| 1 |
vimartin |
1.1 |
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| 2 |
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%Note to authors: these definitions are suggested to be used for consistency
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%\newcommand{\pt}{$p_T$ }
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%\newcommand{\GeVc}{GeV/c}
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%\newcommand{\mll}{\ensuremath{M_{\ell\ell}}}
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%\newcommand{\z}{$Z$ }
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%\newcommand{\zjets}{$Z+\rm{jets}$ }
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%\newcommand{\gjets}{$\gamma+\rm{jets}$ }
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%\newcommand{\Z}{$Z$ } %redundancy can be good
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%\newcommand{\ase}[2]{\ensuremath{_{~- #1}^{~+ #2}}}
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%\newcommand{\MET}{\ensuremath{\rm{E_{T}^{miss}}}}
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%\newcommand{\mt}{\ensuremath{M_T}}
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%\newcommand{\met}{\mbox{$\raisebox{.3ex}{$\not$}E_T$\hspace*{0.5ex}}}
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%\newcommand{\effr}{$R_{e\mu}$} %used to be \epsilon
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%\newcommand{\effrm}{$R_{\mu e}$} %used to be \epsilon
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%\newcommand{\sta}{$\sigma\times A$} %notation is such that A includes BR
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%\newcommand{\statistics}{CL$_\mathrm{S}$}
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\newcommand{\njets}{$N_{\rm{jets}}$}
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%\newcommand{\lumi}{4.98~fb$^{-1}$}
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%\newcommand{\wjets}{$\rm{W}+{\rm jets}$}
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%\newcommand{\zzmet}{$\rm{ZZ}+\MET$}
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%\newcommand{\wzmet}{$\rm{WZ}+\MET$}
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%\newcommand{\wzzmet}{$\rm{WZ/ZZ}+\MET$}
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%\newcommand{\cls} {\ensuremath{\mathrm{CL_S}}}
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\newcommand{\CLs}{\ensuremath{CL_\mathrm{s}}}
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\newcommand{\CLb}{\ensuremath{CL_\mathrm{b}}}
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\newcommand{\CLsb}{\ensuremath{CL_\mathrm{s+b}}}
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| 29 |
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| 30 |
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\newcommand{\GeV}{\ensuremath{\mathrm{Ge\kern -0.1em V}}}
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\newcommand{\TeV}{\ensuremath{\mathrm{Te\kern -0.1em V}}}
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\newcommand{\TeVcc}{\ensuremath{\,\mathrm{Te\kern -0.1em V\!/c}^2}}
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\newcommand{\GeVcc}{\ensuremath{\,\mathrm{Ge\kern -0.1em V\!/c}^2}}
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\newcommand{\MeVcc}{\ensuremath{\,\mathrm{Me\kern -0.1em V\!/c}^2}}
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\newcommand{\GeVc}{\ensuremath{\mathrm{Ge\kern -0.1em V}\!/c}}
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\newcommand{\nanob}{\mbox{{\rm ~nb}~}}
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\newcommand{\fb}{\ensuremath{\mathrm{fb}}}
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\newcommand{\pb}{\ensuremath{\mathrm{pb}}}
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\newcommand{\ifb}{\ensuremath{\mathrm{fb^{-1}}}}
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\newcommand{\ipb}{\ensuremath{\mathrm{pb^{-1}}}}
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\newcommand{\grad}{\ensuremath{^{\circ}}}
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%
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% Special user made math symbols
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%
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\newcommand{\lsim}{\raisebox{-1.5mm}{$\:\stackrel{\textstyle{<}}{\textstyle{\sim}}\:$}}
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\newcommand{\gsim}{\raisebox{-1.5mm}{$\:\stackrel{\textstyle{>}}{\textstyle{\sim}}\:$}}
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% particles
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\newcommand{\pipm}{\ensuremath{\pi^{\pm}}}
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\newcommand{\pizero}{\ensuremath{\pi^{0}}}
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\newcommand{\Hi}{\ensuremath{\mathrm{H}}}
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\newcommand{\W}{\ensuremath{\mathrm{W}}}
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\newcommand{\Wjets}{\ensuremath{\mathrm{W+jets}}}
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\newcommand{\Wfourj}{\ensuremath{\mathrm{W} + \ge 4 \mathrm{jets}}}
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\newcommand{\Zjets}{\ensuremath{\mathrm{Z+jets}}}
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\newcommand{\Wt}{\ensuremath{\mathrm{Wt}}}
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\newcommand{\Wstar}{\ensuremath{\mathrm{W}^{*}}}
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\newcommand{\Wparenthesisstar}{\ensuremath{\mathrm{W}^{(*)}}}
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\newcommand{\WW}{\ensuremath{\W^+\W^-}}
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\newcommand{\Z}{\ensuremath{\mathrm{Z}}}
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\newcommand{\Zstar}{\ensuremath{\mathrm{Z}^{*}}}
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\newcommand{\Astar}{\ensuremath{\mathrm{\gamma}^{*}}}
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\newcommand{\ZZ}{\ensuremath{\Z\Z}}
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\newcommand{\WZ}{\ensuremath{\W\Z}}
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\newcommand{\Wgstar}{\ensuremath{\W\Astar}}
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\newcommand{\E}{\ensuremath{\mathrm{e}}}
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\newcommand{\Ep}{\ensuremath{\mathrm{e}^{+}}}
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\newcommand{\Em}{\ensuremath{\mathrm{e}^{-}}}
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\newcommand{\Epm}{\ensuremath{\mathrm{e}^{\pm}}}
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\newcommand{\Emp}{\ensuremath{\mathrm{e}^{\mp}}}
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\newcommand{\M}{\ensuremath{\mu}}
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\newcommand{\Mp}{\ensuremath{\mu^{+}}}
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\newcommand{\Mm}{\ensuremath{\mu^{-}}}
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\newcommand{\Mpm}{\ensuremath{\mu^{\pm}}}
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\newcommand{\Mmp}{\ensuremath{\mu^{\mp}}}
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\newcommand{\Tau}{\ensuremath{\tau}}
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\newcommand{\Nu}{\ensuremath{\nu}}
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\newcommand{\Nubar}{\ensuremath{\bar{\nu}}}
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\newcommand{\Lep}{\ensuremath{\ell}}
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\newcommand{\Lepp}{\ensuremath{\ell^{+}}}
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\newcommand{\Lepm}{\ensuremath{\ell^{-}}}
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\newcommand{\Lprime}{\ensuremath{\Lep^{\prime}}}
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\newcommand{\Prot}{\ensuremath{\mathrm{p}}}
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\newcommand{\Pbar}{\ensuremath{\bar{\mathrm{p}}}}
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\newcommand{\PP}{\Prot\Prot}
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\newcommand{\PPbar}{\Prot\Pbar}
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vimartin |
1.3 |
\newcommand{\sctop}{\ensuremath{\tilde{t}}}
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| 89 |
vimartin |
1.1 |
\newcommand{\ttbar}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}}}
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\newcommand{\ttll}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}\to\ell\ell}}
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\newcommand{\ttlj}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}\to\ell+\rm{jets}}}
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vimartin |
1.3 |
\newcommand{\ttdl}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}\to\ell\ell}}
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\newcommand{\ttsl}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}\to\ell+\rm{jets}}}
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\newcommand{\ttlt}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}\to\ell\tau}}
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\newcommand{\ttlf}{\ensuremath{\mathrm{t}\bar{\mathrm{t}}\to\ell \mathrm{fake}}}
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vimartin |
1.1 |
%\newcommand{\emu }{\ensuremath{e\mu}}
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%\newcommand{\ee }{\ensuremath{ee}}
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%\newcommand{\eepm}{\ensuremath{e^+ e^-}}
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%\newcommand{\mm }{\ensuremath{\mu\mu}}
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%\newcommand{\mmpm}{\ensuremath{\mu^+ \mu^-}}
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%\newcommand{\empm}{\ensuremath{e^\pm \mu^\mp}}
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\newcommand{\qq}{\ensuremath{\mathrm{q}\mathrm{q}}}
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%\newcommand{\bbbar}{\ensuremath{\mathrm{b}\bar{\mathrm{b}}}}
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\newcommand{\Wtb}{\ensuremath{\W\mathrm{t}\mathrm{b}}}
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\newcommand{\Top}{\ensuremath{\mathrm{t}}}
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\newcommand{\Bot}{\ensuremath{\mathrm{b}}}
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\newcommand{\Atop}{\ensuremath{\bar{\mathrm{t}}}}
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\newcommand{\Abot}{\ensuremath{\bar{\mathrm{b}}}}
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% arrow
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\newcommand{\To}{\ensuremath{\rightarrow}}
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% masses
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vimartin |
1.3 |
\newcommand{\mHi}{\ensuremath{M_{\mathrm{H}}}}
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\newcommand{\mtop}{\ensuremath{M_{\mathrm{top}}}}
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\newcommand{\mW}{\ensuremath{M_{\mathrm{W}}}}
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\newcommand{\mZ}{\ensuremath{M_{\mathrm{Z}}}}
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\newcommand{\mll}{\ensuremath{M_{\Lep\Lep}}}
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benhoob |
1.2 |
\newcommand{\mt}{\ensuremath{M_{\mathrm{T}}}}
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vimartin |
1.1 |
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% kinematics
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\newcommand{\pt}{\ensuremath{p_\mathrm{T}}}
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\newcommand{\ptveto}{\ensuremath{\pt^\mathrm{veto}}}
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\newcommand{\ptl}{\ensuremath{p_\perp^{\Lep}}}
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\newcommand{\ptlmax}{\ensuremath{p_{\mathrm{T}}^{\Lep,\mathrm{max}}}}
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\newcommand{\ptlmin}{\ensuremath{p_{\mathrm{T}}^{\Lep,\mathrm{min}}}}
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\newcommand{\met}{\ensuremath{\Et^{\mathrm{miss}}}}
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\newcommand{\delphill}{\ensuremath{\Delta\phi_{\Lep\Lep}}}
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\newcommand{\deletall}{\ensuremath{\Delta\eta_{\Lep\Lep}}}
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\newcommand{\delphimetl}{\ensuremath{\Delta\phi_{\met\Lep}}}
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\newcommand{\Et}{\ensuremath{E_\mathrm{T}}}
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\newcommand{\delR}{\ensuremath{\Delta R}}
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\newcommand{\Eta}{\ensuremath{\eta}}
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%efficiencies
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\newcommand{\effsig}{\ensuremath{\varepsilon_{\mathrm{bkg}}^{\mathrm{S}}}}
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\newcommand{\effnorm}{\ensuremath{\varepsilon_{\mathrm{bkg}}^{\mathrm{N}}}}
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\newcommand{\Nsig}{\ensuremath{N_{\mathrm{bkg}}^{\mathrm{S}}}}
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\newcommand{\Nnorm}{\ensuremath{N_{\mathrm{bkg}}^{\mathrm{N}}}}
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% processes
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\newcommand{\dyee}{\ensuremath{Z/\gamma^*\to ee}}
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\newcommand{\dymm}{\ensuremath{Z/\gamma^*\to\mu\mu}}
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\newcommand{\dytt}{\ensuremath{Z/\gamma^*\to\tau\tau}}
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\newcommand{\dyll}{\ensuremath{Z/\gamma^*\to\ell\ell}}
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\newcommand{\dy}{\ensuremath{Z/\gamma^*}}
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\newcommand{\zee}{\ensuremath{Z\to ee}}
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\newcommand{\zmm}{\ensuremath{Z\to\mu\mu}}
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\newcommand{\ztt}{\ensuremath{Z\to\tau\tau}}
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%\newcommand{\ttbar}{\ensuremath{t\bar{t}}}
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\newcommand{\ppww}{\ensuremath{pp \to W^+W^-}}
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\newcommand{\wwll}{\ensuremath{WW\to \ell^+\ell^-}}
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\newcommand{\wwlnln}{\ensuremath{W^+W^-\to \ell^+\nu \ell^-\bar{\nu}}}
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\newcommand{\ww}{\ensuremath{WW}}
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\newcommand{\wwpm}{\ensuremath{W^+W^-}}
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\newcommand{\hww}{\ensuremath{H\to W^+W^-}}
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\newcommand{\wz}{\ensuremath{WZ}}
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\newcommand{\zz}{\ensuremath{ZZ}}
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\newcommand{\wgamma}{\ensuremath{W\gamma}}
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\newcommand{\wjets}{\ensuremath{W+}jets}
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| 161 |
vimartin |
1.3 |
\newcommand{\zjets}{\ensuremath{Z+}jets}
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| 162 |
vimartin |
1.1 |
\newcommand{\tw}{\ensuremath{tW}}
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\newcommand{\singletopt}{\ensuremath{t} ($t$-chan)}
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\newcommand{\singletops}{\ensuremath{t} ($s$-chan)}
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\newcommand{\zx}{\ensuremath{\mathrm{DY/WZ/ZZ}}}
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\newcommand{\zv}{\ensuremath{\mathrm{WZ/ZZ}}}
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vimartin |
1.3 |
\newcommand{\vv}{\ensuremath{\mathrm{WW/WZ/ZZ}}}
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\newcommand{\vvv}{\ensuremath{\mathrm{WWW/WWZ/WZZ/ZZZ}}}
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vimartin |
1.1 |
\newcommand{\z}{\ensuremath{\mathrm{Z}}}
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\newcommand{\routin}{\ensuremath{R_{out/in}}}
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%other
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\def\fixme{({\bf FixMe})}
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\newcommand{\ee}{\ensuremath{ee}}
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\newcommand{\emu}{\ensuremath{e\mu}}
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\def\mm{\ensuremath{\mu\mu}}
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% integrated luminosity
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vimartin |
1.3 |
\newcommand{\lumi}{9.7~\ifb}
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vimartin |
1.1 |
%%%%%%%%%%%
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%
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\newcounter{myfootertablecounter}
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\newcommand\myfootnotemark{%
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%\refstepcounter{footnote}%
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\addtocounter{footnote}{1}%
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\footnotemark[\thefootnote]%
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}%
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\newcommand\myfootnotetext[1]{%
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\addtocounter{myfootertablecounter}{1}
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\footnotetext[\value{myfootertablecounter}]{#1}
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}
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% from now on, myfootnote has to be used rather than footnote to
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% adapt the myfootercounter
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\newcommand\myfootnote[1]{%
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\addtocounter{myfootertablecounter}{1}
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\footnote{#1}
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}%
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