\begin{table}[b]
{\centering\small
\begin{tabular}{llllll}
\toprule
             & ggF & VBF & VH \\
\midrule
0/1 jet [\%] & $0.945$ & $2.101$ & $1.702$\\
VBF [\%]     & $0.026$ & $0.979$ & $0.023$\\
\bottomrule
\end{tabular}\par}
\caption{Selection efficiencies for the different Higgs production mechanisms in
  the $H\to\tau\tau$ event categories defined by CMS \cite{CMS-PAS-HIG-12-043}
  (see also Fig.~\ref{fig:signalstrengths}). The columns stand for gluon fusion
  (ggF), vector boson fusion (VBF) and $WH$ or $ZH$ associated production (VH).}
\label{tab:tautaueff}
\end{table}
%
%
%
\begin{table}[p!]
{\centering\small
\begin{tabular}{lllllll}
\toprule
& & ggF & VBF & WH & ZH & ttH \\
\midrule
ATLAS 7 TeV & ucl & $0.929$ & $0.040$ & $0.018$ & $0.010$ & $0.002$\\
& uch & $0.665$ & $0.157$ & $0.099$ & $0.057$ & $0.024$\\
& url & $0.928$ & $0.039$ & $0.020$ & $0.011$ & $0.002$\\
& urh & $0.654$ & $0.161$ & $0.108$ & $0.061$ & $0.018$\\
& ccl & $0.928$ & $0.040$ & $0.019$ & $0.010$ & $0.002$\\
& cch & $0.666$ & $0.153$ & $0.100$ & $0.057$ & $0.025$\\
& crl & $0.928$ & $0.038$ & $0.020$ & $0.011$ & $0.002$\\
& crh & $0.653$ & $0.160$ & $0.110$ & $0.059$ & $0.018$\\
& ct & $0.894$ & $0.052$ & $0.033$ & $0.017$ & $0.003$\\
& jj & $0.225$ & $0.767$ & $0.004$ & $0.002$ & $0.001$\\
\midrule
ATLAS 8 TeV & ucl & $0.937$ & $0.040$ & $0.014$ & $0.008$ & $0.002$\\
& uch & $0.793$ & $0.126$ & $0.041$ & $0.025$ & $0.014$\\
& url & $0.932$ & $0.040$ & $0.016$ & $0.010$ & $0.001$\\
& urh & $0.781$ & $0.133$ & $0.047$ & $0.028$ & $0.011$\\
& ccl & $0.936$ & $0.040$ & $0.013$ & $0.009$ & $0.002$\\
& cch & $0.789$ & $0.126$ & $0.043$ & $0.027$ & $0.015$\\
& crl & $0.932$ & $0.041$ & $0.016$ & $0.010$ & $0.001$\\
& crh & $0.777$ & $0.130$ & $0.052$ & $0.030$ & $0.011$\\
& ct & $0.907$ & $0.055$ & $0.022$ & $0.013$ & $0.002$\\
& lhm2j & $0.450$ & $0.541$ & $0.005$ & $0.003$ & $0.001$\\
& thm2j & $0.238$ & $0.760$ & $0.001$ & $0.001$ & $0.000$\\
& lm2j & $0.481$ & $0.030$ & $0.297$ & $0.172$ & $0.019$\\
& etmiss & $0.041$ & $0.005$ & $0.357$ & $0.476$ & $0.121$\\
& lept & $0.022$ & $0.006$ & $0.632$ & $0.154$ & $0.186$\\
\midrule
CMS 7 TeV & u0 & $0.614$ & $0.168$ & $0.121$ & $0.066$ & $0.031$\\
& u1 & $0.876$ & $0.062$ & $0.036$ & $0.020$ & $0.005$\\
& u2 & $0.913$ & $0.044$ & $0.025$ & $0.014$ & $0.003$\\
& u3 & $0.913$ & $0.044$ & $0.026$ & $0.015$ & $0.002$\\
& jj & $0.268$ & $0.725$ & $0.004$ & $0.002$ & $0.000$\\
\midrule
CMS 8 TeV & u0 & $0.729$ & $0.116$ & $0.082$ & $0.047$ & $0.026$\\
& u1 & $0.835$ & $0.084$ & $0.045$ & $0.026$ & $0.010$\\
& u2 & $0.916$ & $0.045$ & $0.023$ & $0.013$ & $0.004$\\
& u3 & $0.925$ & $0.039$ & $0.021$ & $0.012$ & $0.003$\\
& jj t & $0.207$ & $0.789$ & $0.002$ & $0.001$ & $0.001$\\
& jj l & $0.470$ & $0.509$ & $0.011$ & $0.006$ & $0.005$\\
& mu & $0.000$ & $0.002$ & $0.504$ & $0.286$ & $0.208$\\
& e & $0.011$ & $0.004$ & $0.502$ & $0.285$ & $0.198$\\
& Etmiss & $0.220$ & $0.026$ & $0.407$ & $0.230$ & $0.117$\\
\bottomrule
\end{tabular}\par}
\caption{Fractional contributions of the different Higgs production mechanisms
  to the $H\to\gamma\gamma$ event categories defined by ATLAS and CMS. The
  numbers and category labels are from
  \cite{ATLAS-CONF-2012-091a,ATLAS-CONF-2013-012,CMS-PAS-HIG-13-001} (see also
  Fig.~\ref{fig:signalstrengths}).  The columns stand for gluon fusion (ggF),
  vector boson fusion (VBF), $WH$ associated production (WH), $ZH$ associated
  production (ZH) and $t\bar tH$ associated production (ttH).}
\label{tab:pcvalues}
\end{table}
%
%
%
\begin{figure}[p!]
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    \Text(100,430)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegccl",1.391,1.043,-0.951},
    \Text(-65,420)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny ccl}}=1.391 ^{+1.043} {}_{-0.951}$}}
    \Text(100,420)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegcrh",1.299,1.320,-1.274},
    \Text(-65,410)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny crh}}=1.299 ^{+1.320} {}_{-1.274}$}}
    \Text(100,410)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegcrl",2.220,1.166,-0.997},
    \Text(-65,400)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny crl}}=2.220 ^{+1.166} {}_{-0.997}$}}
    \Text(100,400)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegct",2.818,1.688,-1.596},
    \Text(-65,390)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny ct}}=2.818 ^{+1.688} {}_{-1.596}$}}
    \Text(100,390)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAeglhm2j",2.772,1.780,-1.381},
    \Text(-65,380)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny lhmjj}}=2.772 ^{+1.780} {}_{-1.381}$}}
    \Text(100,380)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAeglm2j",0.332,1.734,-1.458},
    \Text(-65,370)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny lmjj}}=0.332 ^{+1.734} {}_{-1.458}$}}
    \Text(100,370)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegET",2.987,2.716,-2.164},
    \Text(-65,360)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny $\fmslash{E}_{\rm T}$}}=2.987 ^{+2.716} {}_{-2.164}$}}
    \Text(100,360)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegthm2j",1.621,0.829,-0.675},
    \Text(-65,350)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny thmjj}}=1.621 ^{+0.829} {}_{-0.675}$}}
    \Text(100,350)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAeguch",0.962,1.090,-0.936},
    \Text(-65,340)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny uch}}=0.962 ^{+1.090} {}_{-0.936}$}}
    \Text(100,340)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegucl",0.885,0.721,-0.706},
    \Text(-65,330)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny ucl}}=0.885 ^{+0.721} {}_{-0.706}$}}
    \Text(100,330)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegurh",2.711,1.350,-1.151},
    \Text(-65,320)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny urh}}=2.711 ^{+1.350} {}_{-1.151}$}}
    \Text(100,320)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAegurl",2.527,0.921,-0.783},
    \Text(-65,310)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \gamma \gamma )_{\text{\tiny url}}=2.527 ^{+0.921} {}_{-0.783}$}}
    \Text(100,310)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-012}}}
% {"ssAet",0.756,0.775,-0.745},
    \Text(-65,300)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to \tau \tau )=0.756 ^{+0.775} {}_{-0.745}$}}
    \Text(100,300)[cl]{\Black{\scriptsize \cite{Aad:2012an,ATLAS-CONF-2012-160}}}
% {"ssAeW",1.26,0.35},
    \Text(-65,290)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to WW)=1.26 \pm 0.35$}}
    \Text(100,290)[cl]{\Black{\scriptsize \cite{ATLAS-CONF-2013-030}}}
% {"ssAeZ",1.603,0.423,-0.459},
    \Text(-65,280)[cl]{\Black{\scriptsize $\mu ^{\rm A8}(H\to ZZ)=1.603 ^{+0.423} {}_{-0.459}$}}
    \Text(100,280)[cl]{\Black{\scriptsize \cite{Aad:2012an,ATLAS-CONF-2013-013}}}
% {"ssCsbtt",-0.729,2.018,-1.853},
    \Text(-65,270)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(t\bar t\to H\to b\bar b)=-0.729 ^{+2.018} {}_{-1.853}$}}
    \Text(100,270)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020}}}
% {"ssCsb",0.588,1.235,-1.153},
    \Text(-65,260)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(VH\to Vb\bar b)=0.588 ^{+1.235} {}_{-1.153}$}}
    \Text(100,260)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020}}}
% {"ssCsg0",3.832,2.042,-1.671},
    \Text(-65,250)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \gamma \gamma )_{\text{\tiny u0}}=3.832 ^{+2.042} {}_{-1.671}$}}
    \Text(100,250)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCsg1",0.193,1.002,-0.965},
    \Text(-65,240)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \gamma \gamma )_{\text{\tiny u1}}=0.193 ^{+1.002} {}_{-0.965}$}}
    \Text(100,240)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCsg2",0.045,1.262},
    \Text(-65,230)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \gamma \gamma )_{\text{\tiny u2}}=0.045 \pm 1.262$}}
    \Text(100,230)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCsg3",1.493,1.634},
    \Text(-65,220)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \gamma \gamma )_{\text{\tiny u3}}=1.493 \pm 1.634$}}
    \Text(100,220)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCsgjj",4.203,2.339,-1.782},
    \Text(-65,210)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \gamma \gamma )_{\text{\tiny jj}}=4.203 ^{+2.339} {}_{-1.782}$}}
    \Text(100,210)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCstjet",1.000,1.441,-1.400},
    \Text(-65,200)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \tau \tau )_{\text{\tiny 0/1 jet}}=1.000 ^{+1.441} {}_{-1.400}$}}
    \Text(100,200)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020}}}
% {"ssCstVBF",-1.718,1.318,-1.153},
    \Text(-65,190)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \tau \tau )_{\text{\tiny VBF}}=-1.718 ^{+1.318} {}_{-1.153}$}}
    \Text(100,190)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020}}}
% {"ssCstVH",0.671,4.076,-3.047},
    \Text(-65,180)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to \tau \tau )_{\text{\tiny VH}}=0.671 ^{+4.076} {}_{-3.047}$}}
    \Text(100,180)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020}}}
% {"ssCsW",0.726,0.417,-0.412},
    \Text(-65,170)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to WW)=0.726 ^{+0.417} {}_{-0.412}$}}
    \Text(100,170)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-003}}}
% {"ssCsZ",0.671,0.700,-0.494},
    \Text(-65,160)[cl]{\Black{\scriptsize $\mu ^{\rm C7}(H\to ZZ)=0.671 ^{+0.700} {}_{-0.494}$}}
    \Text(100,160)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020}}}
% {"ssCeb",1.584,0.771,-0.704},
    \Text(-65,150)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(VH\to Vb\bar b)=1.584 ^{+0.771} {}_{-0.704}$}}
    \Text(100,150)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020,CMS-PAS-HIG-12-045}}}
% {"ssCeg0",2.198,0.928,-0.817},
    \Text(-65,140)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny u0}}=2.198 ^{+0.928} {}_{-0.817}$}}
    \Text(100,140)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCeg1",0.045,0.705},
    \Text(-65,130)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny u1}}=0.045 \pm 0.705$}}
    \Text(100,130)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCeg2",0.304,0.483},
    \Text(-65,120)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny u2}}=0.304 \pm 0.483$}}
    \Text(100,120)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCeg3",-0.327,0.817,-0.854},
    \Text(-65,110)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny u3}}=-0.327 ^{+0.817} {}_{-0.854}$}}
    \Text(100,110)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCege",-0.661,2.785,-1.968},
    \Text(-65,100)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny $e$}}=-0.661 ^{+2.785} {}_{-1.968}$}}
    \Text(100,100)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCegjjl",0.824,1.077,-1.002},
    \Text(-65,90)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny jj loose}}=0.824 ^{+1.077} {}_{-1.002}$}}
    \Text(100,90)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCegjjt",0.304,0.668,-0.594},
    \Text(-65,80)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny jj tight}}=0.304 ^{+0.668} {}_{-0.594}$}}
    \Text(100,80)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCegET",1.938,2.599,-2.339},
    \Text(-65,70)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny $\fmslash{E}_{\rm T}$}}=1.938 ^{+2.599} {}_{-2.339}$}}
    \Text(100,70)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCegm",0.416,1.819,-1.411},
    \Text(-65,60)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \gamma \gamma )_{\text{\tiny $\mu$}}=0.416 ^{+1.819} {}_{-1.411}$}}
    \Text(100,60)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-001}}}
% {"ssCetjet",1.109,0.416,-0.417},
    \Text(-65,50)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \tau \tau )_{\text{\tiny 0/1 jet}}=1.109 ^{+0.416} {}_{-0.417}$}}
    \Text(100,50)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020,CMS-PAS-HIG-13-004}}}
% {"ssCetVBF",2.375,0.674,-0.703},
    \Text(-65,40)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \tau \tau )_{\text{\tiny VBF}}=2.375 ^{+0.674} {}_{-0.703}$}}
    \Text(100,40)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020,CMS-PAS-HIG-13-004}}}
% {"ssCetVH",0.780,1.613,-1.723},
    \Text(-65,30)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to \tau \tau )_{\text{\tiny VH}}=0.780 ^{+1.613} {}_{-1.723}$}}
    \Text(100,30)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020,CMS-PAS-HIG-13-004}}}
% {"ssCeW",0.647,0.225,-0.221},
    \Text(-65,20)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to WW)=0.647 ^{+0.225} {}_{-0.221}$}}
    \Text(100,20)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-13-003}}}
% {"ssCeZ",0.975,0.332,-0.275}
    \Text(-65,10)[cl]{\Black{\scriptsize $\mu ^{\rm C8}(H\to ZZ)=0.975 ^{+0.332} {}_{-0.275}$}}
    \Text(100,10)[cl]{\Black{\scriptsize \cite{CMS-PAS-HIG-12-020,CMS-PAS-HIG-13-002}}}
    \Text(139,-3)[cb]{\Black{\scriptsize $-6$}}
    \Text(159,-3)[cb]{\Black{\scriptsize $-4$}}
    \Text(179,-3)[cb]{\Black{\scriptsize $-2$}}
    \Text(200.7,-3)[cb]{\Black{\scriptsize $0$}}
    \Text(221,-3)[cb]{\Black{\scriptsize $2$}}
    \Text(241,-3)[cb]{\Black{\scriptsize $4$}}
    \Text(261,-3)[cb]{\Black{\scriptsize $6$}}
    \Text(281,-3)[cb]{\Black{\scriptsize $8$}}
    \Text(301.7,-3)[cb]{\Black{\scriptsize $10$}}
    \Text(321.7,-3)[cb]{\Black{\scriptsize $12$}}
    \Text(341.7,-3)[cb]{\Black{\scriptsize $14$}}
%     \put(290,80){\includegraphics[width=0.13\linewidth]{Images/CKMfitterPackage.eps}}
\end{picture}
\caption{Higgs signal strengths measured by D0, CDF, ATLAS and CMS. The
  superscripts T, A7, A8, C7 and C8 refer to Tevatron, ATLAS \unit{7}{TeV},
  ATLAS \unit{8}{TeV}, CMS \unit{7}{TeV} and CMS \unit{8}{TeV} data,
  respectively. The subscripts jj, cch etc.\ denote the different event
  categories defined by ATLAS and CMS. The combination of all signal strengths
  yields $\mu _{\text{combined}}=1.007 ^{+0.099} {}_{-0.098}$ and is
  illustrated by the green band.}
\label{fig:signalstrengths}
\end{figure}

