|	+20.5	|	-23.9	|
|	125.20	|	4.850E-01	|	+20.1	|	-24.0	|
|	125.30	|	4.833E-01	|	+20.1	|	-24.0	|
|	125.40	|	4.822E-01	|	+20.2	|	-24.0	|
|	125.50	|	4.809E-01	|	+20.1	|	-23.8	|
|	125.60	|	4.792E-01	|	+20.1	|	-23.9	|
|	125.70	|	4.789E-01	|	+20.1	|	-23.9	|
|	125.80	|	4.768E-01	|	+20.1	|	-23.9	|
|	125.90	|	4.757E-01	|	+20.2	|	-24.0	|
|	126.00	|	4.760E-01	|	+20.2	|	-23.8	|
|	126.50	|	4.695E-01	|	+20.0	|	-23.7	|
|	127.00	|	4.635E-01	|	+20.0	|	-23.7	|
|	127.50	|	4.580E-01	|	+20.0	|	-23.6	|
|	128.00	|	4.513E-01	|	+19.9	|	-23.6	|
|	128.50	|	4.463E-01	|	+19.9	|	-23.5	|
|	129.00	|	4.416E-01	|	+20.0	|	-23.4	|
|	129.50	|	4.358E-01	|	+19.9	|	-23.4	|
|	130.00	|	4.304E-01	|	+19.9	|	-23.3	|


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

   * Cross sections are calculated at NLO QCD accuracy (no NLO EW correction) 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> % |  tH (pb)  |  tbarH (pb)  | 
|	120.00	|	7.731E-02	|	+6.7	|	-14.6	|	±3.7	|	±3.5	|	±1.2	|	5.086E-02	|	2.643E-02	|
|	120.50	|	7.711E-02	|	+6.7	|	-14.8	|	±3.7	|	±3.5	|	±1.2	|	5.071E-02	|	2.633E-02	|
|	121.00	|	7.684E-02	|	+6.7	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	5.047E-02	|	2.623E-02	|
|	121.50	|	7.648E-02	|	+6.6	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	5.024E-02	|	2.613E-02	|
|	122.00	|	7.614E-02	|	+6.7	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	5.011E-02	|	2.602E-02	|
|	122.50	|	7.581E-02	|	+6.6	|	-14.6	|	±3.7	|	±3.5	|	±1.2	|	4.985E-02	|	2.590E-02	|
|	123.00	|	7.552E-02	|	+6.6	|	-14.8	|	±3.7	|	±3.5	|	±1.2	|	4.972E-02	|	2.584E-02	|
|	123.50	|	7.523E-02	|	+6.6	|	-14.9	|	±3.7	|	±3.5	|	±1.2	|	4.947E-02	|	2.575E-02	|
|	124.00	|	7.499E-02	|	+6.6	|	-15.1	|	±3.7	|	±3.5	|	±1.2	|	4.930E-02	|	2.560E-02	|
|	124.10	|	7.471E-02	|	+6.6	|	-14.6	|	±3.7	|	±3.5	|	±1.2	|	4.935E-02	|	2.559E-02	|
|	124.20	|	7.477E-02	|	+6.6	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	4.925E-02	|	2.558E-02	|
|	124.30	|	7.481E-02	|	+6.5	|	-14.9	|	±3.7	|	±3.5	|	±1.2	|	4.915E-02	|	2.556E-02	|
|	124.40	|	7.477E-02	|	+6.6	|	-14.9	|	±3.7	|	±3.5	|	±1.2	|	4.918E-02	|	2.557E-02	|
|	124.50	|	7.459E-02	|	+6.6	|	-14.9	|	±3.7	|	±3.5	|	±1.2	|	4.914E-02	|	2.553E-02	|
|	124.60	|	7.452E-02	|	+6.6	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	4.904E-02	|	2.549E-02	|
|	124.70	|	7.448E-02	|	+6.6	|	-14.8	|	±3.7	|	±3.5	|	±1.2	|	4.901E-02	|	2.549E-02	|
|	124.80	|	7.448E-02	|	+6.6	|	-14.9	|	±3.7	|	±3.5	|	±1.2	|	4.898E-02	|	2.546E-02	|
|	124.90	|	7.447E-02	|	+6.6	|	-15.1	|	±3.7	|	±3.6	|	±1.2	|	4.894E-02	|	2.542E-02	|
|	125.00	|	7.425E-02	|	+6.5	|	-14.9	|	±3.7	|	±3.5	|	±1.2	|	4.889E-02	|	2.542E-02	|
|	125.09	|	7.426E-02	|	+6.5	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	4.889E-02	|	2.540E-02	|
|	125.10	|	7.426E-02	|	+6.5	|	-14.7	|	±3.7	|	±3.5	|	±1.2	|	4.889E-02	|	2.540E-02	|
|	125.20	|	7.432E-02	|	+6.5	|	-15.0	|	±3.7	|	±3.5	|	±1.2	|	4.887E-02	|	2.540E-02	|
|	125.30	|	7.430E-02	|	+6.6	|	-14.9	|	±3.8	|	±3.6	|	±1.2	|	4.881E-02	|	2.538E-02	|
|	125.40	|	7.414E-02	|	+6.6	|	-14.9	|	±3.7	|	±3.6	|	±1.2	|	4.879E-02	|	2.534E-02	|
|	125.50	|	7.407E-02	|	+6.6	|	-15.0	|	±3.7	|	±3.5	|	±1.2	|	4.877E-02	|	2.534E-02	|
|	125.60	|	7.409E-02	|	+6.5	|	-15.2	|	±3.7	|	±3.6	|	±1.2	|	4.875E-02	|	2.532E-02	|
|	125.70	|	7.401E-02	|	+6.5	|	-15.0	|	±3.7	|	±3.6	|	±1.2	|	4.870E-02	|	2.531E-02	|
|	125.80	|	7.390E-02	|	+6.5	|	-15.0	|	±3.7	|	±3.6	|	±1.2	|	4.865E-02	|	2.530E-02	|
|	125.90	|	7.370E-02	|	+6.6	|	-14.8	|	±3.7	|	±3.5	|	±1.2	|	4.857E-02	|	2.530E-02	|
|	126.00	|	7.375E-02	|	+6.5	|	-15.0	|	±3.7	|	±3.6	|	±1.2	|	4.858E-02	|	2.527E-02	|
|	126.50	|	7.353E-02	|	+6.5	|	-14.9	|	±3.8	|	±3.6	|	±1.2	|	4.837E-02	|	2.516E-02	|
|	127.00	|	7.329E-02	|	+6.5	|	-15.1	|	±3.8	|	±3.6	|	±1.2	|	4.820E-02	|	2.511E-02	|
|	127.50	|	7.304E-02	|	+6.5	|	-15.1	|	±3.8	|	±3.6	|	±1.2	|	4.807E-02	|	2.499E-02	|
|	128.00	|	7.277E-02	|	+6.5	|	-15.1	|	±3.8	|	±3.6	|	±1.2	|	4.793E-02	|	2.491E-02	|
|	128.50	|	7.244E-02	|	+6.4	|	-15.0	|	±3.8	|	±3.6	|	±1.2	|	4.765E-02	|	2.481E-02	|
|	129.00	|	7.223E-02	|	+6.4	|	-15.1	|	±3.8	|	±3.6	|	±1.2	|	4.755E-02	|	2.474E-02	|
|	129.50	|	7.203E-02	|	+6.4	|	-15.2	|	±3.8	|	±3.6	|	±1.2	|	4.734E-02	|	2.466E-02	|
|	130.00	|	7.184E-02	|	+6.4	|	-15.3	|	±3.8	|	±3.6	|	±1.2	|	4.723E-02	|	2.459E-02	|
</tr>
</table>

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

   * Cross sections are calculated at NLO QCD accuracy (no NLO EW correction) 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> % |  tH (pb)  |  tbarH (pb)  | 
|	120.00	|	3.158E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	2.060E-03	|	1.095E-03	|
|	120.50	|	3.124E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	2.042E-03	|	1.083E-03	|
|	121.00	|	3.101E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	2.022E-03	|	1.073E-03	|
|	121.50	|	3.068E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	2.006E-03	|	1.063E-03	|
|	122.00	|	3.045E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	1.989E-03	|	1.052E-03	|
|	122.50	|	3.007E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	1.971E-03	|	1.043E-03	|
|	123.00	|	2.988E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.3	|	1.953E-03	|	1.033E-03	|
|	123.50	|	2.960E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.935E-03	|	1.023E-03	|
|	124.00	|	2.932E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.915E-03	|	1.014E-03	|
|	124.10	|	2.928E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.916E-03	|	1.012E-03	|
|	124.20	|	2.920E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.912E-03	|	1.010E-03	|
|	124.30	|	2.918E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.906E-03	|	1.008E-03	|
|	124.40	|	2.908E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.904E-03	|	1.006E-03	|
|	124.50	|	2.907E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.902E-03	|	1.004E-03	|
|	124.60	|	2.901E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.897E-03	|	1.003E-03	|
|	124.70	|	2.900E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.892E-03	|	1.000E-03	|
|	124.80	|	2.895E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.891E-03	|	9.980E-04	|
|	124.90	|	2.886E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.888E-03	|	9.960E-04	|
|	125.00	|	2.879E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.882E-03	|	9.960E-04	|
|	125.09	|	2.875E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.881E-03	|	9.930E-04	|
|	125.10	|	2.875E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.881E-03	|	9.930E-04	|
|	125.20	|	2.871E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.876E-03	|	9.910E-04	|
|	125.30	|	2.861E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.874E-03	|	9.890E-04	|
|	125.40	|	2.860E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.871E-03	|	9.880E-04	|
|	125.50	|	2.857E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.868E-03	|	9.870E-04	|
|	125.60	|	2.851E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.863E-03	|	9.830E-04	|
|	125.70	|	2.845E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.859E-03	|	9.820E-04	|
|	125.80	|	2.842E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.858E-03	|	9.800E-04	|
|	125.90	|	2.835E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.855E-03	|	9.790E-04	|
|	126.00	|	2.826E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.849E-03	|	9.770E-04	|
|	126.50	|	2.802E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.837E-03	|	9.670E-04	|
|	127.00	|	2.780E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.820E-03	|	9.590E-04	|
|	127.50	|	2.752E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.804E-03	|	9.500E-04	|
|	128.00	|	2.726E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.788E-03	|	9.410E-04	|
|	128.50	|	2.705E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.771E-03	|	9.330E-04	|
|	129.00	|	2.683E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.755E-03	|	9.240E-04	|
|	129.50	|	2.657E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.742E-03	|	9.160E-04	|
|	130.00	|	2.633E-03	|	+2.4	|	-1.8	|	±2.2	|	±2.2	|	±0.2	|	1.728E-03	|	9.080E-04	|
</tr>
</table>

-- Main.ReiTanaka - 2016-02-13
Topic revision: r7 - 2016-02-16 - ReiTanaka
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