(r18) CERNYellowReportPageAt7TeV < LHCPhysics

LHCPhysics Web>LHCHXSWG>CERNYellowReportPageAt7TeV (revision 18) (raw view)~~EditAttachPDF~~
<!--
   * Set ALLOWTOPICCHANGE = Main.ReiTanaka, Main.MarkusSchumacher2, Main.PierreSavard, Main.ChiaraMariotti, Main.AlexandreNikitenko, Main.MarcoPieri, Main.ChristopheGrojean, Main.DanielDeFlorian, Main.FabioMaltoni
-->


---+ SM 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% 
 
---++ 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

   __%PURPLE%N3LO QCD cross sections supercede those of NNLO+NNLL QCD%ENDCOLOR%__

---+++ *%RED%N3LO%ENDCOLOR%* 
   * Cross sections are calculated by Zürich group at !N3LO QCD and NLO EW accuracies [Anastasiou:2016cez]. 
   * QCD scales: &mu;=&mu;<sub>F</sub>=&mu;<sub>R</sub>=M<sub>H</sub>/2 varied in the range of [M<sub>H</sub>/4,M<sub>H</sub>].
   * Theory uncertainty:
      * "±Theory" uncertainty is interpreted as a flat 100% confidence level. 
      * "TH Gaussian" uncertainty is interpreted as a one-sigma range. It is estimated by max{+TH,-TH}/sqrt{3} as discussed in CERN Report 4 ggF section. 
      * %PURPLE%"TH Gaussian" uncertainty should be used for the construction of the workspace in the current [[http://cds.cern.ch/record/1375842/][LHC-HCG prescription]]%ENDCOLOR%.  
   * PDF set:  !PDF4LHC15_nnlo_100

---+++ *%BLUE%NNLO+NNLL%ENDCOLOR%* 
   * 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>
| |   *%RED%N3LO%ENDCOLOR%*   ||||||| |   *%BLUE%NNLO+NNLL%ENDCOLOR%*   ||||||
|  m<sub>H</sub> (!GeV)  |  Cross Section (pb)  |  +Theory %  |  -Theory %  |  TH Gaussian %   |   &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  | |  Cross Section (pb)  |  +QCD Scale %  |  -QCD Scale %  |  &pm;(PDF+&alpha;<sub>s</sub>) %  |  &pm;PDF % | &pm;&alpha;<sub>s</sub> %  |
|	120.00 	|	1.831E+01	|	+4.5	|	-7.1 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.661E+01	|	+7.4	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	120.50 	|	1.816E+01	|	+4.5	|	-7.1 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.647E+01	|	+7.4	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	121.00 	|	1.800E+01	|	+4.5	|	-7.1 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.634E+01	|	+7.4	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	121.50 	|	1.785E+01	|	+4.5	|	-7.1 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.620E+01	|	+7.4	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	122.00 	|	1.771E+01	|	+4.5	|	-7.1 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.607E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	122.50 	|	1.756E+01	|	+4.5	|	-7.0 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.594E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	123.00 	|	1.741E+01	|	+4.5	|	-7.0 	|	±4.1	|	±3.3	|	±1.9	|	±2.7	|		|	1.581E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	123.50 	|	1.727E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.568E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.00 	|	1.713E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.556E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.10 	|	1.710E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.553E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.20 	|	1.707E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.551E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.30 	|	1.704E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.548E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.40 	|	1.702E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.546E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.50 	|	1.699E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.543E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.60 	|	1.696E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.541E+01	|	+7.3	|	-8.0 	|	±3.2	|	±1.8	|	±2.6	|
|	124.70 	|	1.693E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.538E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	124.80 	|	1.690E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.536E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	124.90 	|	1.688E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.533E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.00 	|	1.685E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.531E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.09 	|	1.682E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.529E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.10 	|	1.682E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.528E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.20 	|	1.679E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.526E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.30 	|	1.677E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.523E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.40 	|	1.674E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.521E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.50 	|	1.671E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.519E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.60 	|	1.668E+01	|	+4.4	|	-7.0 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.516E+01	|	+7.3	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.70 	|	1.666E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.514E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.80 	|	1.663E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.511E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	125.90 	|	1.660E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.509E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	126.00 	|	1.658E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.507E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	126.50 	|	1.644E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.495E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	127.00 	|	1.631E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.483E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	127.50 	|	1.618E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.471E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	128.00 	|	1.605E+01	|	+4.4	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.460E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	128.50 	|	1.592E+01	|	+4.3	|	-6.9 	|	±4.0	|	±3.3	|	±1.9	|	±2.7	|		|	1.448E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	129.00 	|	1.580E+01	|	+4.3	|	-6.8 	|	±3.9	|	±3.3	|	±1.9	|	±2.7	|		|	1.437E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	129.50 	|	1.567E+01	|	+4.3	|	-6.8 	|	±3.9	|	±3.3	|	±1.9	|	±2.7	|		|	1.426E+01	|	+7.2	|	-7.9 	|	±3.2	|	±1.8	|	±2.6	|
|	130.00 	|	1.555E+01	|	+4.3	|	-6.8 	|	±3.9	|	±3.3	|	±1.9	|	±2.7	|		|	1.415E+01	|	+7.1	|	-7.8 	|	±3.2	|	±1.8	|	±2.6	|
</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>).
      * No additional THU nor PU uncertainties assigned. 
   * PDF set:  !PDF4LHC15_nnlo_100 (QCD corrections) and !NNPDF2.3QED (EW corrections + photon PDF)

<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	|	1.302E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	120.50	|	1.296E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	121.00	|	1.289E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	121.50	|	1.283E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	122.00	|	1.277E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	122.50	|	1.271E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	123.00	|	1.265E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	123.50	|	1.259E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.00	|	1.253E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.10	|	1.252E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.20	|	1.251E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.30	|	1.250E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.40	|	1.249E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.50	|	1.247E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.60	|	1.246E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.70	|	1.245E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.80	|	1.244E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	124.90	|	1.243E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.00	|	1.241E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.09	|	1.240E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.10	|	1.240E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.20	|	1.239E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.30	|	1.238E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.40	|	1.237E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.50	|	1.236E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.60	|	1.235E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.70	|	1.233E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.80	|	1.232E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	125.90	|	1.231E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	126.00	|	1.230E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	126.50	|	1.224E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	127.00	|	1.218E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	127.50	|	1.213E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	128.00	|	1.207E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	128.50	|	1.201E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	129.00	|	1.196E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	129.50	|	1.190E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
|	130.00	|	1.185E+00	|	+0.2	|	-0.2	|	±2.2	|	±2.1	|	±0.4	|
</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). 
      * Total cross section is calculated from WH&#8594;l&nu;H cross section by subtracting photon-induced cross section, and then scaled via BR(W&#8594;l&nu;)=0.108535 in NLO EW accuracy.  
   * Program: NNLO QCD (!VH@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% NOT included for total cross section %ENDCOLOR% (agrees with CERN Report 3 numbers within 1%). 
      * %RED% Included in cross sections for dedicated WH&#8594;l&nu;H (l=e,&mu; or &tau;) process (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	|	6.625E-01	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	4.233E-01	|	2.392E-01	|
|	120.50	|	6.532E-01	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	4.176E-01	|	2.357E-01	|
|	121.00	|	6.439E-01	|	+0.7	|	-0.9	|	±2.0	|	±2.0	|	±0.6	|	4.116E-01	|	2.324E-01	|
|	121.50	|	6.349E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	4.059E-01	|	2.291E-01	|
|	122.00	|	6.264E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	4.006E-01	|	2.258E-01	|
|	122.50	|	6.180E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.954E-01	|	2.226E-01	|
|	123.00	|	6.097E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.900E-01	|	2.197E-01	|
|	123.50	|	6.012E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.846E-01	|	2.166E-01	|
|	124.00	|	5.931E-01	|	+0.6	|	-0.8	|	±2.1	|	±2.0	|	±0.7	|	3.795E-01	|	2.136E-01	|
|	124.10	|	5.915E-01	|	+0.6	|	-0.8	|	±2.1	|	±2.0	|	±0.7	|	3.785E-01	|	2.130E-01	|
|	124.20	|	5.899E-01	|	+0.6	|	-0.8	|	±2.1	|	±2.0	|	±0.7	|	3.774E-01	|	2.125E-01	|
|	124.30	|	5.883E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.766E-01	|	2.117E-01	|
|	124.40	|	5.867E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.756E-01	|	2.111E-01	|
|	124.50	|	5.853E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.746E-01	|	2.107E-01	|
|	124.60	|	5.838E-01	|	+0.6	|	-1.0	|	±2.1	|	±2.0	|	±0.7	|	3.738E-01	|	2.100E-01	|
|	124.70	|	5.820E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.726E-01	|	2.094E-01	|
|	124.80	|	5.804E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.716E-01	|	2.088E-01	|
|	124.90	|	5.788E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.706E-01	|	2.082E-01	|
|	125.00	|	5.771E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.696E-01	|	2.076E-01	|
|	125.09	|	5.756E-01	|	+0.7	|	-0.8	|	±2.1	|	±2.0	|	±0.7	|	3.685E-01	|	2.070E-01	|
|	125.10	|	5.756E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.686E-01	|	2.069E-01	|
|	125.20	|	5.740E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.677E-01	|	2.063E-01	|
|	125.30	|	5.725E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.667E-01	|	2.058E-01	|
|	125.40	|	5.708E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.656E-01	|	2.052E-01	|
|	125.50	|	5.694E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.648E-01	|	2.046E-01	|
|	125.60	|	5.679E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.638E-01	|	2.041E-01	|
|	125.70	|	5.665E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.629E-01	|	2.035E-01	|
|	125.80	|	5.650E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.619E-01	|	2.031E-01	|
|	125.90	|	5.633E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.608E-01	|	2.025E-01	|
|	126.00	|	5.618E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.599E-01	|	2.019E-01	|
|	126.50	|	5.542E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.551E-01	|	1.991E-01	|
|	127.00	|	5.469E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.505E-01	|	1.964E-01	|
|	127.50	|	5.395E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.7	|	3.459E-01	|	1.937E-01	|
|	128.00	|	5.323E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.414E-01	|	1.909E-01	|
|	128.50	|	5.253E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.368E-01	|	1.884E-01	|
|	129.00	|	5.182E-01	|	+0.7	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.324E-01	|	1.857E-01	|
|	129.50	|	5.116E-01	|	+0.6	|	-1.0	|	±2.1	|	±2.0	|	±0.6	|	3.283E-01	|	1.834E-01	|
|	130.00	|	5.046E-01	|	+0.6	|	-0.9	|	±2.1	|	±2.0	|	±0.6	|	3.240E-01	|	1.807E-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	|	4.685E-02	|	+0.6	|	-0.9	|	±1.9	|	±1.8	|	±0.6	|	9.10E-04	|	2.648E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.20E-04	|
|	120.50	|	4.622E-02	|	+0.6	|	-1.0	|	±1.9	|	±1.8	|	±0.6	|	9.00E-04	|	2.610E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.20E-04	|
|	121.00	|	4.557E-02	|	+0.7	|	-0.9	|	±1.9	|	±1.9	|	±0.6	|	9.00E-04	|	2.574E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.20E-04	|
|	121.50	|	4.495E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	9.00E-04	|	2.538E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.20E-04	|
|	122.00	|	4.438E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	9.00E-04	|	2.503E-02	|	+0.7	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.20E-04	|
|	122.50	|	4.380E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.90E-04	|	2.468E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.20E-04	|
|	123.00	|	4.322E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.90E-04	|	2.435E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	123.50	|	4.263E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.90E-04	|	2.402E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.00	|	4.207E-02	|	+0.7	|	-0.8	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.369E-02	|	+0.5	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.10	|	4.196E-02	|	+0.7	|	-0.8	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.363E-02	|	+0.5	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.20	|	4.184E-02	|	+0.7	|	-0.8	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.357E-02	|	+0.5	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.30	|	4.175E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.349E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.40	|	4.165E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.342E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.50	|	4.154E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.338E-02	|	+0.5	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.60	|	4.145E-02	|	+0.6	|	-1.0	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.330E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.70	|	4.132E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.324E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.80	|	4.121E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.317E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	124.90	|	4.110E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.311E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.00	|	4.099E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.304E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.09	|	4.088E-02	|	+0.7	|	-0.8	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.298E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.10	|	4.089E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.297E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.20	|	4.079E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.290E-02	|	+0.7	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.30	|	4.068E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.285E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.40	|	4.056E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.278E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.50	|	4.047E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.80E-04	|	2.272E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.60	|	4.036E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.266E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.2	|	±0.6	|	5.10E-04	|
|	125.70	|	4.026E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.259E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.2	|	±0.6	|	5.00E-04	|
|	125.80	|	4.015E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.254E-02	|	+0.6	|	-0.8	|	±2.3	|	±2.3	|	±0.6	|	5.00E-04	|
|	125.90	|	4.003E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.248E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.3	|	±0.6	|	5.00E-04	|
|	126.00	|	3.993E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.241E-02	|	+0.7	|	-0.8	|	±2.3	|	±2.3	|	±0.6	|	5.00E-04	|
|	126.50	|	3.941E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.211E-02	|	+0.6	|	-0.9	|	±2.3	|	±2.3	|	±0.6	|	5.00E-04	|
|	127.00	|	3.891E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.70E-04	|	2.182E-02	|	+0.6	|	-1.0	|	±2.3	|	±2.3	|	±0.6	|	5.00E-04	|
|	127.50	|	3.840E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.7	|	8.60E-04	|	2.152E-02	|	+0.6	|	-0.9	|	±2.4	|	±2.3	|	±0.6	|	5.00E-04	|
|	128.00	|	3.791E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.60E-04	|	2.122E-02	|	+0.7	|	-0.9	|	±2.4	|	±2.3	|	±0.6	|	5.00E-04	|
|	128.50	|	3.742E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.60E-04	|	2.094E-02	|	+0.7	|	-0.9	|	±2.4	|	±2.3	|	±0.6	|	4.90E-04	|
|	129.00	|	3.694E-02	|	+0.7	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.60E-04	|	2.065E-02	|	+0.6	|	-0.9	|	±2.4	|	±2.3	|	±0.6	|	4.90E-04	|
|	129.50	|	3.648E-02	|	+0.6	|	-1.0	|	±2.0	|	±1.9	|	±0.6	|	8.50E-04	|	2.039E-02	|	+0.6	|	-0.9	|	±2.4	|	±2.3	|	±0.6	|	4.90E-04	|
|	130.00	|	3.601E-02	|	+0.6	|	-0.9	|	±2.0	|	±1.9	|	±0.6	|	8.50E-04	|	2.010E-02	|	+0.7	|	-0.9	|	±2.4	|	±2.3	|	±0.6	|	4.90E-04	|
</tr>
</table>


---++ ZH  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). 
      * Total cross section is calculated from ZH&#8594;llH,&nu;&nu;H cross sections by subtracting photon-induced cross section, and then scaled via BR(Z&#8594;ll)=0.0335962 and BR(Z&#8594;&nu;&nu;)=0.201030 in NLO EW accuracy.  
      * gg&#8594;ZH (box-diagram) occurs as a part of NNLO QCD correction and included in the total cross section. 
      * ZH cross section went up by +1~2%, due to +22~16% for &#8730;s = 7-14 !TeV, due to increase in gg&#8594;ZH for NLO+NLL QCD corrections (NLO in CERN Report 3).
   * Program: NNLO QCD (!VH@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(1%) or below 
      * %RED% NOT included for total cross section %ENDCOLOR% (agrees with CERN Report 3 numbers). 
      * %RED% Included in cross sections for dedicated ZH&#8594;llH,&nu;&nu;H (l=e,&mu; or &tau;) processes (%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	|	3.851E-01	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	2.961E-02	|
|	120.50	|	3.803E-01	|	+2.4	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	2.938E-02	|
|	121.00	|	3.755E-01	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	2.931E-02	|
|	121.50	|	3.705E-01	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	2.909E-02	|
|	122.00	|	3.657E-01	|	+2.6	|	-2.1	|	±1.7	|	±1.6	|	±0.7	|	2.896E-02	|
|	122.50	|	3.612E-01	|	+2.6	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	2.876E-02	|
|	123.00	|	3.563E-01	|	+2.7	|	-2.1	|	±1.7	|	±1.6	|	±0.7	|	2.851E-02	|
|	123.50	|	3.518E-01	|	+2.6	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	2.841E-02	|
|	124.00	|	3.478E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.839E-02	|
|	124.10	|	3.470E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.822E-02	|
|	124.20	|	3.461E-01	|	+2.5	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.822E-02	|
|	124.30	|	3.452E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.817E-02	|
|	124.40	|	3.444E-01	|	+2.5	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.817E-02	|
|	124.50	|	3.434E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.814E-02	|
|	124.60	|	3.426E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.814E-02	|
|	124.70	|	3.417E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.809E-02	|
|	124.80	|	3.408E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.792E-02	|
|	124.90	|	3.401E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.792E-02	|
|	125.00	|	3.392E-01	|	+2.6	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	2.789E-02	|
|	125.09	|	3.384E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.792E-02	|
|	125.10	|	3.383E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.789E-02	|
|	125.20	|	3.375E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.789E-02	|
|	125.30	|	3.366E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.787E-02	|
|	125.40	|	3.357E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.784E-02	|
|	125.50	|	3.348E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.782E-02	|
|	125.60	|	3.339E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.782E-02	|
|	125.70	|	3.333E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.782E-02	|
|	125.80	|	3.325E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.779E-02	|
|	125.90	|	3.315E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.762E-02	|
|	126.00	|	3.307E-01	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.760E-02	|
|	126.50	|	3.265E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.752E-02	|
|	127.00	|	3.225E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.730E-02	|
|	127.50	|	3.185E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.722E-02	|
|	128.00	|	3.146E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.697E-02	|
|	128.50	|	3.109E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.690E-02	|
|	129.00	|	3.071E-01	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	2.665E-02	|
|	129.50	|	3.033E-01	|	+2.7	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	2.645E-02	|
|	130.00	|	2.996E-01	|	+2.7	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	2.635E-02	|
</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	|	1.297E-02	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	1.00E-03	|	3.00E-05	|	7.740E-02	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	5.92E-03	|	0.00E+00	|
|	120.50	|	1.281E-02	|	+2.4	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	9.90E-04	|	3.00E-05	|	7.643E-02	|	+2.4	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	5.89E-03	|	0.00E+00	|
|	121.00	|	1.265E-02	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	9.90E-04	|	3.00E-05	|	7.546E-02	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	5.86E-03	|	0.00E+00	|
|	121.50	|	1.248E-02	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	9.80E-04	|	3.00E-05	|	7.448E-02	|	+2.5	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	5.83E-03	|	0.00E+00	|
|	122.00	|	1.232E-02	|	+2.6	|	-2.1	|	±1.7	|	±1.6	|	±0.7	|	9.80E-04	|	3.00E-05	|	7.351E-02	|	+2.6	|	-2.1	|	±1.7	|	±1.6	|	±0.7	|	5.78E-03	|	0.00E+00	|
|	122.50	|	1.217E-02	|	+2.6	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	9.70E-04	|	3.00E-05	|	7.259E-02	|	+2.6	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	5.76E-03	|	0.00E+00	|
|	123.00	|	1.200E-02	|	+2.7	|	-2.1	|	±1.7	|	±1.6	|	±0.7	|	9.60E-04	|	3.00E-05	|	7.162E-02	|	+2.7	|	-2.1	|	±1.7	|	±1.6	|	±0.7	|	5.72E-03	|	0.00E+00	|
|	123.50	|	1.185E-02	|	+2.6	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	9.60E-04	|	3.00E-05	|	7.073E-02	|	+2.6	|	-2.2	|	±1.7	|	±1.6	|	±0.7	|	5.68E-03	|	0.00E+00	|
|	124.00	|	1.172E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.60E-04	|	3.00E-05	|	6.990E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.67E-03	|	0.00E+00	|
|	124.10	|	1.169E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.973E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.66E-03	|	0.00E+00	|
|	124.20	|	1.166E-02	|	+2.5	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.958E-02	|	+2.5	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.66E-03	|	0.00E+00	|
|	124.30	|	1.163E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.937E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.64E-03	|	0.00E+00	|
|	124.40	|	1.160E-02	|	+2.5	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.923E-02	|	+2.5	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.64E-03	|	0.00E+00	|
|	124.50	|	1.157E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.901E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.63E-03	|	0.00E+00	|
|	124.60	|	1.154E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.888E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.63E-03	|	0.00E+00	|
|	124.70	|	1.151E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.50E-04	|	3.00E-05	|	6.869E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.61E-03	|	0.00E+00	|
|	124.80	|	1.148E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.850E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.60E-03	|	0.00E+00	|
|	124.90	|	1.146E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.835E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.60E-03	|	0.00E+00	|
|	125.00	|	1.143E-02	|	+2.6	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.818E-02	|	+2.6	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	5.59E-03	|	0.00E+00	|
|	125.09	|	1.140E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.802E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.60E-03	|	0.00E+00	|
|	125.10	|	1.140E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.800E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.59E-03	|	0.00E+00	|
|	125.20	|	1.137E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.782E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.59E-03	|	0.00E+00	|
|	125.30	|	1.134E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.765E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.58E-03	|	0.00E+00	|
|	125.40	|	1.131E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.749E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.57E-03	|	0.00E+00	|
|	125.50	|	1.128E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.728E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.56E-03	|	0.00E+00	|
|	125.60	|	1.125E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.713E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.56E-03	|	0.00E+00	|
|	125.70	|	1.123E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.697E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.56E-03	|	0.00E+00	|
|	125.80	|	1.120E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.40E-04	|	3.00E-05	|	6.683E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.55E-03	|	0.00E+00	|
|	125.90	|	1.117E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.30E-04	|	3.00E-05	|	6.662E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.54E-03	|	0.00E+00	|
|	126.00	|	1.114E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.30E-04	|	3.00E-05	|	6.648E-02	|	+2.6	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.53E-03	|	0.00E+00	|
|	126.50	|	1.100E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.30E-04	|	3.00E-05	|	6.562E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.50E-03	|	0.00E+00	|
|	127.00	|	1.087E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.20E-04	|	3.00E-05	|	6.482E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.47E-03	|	0.00E+00	|
|	127.50	|	1.073E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.20E-04	|	3.00E-05	|	6.403E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.44E-03	|	0.00E+00	|
|	128.00	|	1.060E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.10E-04	|	3.00E-05	|	6.324E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.40E-03	|	0.00E+00	|
|	128.50	|	1.048E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.10E-04	|	3.00E-05	|	6.248E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.37E-03	|	0.00E+00	|
|	129.00	|	1.035E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	9.00E-04	|	3.00E-05	|	6.172E-02	|	+2.7	|	-2.3	|	±1.7	|	±1.6	|	±0.7	|	5.33E-03	|	0.00E+00	|
|	129.50	|	1.022E-02	|	+2.7	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	8.90E-04	|	3.00E-05	|	6.097E-02	|	+2.7	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	5.31E-03	|	0.00E+00	|
|	130.00	|	1.010E-02	|	+2.7	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	8.90E-04	|	3.00E-05	|	6.022E-02	|	+2.7	|	-2.4	|	±1.7	|	±1.6	|	±0.7	|	5.27E-03	|	0.00E+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	|	1.005E-01	|	+3.6	|	-9.3	|	±4.5	|	±3.9	|	±2.2	|
|	120.50	|	9.936E-02	|	+3.6	|	-9.3	|	±4.5	|	±3.9	|	±2.2	|
|	121.00	|	9.800E-02	|	+3.6	|	-9.3	|	±4.5	|	±3.9	|	±2.2	|
|	121.50	|	9.679E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	122.00	|	9.572E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	122.50	|	9.455E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	123.00	|	9.335E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	123.50	|	9.216E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.00	|	9.107E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.10	|	9.084E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.20	|	9.060E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.30	|	9.042E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.40	|	9.018E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.50	|	9.007E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.60	|	8.972E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.70	|	8.957E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.80	|	8.930E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	124.90	|	8.912E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.00	|	8.878E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.09	|	8.864E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.10	|	8.873E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.20	|	8.841E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.30	|	8.825E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.40	|	8.794E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.50	|	8.783E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.60	|	8.761E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.70	|	8.742E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.80	|	8.714E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	125.90	|	8.703E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	126.00	|	8.674E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	126.50	|	8.571E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	127.00	|	8.477E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	127.50	|	8.369E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	128.00	|	8.262E-02	|	+3.5	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	128.50	|	8.167E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	129.00	|	8.073E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	129.50	|	7.973E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
|	130.00	|	7.882E-02	|	+3.4	|	-9.2	|	±4.5	|	±3.9	|	±2.2	|
</tr>
</table>


---++ bbH  Process 
   * The cross  sections are the Santander matched numbers with 5FS (NNLO) and 4FS (NLO). No EW corrections. 
   * 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>) %  |
|	120.00	|	1.782E-01	|	+21.0	|	-22.8	|
|	120.50	|	1.762E-01	|	+21.0	|	-22.8	|
|	121.00	|	1.735E-01	|	+20.9	|	-22.7	|
|	121.50	|	1.710E-01	|	+20.9	|	-22.7	|
|	122.00	|	1.688E-01	|	+20.9	|	-22.7	|
|	122.50	|	1.663E-01	|	+20.8	|	-22.6	|
|	123.00	|	1.634E-01	|	+20.7	|	-22.5	|
|	123.50	|	1.619E-01	|	+20.7	|	-22.5	|
|	124.00	|	1.597E-01	|	+20.8	|	-22.6	|
|	124.10	|	1.591E-01	|	+20.8	|	-22.6	|
|	124.20	|	1.586E-01	|	+20.8	|	-22.6	|
|	124.30	|	1.583E-01	|	+20.8	|	-22.7	|
|	124.40	|	1.579E-01	|	+20.9	|	-22.7	|
|	124.50	|	1.573E-01	|	+20.7	|	-22.5	|
|	124.60	|	1.572E-01	|	+20.8	|	-22.5	|
|	124.70	|	1.564E-01	|	+20.8	|	-22.5	|
|	124.80	|	1.557E-01	|	+20.8	|	-22.6	|
|	124.90	|	1.555E-01	|	+20.8	|	-22.6	|
|	125.00	|	1.552E-01	|	+20.7	|	-22.4	|
|	125.09	|	1.545E-01	|	+20.7	|	-22.5	|
|	125.10	|	1.547E-01	|	+20.8	|	-22.5	|
|	125.20	|	1.543E-01	|	+20.8	|	-22.5	|
|	125.30	|	1.538E-01	|	+20.8	|	-22.5	|
|	125.40	|	1.532E-01	|	+20.8	|	-22.6	|
|	125.50	|	1.527E-01	|	+20.7	|	-22.4	|
|	125.60	|	1.524E-01	|	+20.6	|	-22.4	|
|	125.70	|	1.521E-01	|	+20.7	|	-22.5	|
|	125.80	|	1.514E-01	|	+20.7	|	-22.5	|
|	125.90	|	1.510E-01	|	+20.8	|	-22.5	|
|	126.00	|	1.508E-01	|	+20.7	|	-22.3	|
|	126.50	|	1.486E-01	|	+20.6	|	-22.3	|
|	127.00	|	1.467E-01	|	+20.6	|	-22.3	|
|	127.50	|	1.446E-01	|	+20.5	|	-22.2	|
|	128.00	|	1.425E-01	|	+20.4	|	-22.2	|
|	128.50	|	1.406E-01	|	+20.4	|	-22.2	|
|	129.00	|	1.389E-01	|	+20.4	|	-22.1	|
|	129.50	|	1.370E-01	|	+20.4	|	-22.1	|
|	130.00	|	1.351E-01	|	+20.3	|	-22.1	|
</tr>
</table>


---++ 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	|	1.289E-02	|	+7.6	|	-16.6	|	±4.9	|	±4.7	|	±1.5	|	8.880E-03	|	4.000E-03	|
|	120.50	|	1.281E-02	|	+7.5	|	-16.5	|	±4.9	|	±4.7	|	±1.5	|	8.830E-03	|	3.970E-03	|
|	121.00	|	1.273E-02	|	+7.6	|	-16.5	|	±4.9	|	±4.7	|	±1.5	|	8.780E-03	|	3.950E-03	|
|	121.50	|	1.267E-02	|	+7.5	|	-16.6	|	±4.9	|	±4.7	|	±1.5	|	8.730E-03	|	3.930E-03	|
|	122.00	|	1.260E-02	|	+7.5	|	-16.6	|	±4.9	|	±4.7	|	±1.5	|	8.690E-03	|	3.920E-03	|
|	122.50	|	1.254E-02	|	+7.5	|	-16.8	|	±4.9	|	±4.7	|	±1.5	|	8.630E-03	|	3.890E-03	|
|	123.00	|	1.247E-02	|	+7.5	|	-16.7	|	±4.9	|	±4.7	|	±1.5	|	8.600E-03	|	3.880E-03	|
|	123.50	|	1.241E-02	|	+7.4	|	-16.8	|	±4.9	|	±4.7	|	±1.5	|	8.550E-03	|	3.860E-03	|
|	124.00	|	1.236E-02	|	+7.4	|	-17.0	|	±4.9	|	±4.7	|	±1.5	|	8.510E-03	|	3.840E-03	|
|	124.10	|	1.235E-02	|	+7.4	|	-16.9	|	±4.9	|	±4.7	|	±1.5	|	8.510E-03	|	3.840E-03	|
|	124.20	|	1.235E-02	|	+7.4	|	-17.0	|	±4.9	|	±4.7	|	±1.5	|	8.500E-03	|	3.830E-03	|
|	124.30	|	1.233E-02	|	+7.4	|	-17.0	|	±4.9	|	±4.7	|	±1.5	|	8.500E-03	|	3.830E-03	|
|	124.40	|	1.231E-02	|	+7.4	|	-17.0	|	±4.9	|	±4.7	|	±1.5	|	8.500E-03	|	3.830E-03	|
|	124.50	|	1.228E-02	|	+7.4	|	-16.9	|	±4.9	|	±4.7	|	±1.5	|	8.460E-03	|	3.820E-03	|
|	124.60	|	1.228E-02	|	+7.4	|	-16.8	|	±4.9	|	±4.7	|	±1.5	|	8.470E-03	|	3.820E-03	|
|	124.70	|	1.226E-02	|	+7.4	|	-16.8	|	±4.9	|	±4.7	|	±1.5	|	8.470E-03	|	3.810E-03	|
|	124.80	|	1.225E-02	|	+7.4	|	-16.8	|	±4.9	|	±4.7	|	±1.5	|	8.440E-03	|	3.810E-03	|
|	124.90	|	1.223E-02	|	+7.4	|	-16.8	|	±4.9	|	±4.7	|	±1.5	|	8.430E-03	|	3.800E-03	|
|	125.00	|	1.226E-02	|	+7.3	|	-17.2	|	±4.9	|	±4.7	|	±1.5	|	8.430E-03	|	3.800E-03	|
|	125.09	|	1.223E-02	|	+7.4	|	-17.0	|	±5.0	|	±4.7	|	±1.5	|	8.420E-03	|	3.800E-03	|
|	125.10	|	1.223E-02	|	+7.4	|	-17.0	|	±5.0	|	±4.7	|	±1.5	|	8.420E-03	|	3.800E-03	|
|	125.20	|	1.222E-02	|	+7.3	|	-16.9	|	±5.0	|	±4.7	|	±1.5	|	8.410E-03	|	3.800E-03	|
|	125.30	|	1.221E-02	|	+7.4	|	-16.9	|	±5.0	|	±4.7	|	±1.5	|	8.410E-03	|	3.790E-03	|
|	125.40	|	1.217E-02	|	+7.4	|	-16.8	|	±5.0	|	±4.7	|	±1.5	|	8.400E-03	|	3.790E-03	|
|	125.50	|	1.219E-02	|	+7.4	|	-17.0	|	±5.0	|	±4.7	|	±1.5	|	8.400E-03	|	3.790E-03	|
|	125.60	|	1.218E-02	|	+7.3	|	-17.1	|	±5.0	|	±4.7	|	±1.5	|	8.390E-03	|	3.780E-03	|
|	125.70	|	1.216E-02	|	+7.3	|	-17.0	|	±5.0	|	±4.7	|	±1.5	|	8.380E-03	|	3.780E-03	|
|	125.80	|	1.214E-02	|	+7.4	|	-16.8	|	±5.0	|	±4.7	|	±1.5	|	8.360E-03	|	3.780E-03	|
|	125.90	|	1.213E-02	|	+7.3	|	-17.0	|	±5.0	|	±4.7	|	±1.5	|	8.350E-03	|	3.770E-03	|
|	126.00	|	1.213E-02	|	+7.3	|	-17.0	|	±5.0	|	±4.7	|	±1.5	|	8.340E-03	|	3.770E-03	|
|	126.50	|	1.207E-02	|	+7.3	|	-17.1	|	±5.0	|	±4.7	|	±1.5	|	8.320E-03	|	3.750E-03	|
|	127.00	|	1.199E-02	|	+7.3	|	-17.1	|	±5.0	|	±4.7	|	±1.5	|	8.270E-03	|	3.740E-03	|
|	127.50	|	1.197E-02	|	+7.3	|	-17.1	|	±5.0	|	±4.7	|	±1.5	|	8.240E-03	|	3.720E-03	|
|	128.00	|	1.190E-02	|	+7.2	|	-17.2	|	±5.0	|	±4.7	|	±1.5	|	8.200E-03	|	3.700E-03	|
|	128.50	|	1.185E-02	|	+7.2	|	-17.5	|	±5.0	|	±4.8	|	±1.5	|	8.160E-03	|	3.690E-03	|
|	129.00	|	1.178E-02	|	+7.3	|	-17.2	|	±5.0	|	±4.8	|	±1.5	|	8.120E-03	|	3.670E-03	|
|	129.50	|	1.174E-02	|	+7.2	|	-17.4	|	±5.0	|	±4.8	|	±1.5	|	8.080E-03	|	3.660E-03	|
|	130.00	|	1.167E-02	|	+7.2	|	-17.4	|	±5.0	|	±4.8	|	±1.5	|	8.040E-03	|	3.650E-03	|
</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	|	1.028E-03	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	7.090E-04	|	3.190E-04	|
|	120.50	|	1.018E-03	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	7.030E-04	|	3.150E-04	|
|	121.00	|	1.008E-03	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.960E-04	|	3.110E-04	|
|	121.50	|	1.000E-03	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.890E-04	|	3.090E-04	|
|	122.00	|	9.870E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.820E-04	|	3.050E-04	|
|	122.50	|	9.780E-04	|	+2.8	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.760E-04	|	3.020E-04	|
|	123.00	|	9.690E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.690E-04	|	2.990E-04	|
|	123.50	|	9.600E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.630E-04	|	2.960E-04	|
|	124.00	|	9.490E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.550E-04	|	2.930E-04	|
|	124.10	|	9.470E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.540E-04	|	2.920E-04	|
|	124.20	|	9.430E-04	|	+2.8	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.530E-04	|	2.910E-04	|
|	124.30	|	9.430E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.520E-04	|	2.910E-04	|
|	124.40	|	9.410E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.510E-04	|	2.900E-04	|
|	124.50	|	9.390E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.500E-04	|	2.900E-04	|
|	124.60	|	9.370E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.480E-04	|	2.890E-04	|
|	124.70	|	9.350E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.470E-04	|	2.880E-04	|
|	124.80	|	9.340E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.450E-04	|	2.880E-04	|
|	124.90	|	9.330E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.440E-04	|	2.870E-04	|
|	125.00	|	9.300E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.420E-04	|	2.870E-04	|
|	125.09	|	9.290E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.420E-04	|	2.860E-04	|
|	125.10	|	9.290E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.420E-04	|	2.860E-04	|
|	125.20	|	9.250E-04	|	+2.8	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.410E-04	|	2.850E-04	|
|	125.30	|	9.250E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.400E-04	|	2.850E-04	|
|	125.40	|	9.220E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.380E-04	|	2.840E-04	|
|	125.50	|	9.210E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.380E-04	|	2.840E-04	|
|	125.60	|	9.190E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.360E-04	|	2.830E-04	|
|	125.70	|	9.170E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.340E-04	|	2.830E-04	|
|	125.80	|	9.160E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.330E-04	|	2.820E-04	|
|	125.90	|	9.140E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.320E-04	|	2.810E-04	|
|	126.00	|	9.120E-04	|	+2.9	|	-2.5	|	±3.0	|	±3.0	|	±0.0	|	6.300E-04	|	2.800E-04	|
|	126.50	|	9.030E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.250E-04	|	2.780E-04	|
|	127.00	|	8.940E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.190E-04	|	2.750E-04	|
|	127.50	|	8.850E-04	|	+2.9	|	-2.6	|	±3.0	|	±3.0	|	±0.0	|	6.130E-04	|	2.720E-04	|
|	128.00	|	8.750E-04	|	+2.9	|	-2.5	|	±3.1	|	±3.1	|	±0.0	|	6.070E-04	|	2.700E-04	|
|	128.50	|	8.690E-04	|	+2.9	|	-2.6	|	±3.1	|	±3.1	|	±0.0	|	6.010E-04	|	2.670E-04	|
|	129.00	|	8.600E-04	|	+2.9	|	-2.6	|	±3.1	|	±3.1	|	±0.0	|	5.950E-04	|	2.640E-04	|
|	129.50	|	8.520E-04	|	+2.9	|	-2.6	|	±3.1	|	±3.1	|	±0.0	|	5.890E-04	|	2.620E-04	|
|	130.00	|	8.430E-04	|	+2.9	|	-2.6	|	±3.1	|	±3.1	|	±0.0	|	5.850E-04	|	2.590E-04	|
</tr>
</table>

-- Main.ReiTanaka - 2016-03-01
Topic revision: r18 - 2016-07-02 - ReiTanaka
LHCPhysics
LHCPhysics Web
LHCPhysics.Higgs
Public webs
- Cern Search
- TWiki Search
- Google Search
LHCPhysics All webs
Copyright &© 2008-2021 by the contributing authors. All material on this collaboration platform is the property of the contributing authors.
or Ideas, requests, problems regarding TWiki? use Discourse or Send feedback