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Higgs cross sections for HLLHC and HELHC 
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PDF+α_{s} uncertainties are according to PDF4LHC recipe. a) Numbers in complexpolescheme with NNLO+NNLL QCD + NLO EW corrections (D. de Florian, G. Passarino) . b) Higgs width zerowidth approximation, same as CERN Report 1, with NNLO QCD + NLO EW corrections. (D. Rebuzzi)  
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< <  c) Higgs width Zerowidth approximation, with NNLO QCD + NLO EW (WH/ZH) and NLO QCD corrections (ttH). Numbers from CERN2011002, Table 39, and TWiki page summary.  
> >  c) Higgs width Zerowidth approximation, with NNLO QCD + NLO EW (WH/ZH) and NLO QCD corrections (ttH). Numbers from CERN2011002, Table 39, and TWiki page summary.  
d) The cross section is the Santander matched numbers with 5FS (NNLO, R. Harlander) and 4FS (NLO, M. Spira) (see Section 12.2.2 in CERN Report 2).
SM Higgs production cross sections at √s = 33 TeV (M_{H}=125, 800 GeV)  
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SM Higgs decay branching ratio (M_{H}=125GeV)  
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2. Higgs cross sections and branching ratios for HL/HELHC  
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SM Higgs production cross sections at √s = 14 TeV (M_{H}=125, 800 GeV) 
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Higgs cross sections for HLLHC and HELHC 
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Monte Carlo  
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6. Plots
 
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Figure 1: Higgsboson production cross sections as a function of centreofmass energies.
 
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< <  Figure 1: Standard Model process cross sections at hadron colliders as a function of centreofmass energy (left), cross sections for SM and BSM particles as a function of mass at √s = 7 TeV (right). More plots for 8 and 33 TeV to come. (J. Stirling, see also here).  
> >  Figure 2: Standard Model process cross sections at hadron colliders as a function of centreofmass energy (left), cross sections for SM and BSM particles as a function of mass at √s = 7 TeV (right). More plots for 8 and 33 TeV to come. (J. Stirling, see also here).  
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< <  Figure 2: The ratio of parton luminosities between 7, 8, 14 and 33 TeV. (J. Stirling, see also here).
 
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a) Numbers in complexpolescheme with NNLO+NNLL QCD + NLO EW corrections (D. de Florian, G. Passarino) . b) Higgs width zerowidth approximation, same as CERN Report 1, with NNLO QCD + NLO EW corrections. (D. Rebuzzi) c) Higgs width Zerowidth approximation, with NNLO QCD + NLO EW (WH/ZH) and NLO QCD corrections (ttH). Numbers from CERN2011002, Table 39, and TWiki page summary.  
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< <  d) The cross section is the Santander matched numbers with 5FS (NNLO, R. Harlander) and 4FS (NLO, M. Spira) (see Section 12.2.2 in CERN Report 2) with mb=4.75 GeV.  
> >  d) The cross section is the Santander matched numbers with 5FS (NNLO, R. Harlander) and 4FS (NLO, M. Spira) (see Section 12.2.2 in CERN Report 2).  
SM Higgs production cross sections at √s = 33 TeV (M_{H}=125, 800 GeV) 
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PDF+α_{s} uncertainties are according to PDF4LHC recipe. a) Numbers in complexpolescheme with NNLO+NNLL QCD + NLO EW corrections (D. de Florian, G. Passarino) . b) Higgs width zerowidth approximation, same as CERN Report 1, with NNLO QCD + NLO EW corrections. (D. Rebuzzi)  
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< <  c) Higgs width Zerowidth approximation, with NNLO QCD + NLO EW (WH/ZH) and NLO QCD corrections (ttH). Numbers from CERN2011002, Table 39, and TWiki page summary.  
> >  c) Higgs width Zerowidth approximation, with NNLO QCD + NLO EW (WH/ZH) and NLO QCD corrections (ttH). Numbers from CERN2011002, Table 39, and TWiki page summary. d) The cross section is the Santander matched numbers with 5FS (NNLO, R. Harlander) and 4FS (NLO, M. Spira) (see Section 12.2.2 in CERN Report 2) with mb=4.75 GeV.  
SM Higgs production cross sections at √s = 33 TeV (M_{H}=125, 800 GeV)  
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PDF+α_{s} uncertainties are according to PDF4LHC recipe. a) Numbers in complexpolescheme with NNLO+NNLL QCD + NLO EW corrections (D. de Florian, G. Passarino). b) Higgs width zerowidth approximation, same as CERN Report 1, with NNLO QCD + NLO EW corrections (D. Rebuzzi) c) NNLO QCD + NLO EW corrections (R. Harlander).  
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< <  d) NLO QCD. (M. Spira).  
> >  d) NLO QCD. (M. Spira). e) NNLO QCD in 5FS (R. Harlander).  
SM Higgspair (triple) production cross sections at √s = 7 and 8 TeV (M_{H}=125GeV)  
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PDF is NNLO(NLO) MSTW2008 set. Numbers in () parentheses are the crosssection ratio wrt 14 TeV. a) NNLO+NNLL QCD + NLO EW corrections. QCD scale and PDF+α_{s} uncertainties remain constant about +8% for both (D. de Florian). b) NNLO QCD only with VBF@NNLO (M. Zaro). c) NNLO QCD only with VH@NNLO (R. Harlander). d) NLO QCD. (M. Spira).  
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< <  e) NLO QCD with HPAIR. The central scale is the invariant mass of the Higgs pair. The scale is varied by a factor 2 up and down. (M. Spira).  
> >  e) NNLO QCD in 5FS (R. Harlander). f) NLO QCD with HPAIR. The central scale is the invariant mass of the Higgs pair. The scale is varied by a factor 2 up and down. (M. Spira).  

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Higgs cross sections for HLLHC and HELHC
1. LHC acclerarator benchmark scenario
2. Higgs cross sections and branching ratios for HL/HELHC
SM Higgs production cross sections at √s = 14 TeV (M_{H}=125, 800 GeV)
a) Numbers in complexpolescheme with NNLO+NNLL QCD + NLO EW corrections (D. de Florian, G. Passarino) . b) Higgs width zerowidth approximation, same as CERN Report 1, with NNLO QCD + NLO EW corrections. (D. Rebuzzi) c) Higgs width Zerowidth approximation, with NNLO QCD + NLO EW (WH/ZH) and NLO QCD corrections (ttH). Numbers from CERN2011002, Table 39, and TWiki page summary.
SM Higgs production cross sections at √s = 33 TeV (M_{H}=125, 800 GeV)
a) Numbers in complexpolescheme with NNLO+NNLL QCD + NLO EW corrections (D. de Florian, G. Passarino). b) Higgs width zerowidth approximation, same as CERN Report 1, with NNLO QCD + NLO EW corrections (D. Rebuzzi) c) NNLO QCD + NLO EW corrections (R. Harlander). d) NLO QCD. (M. Spira).
SM Higgspair (triple) production cross sections at √s = 7 and 8 TeV (M_{H}=125GeV)
SM Higgspair (triple) production cross sections at √s = 14 and 33 TeV (M_{H}=125GeV)
SM Higgs decay branching ratio (M_{H}=125GeV)
3. Major SM background process cross sections
ttbar cross section at √s = 8, 14 and 33 TeV
4. Higgs cross sections for HELHC
SM Higgs production cross sections at √s = 14, 33, 40, 60, 80 and 100 TeV (M_{H}=125 GeV)
a) NNLO+NNLL QCD + NLO EW corrections. QCD scale and PDF+α_{s} uncertainties remain constant about +8% for both (D. de Florian). b) NNLO QCD only with VBF@NNLO (M. Zaro). c) NNLO QCD only with VH@NNLO (R. Harlander). d) NLO QCD. (M. Spira). e) NLO QCD with HPAIR. The central scale is the invariant mass of the Higgs pair. The scale is varied by a factor 2 up and down. (M. Spira).
a) OpenLoops+Sherpa, NLO QCD corrections only, with dynamical renormalization scale set to the virtuality of the intermediate vector boson. gg → ZH is not included (F. Cascioli, J. Thompson). b) OpenLoops+Sherpa, NLO QCD corrections only, with μ_{R} = M_{top} + M_{H}/2 (F. Cascioli, J. Thompson).
Figure : Parton luminosity and ratio for Ecms=14, 40, 60, 80 and 100 TeV. (J. Stirling, see also here).
5. Tools
Monte Carlo
6. Plots
Figure 2: The ratio of parton luminosities between 7, 8, 14 and 33 TeV. (J. Stirling, see also here).
Figure 4: Higgsboson pair production cross section in gg→HH as a function of Higgsboson mass at centreofmass energies at 14 and 33 TeV (M. Spira).
6. References
 ReiTanaka  19 Dec 2013 