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\typeout{TeV4LHC macros `qcd-tev4lhc.sty'. <October 23, 2005>.}
\NeedsTeXFormat{LaTeX2e}
\ProvidesPackage{qcd-tev4lhc}[10/23/05 Macros for TeV4LHC Write-up.]
%
% +--------------------------------------------------------------------+
% | |
% | The yspace macro |
% | |
% | Modification of David Carlisle's xspace package which puts a space |
% | after a macro if needed. I just turned it off inside mathmode, |
% | that's all. |
% | Now you don't need to put \; or \, or whatever after a macro. |
% | |
% +--------------------------------------------------------------------+
%
\DeclareRobustCommand\yspace{\futurelet\@let@token\@yspace}
\def\@yspace{%
\ifx\@let@token\bgroup\else
\ifx\@let@token\egroup\else
\ifx\@let@token\/\else
\ifx\@let@token\ \else
\ifx\@let@token~\else
\ifx\@let@token.\else
\ifx\@let@token!\else
\ifx\@let@token,\else
\ifx\@let@token:\else
\ifx\@let@token;\else
\ifx\@let@token?\else
\ifx\@let@token/\else
\ifx\@let@token'\else
\ifx\@let@token)\else
\ifx\@let@token-\else
\ifmmode\else
\space
\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi\fi}
%
% +--------------------------------------------------------------------+
% | |
% | Units etc
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\rts}{\ensuremath{\sqrt{s}}\yspace}
\newcommand{\keV}{\ensuremath{\mathrm{\ ke\kern -0.1em V}}\yspace}
\newcommand{\GeV}{\ensuremath{\mathrm{\ Ge\kern -0.1em V}}\yspace}
\newcommand{\TeV}{\ensuremath{\mathrm{\ Te\kern -0.1em V}}\yspace}
\newcommand{\MeV}{\ensuremath{\mathrm{\ Me\kern -0.1em V}}\yspace}
\newcommand{\eV}{\ensuremath{\mathrm{\ e\kern -0.1em V}}\yspace}
\newcommand{\cm}{\ensuremath{\mathrm{\ cm}}\yspace}
\newcommand{\mm}{\ensuremath{\mathrm{\ mm}}\yspace}
\newcommand{\mum}{\ensuremath{\mathrm{\ \mu m}}\yspace}
\newcommand{\pb}{\ensuremath{\mathrm{\ pb}^{-1}}\yspace}% Inverse picobarns.
\newcommand{\nb}{\ensuremath{\mathrm{\ nb}^{-1}}\yspace}% Inverse nanobarns.
\newcommand{\fb}{\ensuremath{\mathrm{\ fb}^{-1}}\yspace}% Inverse femptobarns.
\newcommand{\mrad}{\ensuremath{\mathrm{\ mrad}}\yspace}
\newcommand{\rad}{\ensuremath{\mathrm{\ rad}}\yspace}
\newcommand{\etal}{\textit{\ et~al.}\yspace}% For author lists in bibliography.
\newcommand{\ET}{\ensuremath{E_T}\yspace}
\newcommand{\PT}{\ensuremath{P_T}\yspace}
% +--------------------------------------------------------------------+
% | |
% | Particle-antiparticle pair notations. |
% | |
% +--------------------------------------------------------------------+
%
\def\antibar#1{\ensuremath{#1\bar{#1}}}%
\def\bbar{\ensuremath{\bar{b}}}
\def\bbbar{\antibar{b}\yspace}%
\def\cbar{\ensuremath{\bar{c}}}
\def\ccbar{\antibar{c}\yspace}%
\def\sbar{\ensuremath{\bar{s}}}
\def\ssbar{\antibar{s}\yspace}%
\def\ubar{\ensuremath{\bar{u}}}
\def\uubar{\antibar{u}\yspace}%
\def\dbar{\ensuremath{\bar{d}}}
\def\ddbar{\antibar{d}\yspace}%
\def\f{\ensuremath{f}\yspace}
\def\fbar{\ensuremath{\bar{f}}\yspace}
\def\ffbar{\antibar{f}\yspace}%
\def\qbar{\ensuremath{\bar{q}}}
\def\qqbar{\antibar{q}\yspace}%
\def\nbar{\ensuremath{\bar{\nu}}}
\def\nnbar{\antibar{\nu}\yspace}%
\def\ra{\ensuremath{\!\rightarrow\!}}
%
% +--------------------------------------------------------------------+
% | |
% | Here are e+, e-, e+e-, etc. |
% | |
% +--------------------------------------------------------------------+
%
\def\e{\ensuremath{e}}%
\def\epm{\ensuremath{e{\pm}}\yspace}%
\def\epem{\ensuremath{e+e^-}\yspace}%
\def\mumu{\ensuremath{\mu+ \mu^-}\yspace}%
\def\tautau{\ensuremath{\tau+ \tau^-}\yspace}%
%%%%\def\ll{\ensuremath{\ell^+ \ell^-}\yspace}%
\def\nunubar{\ensuremath{\nu\bar{\nu}}\yspace}%
%
% +--------------------------------------------------------------------+
% | |
% | Particles and whatnot. |
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\Z}{\ensuremath{Z}\yspace}
\newcommand{\W}{\ensuremath{W}\yspace}
\newcommand{\ZZ}{\ensuremath{ZZ}\yspace}
\newcommand{\Wpm}{\ensuremath{W^{\pm}}\yspace}
\newcommand{\WW}{\ensuremath{W^+W^-}\yspace}
\newcommand{\pion}{\ensuremath{\pi}\yspace}
\newcommand{\quark}{\ensuremath{q}\yspace}
\newcommand{\antiquark}{\ensuremath{\bar{q}}\yspace}
\newcommand{\bquark}{\ensuremath{b}\yspace}
\newcommand{\uquark}{\ensuremath{u}\yspace}
\newcommand{\dquark}{\ensuremath{d}\yspace}
\newcommand{\cquark}{\ensuremath{c}\yspace}
\newcommand{\squark}{\ensuremath{s}\yspace}
\newcommand{\tquark}{\ensuremath{t}\yspace}
\newcommand{\bantiquark}{\ensuremath{\bar{b}}\yspace}
\newcommand{\kaon}{\ensuremath{K}\yspace}
\newcommand{\kshort}{\ensuremath{K^0_S}\yspace}
\newcommand{\klong}{\ensuremath{K^0_L}\yspace}
\newcommand{\lambdazero}{\ensuremath{\Lambda^0}\yspace}
\newcommand{\Bzero}{\ensuremath{B^0}\yspace}
\newcommand{\Bpm}{\ensuremath{B^{\pm}}\yspace}
\newcommand{\Bzeros}{\ensuremath{B^0_{\squark}}\yspace}
%%%\newcommand{\Dzero}{\ensuremath{D^0}\yspace}
\newcommand{\Dpm}{\ensuremath{D^{\pm}}\yspace}
\newcommand{\Dpms}{\ensuremath{D^{\pm}_{\squark}}\yspace}
\newcommand{\lambdacpm}{\ensuremath{\Lambda^{\pm}_{\cquark}}\yspace}
\newcommand{\piminus}{\ensuremath{\pi^{-}}\yspace}
\newcommand{\piplus}{\ensuremath{\pi^{+}}\yspace}
\newcommand{\pizero}{\ensuremath{\pi^{o}}\yspace}
\newcommand{\tauminus}{\ensuremath{\tau^{-}}\yspace}
\newcommand{\tauplus}{\ensuremath{\tau^{+}}\yspace}
\newcommand{\neutrino}{\ensuremath{\nu}\yspace}
\newcommand{\neutrinobar}{\ensuremath{\bar{\nu}}\yspace}
\newcommand{\nue}{\ensuremath{\nu_\e}\yspace}
\newcommand{\numu}{\ensuremath{\nu_\mu}\yspace}
\newcommand{\nutau}{\ensuremath{\nu_\tau}\yspace}
\newcommand{\nubare}{\ensuremath{\bar\nu_\e}\yspace}
\newcommand{\nubarmu}{\ensuremath{\bar\nu_\mu}\yspace}
\newcommand{\nubartau}{\ensuremath{\bar\nu_\tau}\yspace}
\newcommand{\Hplusminus}{\ensuremath{H^{+}H^{-}}\yspace}
\newcommand{\Hpm}{\ensuremath{H^{\pm}}\yspace}
\newcommand{\h}{\ensuremath{h}\yspace}
\newcommand{\A}{\ensuremath{A}\yspace}
\newcommand{\bigH}{\ensuremath{H}\yspace}
\newcommand{\hZ}{\ensuremath{hZ}\yspace}
\newcommand{\hA}{\ensuremath{hA}\yspace}
\newcommand{\SMHZ}{\ensuremath{HZ}\yspace}
\newcommand{\hboson}{\ensuremath{h^{0}}\yspace}
\newcommand{\Hboson}{\ensuremath{H^{0}}\yspace}
\newcommand{\Aboson}{\ensuremath{A^{0}}\yspace}
% Some more below, from D0 Single top searches
\newcommand{\MET} {\mbox{$\not\!\!E_T$}}
\newcommand{\met} {\mbox{$\not\!\!E_T$}}
\newcommand{\rar} {\mbox{$\rightarrow$}}
\newcommand{\ipb} {\mbox{$ {\rm pb}^{-1} $}}
\newcommand{\dzero} {D\O\yspace}
% \newcommand{\dzero} {\ensuremath{\mbox{D\O}}}
\newcommand{\metc} {\mbox{$\not\!\!E_T^{\rm cal}$}}
\newcommand{\metjes} {\mbox{$\not\!\!E_T^{\rm JES}$}}
\newcommand{\mdeta} {\mbox{$|\eta^{\rm det}|$}}
\newcommand{\deta} {\mbox{$\eta^{\rm det}$}}
\newcommand{\meta} {\mbox{$|\eta|$}}
\newcommand{\rargap} {\mbox{ $\rightarrow$ }}
\newcommand{\ejm} {\mbox{$e$+jets/$\mu$}}
\newcommand{\mjm} {\mbox{$\mu$+jets/$\mu$}}
\newcommand{\ejbm} {\mbox{$e$+jets(/$\mu$)}}
\newcommand{\mjbm} {\mbox{$\mu$+jets(/$\mu$)}}
\newcommand{\ej} {\mbox{$e$+jets}}
\newcommand{\mj} {\mbox{$\mu$+jets}}
\newcommand{\tbbar} {\mbox{$tb$}}
\newcommand{\tqbbar} {\mbox{$tqb$}}
\newcommand{\Wbbbar} {\mbox{$Wb\bar{b}$}}
\newcommand{\Wccbar} {\mbox{$Wc\bar{c}$}}
\newcommand{\Wjjbar} {\mbox{$Wj\bar{j}$}}
\newcommand{\comphep} {C\rm{omp}\sc{hep}}
\newcommand{\herwig} {{\sc{herwig}}}
\newcommand{\pythia} {{\sc{pythia}}}
\newcommand{\alpgen} {{\sc{alpgen}}}
\newcommand{\singletop} {\rm{SingleTop}}
\newcommand{\tauola} {\sc{tauola}}
\newcommand{\evtgen} {\sc{evtgen}}
\newcommand{\geant} {\sc{geant}}
\newcommand{\dogstar} {\sc{d}0\sc{gstar}}
\newcommand{\dosim} {\sc{d}0\sc{sim}}
\newcommand{\reco} {\sc{reco}}
\newcommand{\trigsim} {\sc{trigsim}}
\def \gev {\mbox{${\rm GeV/}c{\rm ^2}$}}
\def \tev {\mbox{${\rm TeV/}c{\rm ^2}$}}
%
% +--------------------------------------------------------------------+
% | |
% | Particles masses |
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\mtau}{\ensuremath{m_\tau}\yspace}
\newcommand{\mt}{\ensuremath{m_t}\yspace}
\newcommand{\mb}{\ensuremath{m_b}\yspace}
\newcommand{\mc}{\ensuremath{m_c}\yspace}
\newcommand{\mZ}{\ensuremath{m_Z}\yspace}
\newcommand{\mW}{\ensuremath{m_W}\yspace}
\newcommand{\mHplusminus}{\ensuremath{m_{H^\pm}}\yspace}
\newcommand{\mh}{\ensuremath{m_h}\yspace}
\newcommand{\mH}{\ensuremath{m_H}\yspace}
\newcommand{\mA}{\ensuremath{m_A}\yspace}
\newcommand{\mX}{\ensuremath{m_X}\yspace}
\newcommand{\MZ}{\ensuremath{M_Z}\yspace}
\newcommand{\MW}{\ensuremath{M_W}\yspace}
%\newcommand{\Mh}{\ensuremath{M_h}\yspace}
\newcommand{\MH}{\ensuremath{M_H}\yspace}
\newcommand{\MA}{\ensuremath{M_A}\yspace}
%
% +--------------------------------------------------------------------+
% | |
% | Tevatron production |
% | |
% +--------------------------------------------------------------------+
%
\def\pbar{\ensuremath{\bar{\mathrm{p}}}}
\def\ppbar{\antibar{\mathrm{p}}\yspace}%
\def\tbar{\ensuremath{\bar{\mathrm{t}}}}
\def\ttbar{\antibar{\mathrm{t}}\yspace}%
\newcommand{\ggtoA}{\ensuremath{gg\!\rightarrow\!\A}\yspace}
\newcommand{\Atotautau}{\ensuremath{\Ato\tautau}\yspace}
\newcommand{\htotautau}{\ensuremath{\hto\tautau}\yspace}
\newcommand{\bbAtobbbb}{\ensuremath{\bbbar\Ato\bbbar\bbbar}\yspace}
\newcommand{\bbhtobbbb}{\ensuremath{\bbbar\Ato\bbbar\bbbar}\yspace}
\newcommand{\qqtobbAtobbbb}{\ensuremath{\qqbar\!\rightarrow\!\bbbar\Ato\bbbar\bbbar}\yspace}
\newcommand{\ggtobbAtobbbb}{\ensuremath{gg\!\rightarrow\!\bbbar\Ato\bbbar\bbbar}\yspace}
\newcommand{\ggtobbAhtobbbb}{\ensuremath{gg\!\rightarrow\!\bbbar\A/\hto\bbbar\bbbar}\yspace}
\newcommand{\pptobbAtobbbb}{\ensuremath{\ppbar\!\rightarrow\!\bbbar\Ato\bbbar\bbbar}\yspace}
\newcommand{\ggtoAtotautau}{\ensuremath{gg\!\rightarrow\!\Atotautau}\yspace}
\newcommand{\ggtohtotautau}{\ensuremath{gg\!\rightarrow\!\htotautau}\yspace}
\newcommand{\ppbartottbar}{\ensuremath{\ppbar\!\rightarrow\!\ttbar}\yspace}
%
% +--------------------------------------------------------------------+
% | |
% | Tevatron and W decays |
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\Wto}{\ensuremath{\W\!\rightarrow\!}}
\newcommand{\Wtoqq}{\ensuremath{\W\!\rightarrow\!q\bar{q'}}\yspace}
\newcommand{\Wtolnu}{\ensuremath{\W\!\rightarrow\!l\nu}\yspace}
\newcommand{\Wtoenu}{\ensuremath{\W\!\rightarrow\!\e\nu}\yspace}
\newcommand{\DtoKpi}{\ensuremath{D^0\!\rightarrow\! K\pi}\yspace}
%
% +--------------------------------------------------------------------+
% | |
% | Higgs decays |
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\hto}{\ensuremath{\h\!\rightarrow\!}}
\newcommand{\Hto}{\ensuremath{\bigH\!\rightarrow\!}}
\newcommand{\Ato}{\ensuremath{\A\!\rightarrow\!}}
\newcommand{\hAto}{\ensuremath{\h\A\!\rightarrow\!}}
\newcommand{\htobb}{\ensuremath{\hto b\bar{b}}\yspace}
\newcommand{\Htobb}{\ensuremath{\Hto b\bar{b}}\yspace}
\newcommand{\htocc}{\ensuremath{\hto c\bar{c}}\yspace}
\newcommand{\Htocc}{\ensuremath{\Hto c\bar{c}}\yspace}
\newcommand{\htogg}{\ensuremath{\hto gg}\yspace}
\newcommand{\Htogg}{\ensuremath{\Hto gg}\yspace}
\newcommand{\Htophotons}{\ensuremath{\Hto \gamma\gamma}\yspace}
\newcommand{\htott}{\ensuremath{\hto \tautau}\yspace}
\newcommand{\Htott}{\ensuremath{\Hto \tautau}\yspace}
\newcommand{\Atobb}{\ensuremath{\Ato b\bar{b}}\yspace}
\newcommand{\Atott}{\ensuremath{\Ato \tautau}\yspace}
\newcommand{\HplustoLep}{\ensuremath{H^{+}\!\!\!\rightarrow\!
\tau^+\nutau}\yspace}
\newcommand{\HplustoHad}{\ensuremath{H^{+}\!\!\!\rightarrow\!
\mathrm{c\bar{s}}}\yspace}
\newcommand{\hAtobbbb}{\ensuremath{\hA\!\rightarrow\!
b\bar{b}b\bar{b}}\yspace}
\newcommand{\hAtobbbbToo}{\ensuremath{\hA\rightarrow
b\bar{b}b\bar{b}}\yspace}
\newcommand{\hAtobbtt}{\ensuremath{\hA\!\rightarrow\!
b\bar{b}\tau^+\tau^-}\yspace}
\newcommand{\hAtottbb}{\ensuremath{\hA\!\rightarrow\!
\tau^+\tau^-b\bar{b}}\yspace}
\newcommand{\hZtobbqq}{\ensuremath{\hZ\!\rightarrow\!
b\bar{b}q\bar{q}}\yspace}
\newcommand{\hZtoAAff}{\ensuremath{\hZ\!\rightarrow\!
AAf\bar{f}}\yspace}
\newcommand{\hZtobbqqToo}{\ensuremath{\hZ\rightarrow
b\bar{b}q\bar{q}}\yspace}
\newcommand{\hZtoqqqq}{\ensuremath{\hZ\!\rightarrow\!
q\bar{q}q\bar{q}}\yspace}
\newcommand{\hZtoccqq}{\ensuremath{\hZ\!\rightarrow\!
c\bar{c}q\bar{q}}\yspace}
\newcommand{\hZtoggqq}{\ensuremath{\hZ\!\rightarrow\!
ggq\bar{q}}\yspace}
\newcommand{\hZtobbnn}{\ensuremath{\hZ\!\rightarrow\!
b\bar{b}\nu\bar{\nu}}\yspace}
\newcommand{\hZtobbll}{\ensuremath{\hZ\!\rightarrow\!
b\bar{b}\ell^+\ell^-}\yspace}
\newcommand{\hZtoqqll}{\ensuremath{\hZ\!\rightarrow\!
q\bar{q}\ell^+\ell^-}\yspace}
\newcommand{\hZtobbtt}{\ensuremath{\hZ\!\rightarrow\!
b\bar{b}\tau^+\tau^-}\yspace}
\newcommand{\hZtottbb}{\ensuremath{\hZ\!\rightarrow\!
\tau^+\tau^-b\bar{b}}\yspace}
\newcommand{\hZtottqq}{\ensuremath{\hZ\!\rightarrow\!
\tau^+\tau^-q\bar{q}}\yspace}
\newcommand{\hZtoqqtt}{\ensuremath{\hZ\!\rightarrow\!
q\bar{q}\tau^+\tau^-}\yspace}
\newcommand{\htoAA}{\ensuremath{\hto\A\A}\yspace}
%
% +--------------------------------------------------------------------+
% | |
% | SUSY Notations |
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\tanb} {\ensuremath{\tan\beta}\yspace}
\newcommand{\Stop} {\ensuremath{\tilde t}\yspace}
\newcommand{\Sbot} {\ensuremath{\tilde b}\yspace}
\newcommand{\StopL}{\ensuremath{\tilde{t}_L}\yspace}
\newcommand{\StopR}{\ensuremath{\tilde{t}_R}\yspace}
\newcommand{\SbotL}{\ensuremath{\tilde{b}_L}\yspace}
\newcommand{\SbotR}{\ensuremath{\tilde{b}_R}\yspace}
\newcommand{\mhmax}{\ensuremath{\mh^{\mathrm{max}}}\yspace}
\newcommand{\MstL} {\ensuremath{M_{\tilde{t}_L}}\yspace}
\newcommand{\MstR} {\ensuremath{M_{\tilde{t}_R}}\yspace}
\newcommand{\MsbL} {\ensuremath{M_{\tilde{b}_L}}\yspace}
\newcommand{\MsbR} {\ensuremath{M_{\tilde{b}_R}}\yspace}
\newcommand{\msusy}{\ensuremath{M_{\mathrm{SUSY}}}\yspace}
\newcommand{\At} {\ensuremath{A_t}\yspace}
\newcommand{\Ab} {\ensuremath{A_b}\yspace}
\newcommand{\Xt} {\ensuremath{X_t}\yspace}
\newcommand{\Xb} {\ensuremath{X_b}\yspace}
\newcommand{\mgl} {\ensuremath{m_{\tilde{g}}}\yspace}
\newcommand{\CZb} {\ensuremath{\cos 2\beta}\yspace}
\newcommand{\CTb} {\ensuremath{\cot\beta}\yspace}
\newcommand{\sw} {\ensuremath{s_\mathrm{w}}\yspace}
\newcommand{\cw} {\ensuremath{c_\mathrm{w}}\yspace}
%
% +--------------------------------------------------------------------+
% | |
% | Names of Codes |
% | |
% +--------------------------------------------------------------------+
%
\newcommand{\IS}{{\sf ISAJET}}
\newcommand{\CK}{{\sf CKKW}}
\newcommand{\PY}{{\sc PYTHIA}\yspace}
\newcommand{\IW}{{\sf ISAWIG}}
\newcommand{\MN}{{\sc MC@NLO}\yspace}
\newcommand{\JM}{{\sc JIMMY}\yspace}
\newcommand{\TA}{{\sf TAUOLA}}
\newcommand{\AL}{{\sf ALPGEN}}\newcommand{\AR}{{\sf ARIADNE}}
\newcommand{\CI}{{\sf CIRCE}}
\newcommand{\HD}{{\sf HDECAY}}
\newcommand{\HP}{{\sf HERWIG++}}
\newcommand{\HW}{{\sc HERWIG}\yspace}
\newcommand{\LHAPDF}{{\sc LHAPDF}\yspace}
\newcommand{\fastNLO}{{\sc fastNLO}\yspace}
\newcommand{\HA}{{\sf HARWIG}}
\newcommand{\MAD}{{\sf MADGRAPH}}
%
\hyphenation{KARMEN}
\hyphenation{HERWIG}
\hyphenation{PYTHIA}
\hyphenation{JETSET}
\hyphenation{SUSYGEN}
\hyphenation{ARIADNE}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%%% [re]defined commands from D0 wwidth (
\newcommand{\centervalue}{2.011}
\newcommand{\staterror}{0.093}
\newcommand{\systerror}{0.099}
\newcommand{\centerratiofit}{2.004}
\newcommand{\statratiofit}{0.091}
% \newcommand{\gev}{\ensuremath{\mbox{GeV}}}
\newcommand{\egev}{\ensuremath{\mbox{GeV}}}
\newcommand{\pgev}{\ensuremath{\mbox{GeV/c}}}
\newcommand{\mgev}{\ensuremath{\mbox{GeV/c}^{2}}}
%%% \newcommand{\et}{\ensuremath{\mbox{E}_{\mbox{T}}}}
\newcommand{\emet}{\ensuremath{\mbox{E}^{\mbox{EM}}_{\mbox{T}}}}
\newcommand{\hadet}{\ensuremath{\mbox{E}^{\mbox{HAD}}_{\mbox{T}}}}
\newcommand{\vete}{\ensuremath{\vec{\mbox{E}}_{\mbox{T}}^{e}}}
\newcommand{\vmet}{\ensuremath{{\not\! \vec{\mbox{E}}}_{\mbox{T}}}}
%%% \newcommand{\met}{\ensuremath{{\not\! E}_{T}}}
\newcommand{\mpt}{\ensuremath{{\not\! \vec{p}}_{T}}}
\newcommand{\pxmet}{\ensuremath{{\not\! \mbox{P}}_{\mbox{x}}}}
\newcommand{\pymet}{\ensuremath{{\not\! \mbox{P}}_{\mbox{y}}}}
\newcommand{\vu}{\ensuremath{\vec{\mbox{U}}}}
\newcommand{\qt}{\ensuremath{\mbox{q}_{\mbox{T}}}}
\newcommand{\rawaz}{\ensuremath{\mbox{A}_{\mbox{W}}/\mbox{A}_{\mbox{Z}}}}
\newcommand{\awaz}{\ensuremath{\frac{\mbox{A}_{\mbox{W}}}{\mbox{A}_{\mbox{Z}}}}}
\newcommand{\aw}{\ensuremath{\mbox{A}_{\mbox{W}}}}
\newcommand{\az}{\ensuremath{\mbox{A}_{\mbox{Z}}}}
\newcommand{\mw}{\ensuremath{\mbox{M}_{\mbox{W}}}}
\newcommand{\mz}{\ensuremath{\mbox{M}_{\mbox{Z}}}}
\newcommand{\stw}{\ensuremath{\sin^2 \theta_{\mbox{W}}}}
\newcommand{\ppt}{\ensuremath{\mbox{P}_{\mbox{T}}}}
\newcommand{\eop}{\ensuremath{\mbox{E}/\mbox{P}}}
\newcommand{\zzero}{\ensuremath{\mbox{Z}^{\circ}}}
\newcommand{\hadoem}{\ensuremath{\mbox{Had}/\mbox{Em}}}
\newcommand{\ethadoem}{\ensuremath{\hadet / \emet}}
%%% \newcommand{\mt}{\ensuremath{\mbox{M}_{\mbox{T}}}}
\newcommand{\mee}{\ensuremath{\mbox{M}_{\mbox{e^+e^-}}}}
%% \newcommand\mee{M_{e^+ e^-}}
\newcommand{\ect}{\ensuremath{\mbox{c}_{\mbox{1}}}}
\newcommand{\ecl}{\ensuremath{\mbox{c}_{\mbox{2}}}}
\newcommand{\ecll}{\ensuremath{\mbox{c}_{\mbox{3}}}}
\newcommand{\ep}{\ensuremath{\mbox{p}}}
\newcommand{\ef}{\ensuremath{\mbox{f}}}
\newcommand{\etrig}{\ensuremath{\epsilon_{\mbox{T}}}}
\newcommand{\etrigl}{\ensuremath{\epsilon^{\mbox{l}}_{\mbox{T}}}}
\newcommand{\etrige}{\ensuremath{\epsilon^{\mbox{e}}_{\mbox{T}}}}
\newcommand{\npp}{\ensuremath{\mbox{N}_{\mbox{PP}}}}
\newcommand{\npf}{\ensuremath{\mbox{N}_{\mbox{PF}}}}
\newcommand{\ntot}{\ensuremath{\mbox{N}_{\mbox{tot}}}}
\newcommand{\nppss}{\ensuremath{\mbox{N}_{\mbox{PP}}^{\mbox{ss}}}}
\newcommand{\npfss}{\ensuremath{\mbox{N}_{\mbox{PF}}^{\mbox{ss}}}}
\newcommand{\fracl}{\ensuremath{\mbox{f}_{\mbox{l}}}}
\newcommand{\frach}{\ensuremath{\mbox{f}_{\mbox{h}}}}
\newcommand{\fcc}{\ensuremath{\mbox{F}_{\mbox{cc}}}}
\newcommand{\fcp}{\ensuremath{\mbox{F}_{\mbox{cp}}}}
\newcommand{\fcf}{\ensuremath{\mbox{F}_{\mbox{cf}}}}
\newcommand{\ew}{\ensuremath{\epsilon_{\mbox{W}}}}
\newcommand{\ez}{\ensuremath{\epsilon_{\mbox{Z}}}}
\newcommand{\wtaunusign}{\ensuremath{\mbox{W}^{\pm} \rightarrow \tau^{\pm} \nu}}
\newcommand{\wtaunu}{\ensuremath{W \rightarrow \tau \nu}}
\newcommand{\wen}{\ensuremath{W \rightarrow e \nu}}
\newcommand{\wenu}{\ensuremath{\mbox{W}^{\pm} \rightarrow \mbox{e}^{\pm} \nu}}
\newcommand{\wud}{\ensuremath{\mbox{W}^+ \rightarrow u \overline{d}}}
\newcommand{\wdu}{\ensuremath{\mbox{W}^- \rightarrow d \overline{u}}}
\newcommand{\wmunu}{\ensuremath{\mbox{W}^{\pm} \rightarrow \mu^{\pm} \nu}}
\newcommand{\ztautau}{\ensuremath{\mbox{Z}^{\circ} \rightarrow \tau^+ \tau^-}}
\newcommand{\znunu}{\ensuremath{\mbox{Z}^{\circ} \rightarrow \nu \overline{\nu}}}
\newcommand{\zuu}{\ensuremath{\mbox{Z}^{\circ} \rightarrow u \overline{u}}}
\newcommand{\zeesign}{\ensuremath{\mbox{Z}^{\circ} \rightarrow \mbox{e}^+\mbox{e}^-}}
\newcommand{\zee}{\ensuremath{Z \rightarrow ee}}
\newcommand{\zmumu}{\ensuremath{\mbox{Z}^{\circ} \rightarrow \mu ^{+} \mu ^{-}}}
%%% \newcommand{\qqbar}{\ensuremath{q\overline{q}}}
%%% \newcommand{\ppbar}{\ensuremath{p\overline{p}}}
%%% \newcommand{\ttbar}{\ensuremath{t\overline{t}}}
\newcommand{\gamw}{\ensuremath{\Gamma \left( \mbox{W} \right) }}
\newcommand{\gamz}{\ensuremath{\Gamma \left( \mbox{Z} \right) }}
\newcommand{\gamwenu}{\ensuremath{\Gamma \left( \wenu \right) }}
\newcommand{\gamzee}{\ensuremath{\Gamma \left( \zee \right) }}
\newcommand{\sigw}{\ensuremath{\sigma_{\mbox{W}}}}
\newcommand{\sigz}{\ensuremath{\sigma_{\mbox{Z}}}}
\newcommand{\z}{Z$^{\circ} \ $}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\renewcommand{\baselinestretch}{1.1}
% Symbol definitions
\newcommand\ltap{\
\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}\ }
\newcommand\gtap{\
\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}\ }
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% \simge and \simle make "approx greater than" and "approx less than"
\newcommand\simge{\mathrel{%
\rlap{\raise 0.511ex \hbox{$>$}}{\lower 0.511ex \hbox{$\sim$}}}}
\newcommand\simle{\mathrel{
\rlap{\raise 0.511ex \hbox{$<$}}{\lower 0.511ex \hbox{$\sim$}}}}
% \slashcar puts a slash through a character to represent contraction
% with Dirac matrices. Use \not instead for negation of relations, and use
% \hbar for hbar.
\newcommand{\slashchar}[1]%
{\kern .25em\raise.18ex\hbox{$/$}\kern-.75em #1}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\def\lsim{\mathrel{\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\def\gsim{\mathrel{\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}}}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%% from landscape/TC/TC.tex
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\newcommand{\bs}{\boldsymbol}
\newcommand\nn{\nonumber}
\newcommand\whW{\widehat W}
\newcommand\wtW{\widetilde W}
\newcommand\whD{\widehat D}
\newcommand\wtD{\widetilde D}
\newcommand\homega{\widehat\omega_{Da}}
\newcommand\whomega{\widehat\omega_8}
\newcommand\whomegaz{\widehat\omega_{8,0}}
\newcommand\dtwoE{d^2E(W)/d\Lambda^2}
\newcommand{\bket}{\ensuremath{|B^0 \rangle}}
\newcommand{\bbra}{\ensuremath{\langle B^0|}}
\newcommand{\bbarket}{\ensuremath{|\bar{B}^0\rangle}}
\newcommand{\bbarbra}{\ensuremath{\langle \bar{B}^0|}}
\newcommand{\lcp}{\ensuremath{\lambda_{CP}}}
\newcommand{\dmu}{\ensuremath{\partial_{\mu}}}
\newcommand{\dmup}{\ensuremath{\partial^{\mu}}}
\newcommand{\dnu}{\ensuremath{\partial_{\nu}}}
\newcommand{\sigbar}{\ensuremath{\bar{\sigma}^{\mu}\cdot}}
\newcommand{\sig}{\ensuremath{\sigma^{\mu}\cdot}}
\newcommand{\VA}{\ensuremath{\gamma^{\mu}(1 - \gamma_5)}}
\newcommand{\gm}{\ensuremath{\gamma^{\mu}}}
\newcommand{\gd}{\ensuremath{\gamma_{\mu}}}
\newcommand{\gammat}{\ensuremath{\left( \begin{array}{cc} 0 & \sigma^{\mu} \\
\bar{\sigma}^{\mu} & 0 \\ \end{array} \right)}}
\newcommand{\gndbra}{\ensuremath{\langle \Omega |}}
\newcommand{\gndket}{\ensuremath{|\Omega \rangle}}
\newcommand{\half}{\ensuremath{\frac{1}{2}}}
\newcommand{\thhalf}{\ensuremath{\frac{3}{2}}}
\newcommand{\hsig}{\ensuremath{\frac{\sigma_a}{2}}}
\newcommand{\BD}{\ensuremath{B_d}}
\newcommand{\BDbar}{\ensuremath{\bar B_d}}
\newcommand{\stwobeta}{\ensuremath{\sin{2\beta}}}
\newcommand\thc{\theta_C}
\newcommand\thy{\theta_Y}
\newcommand\dagg{\dagger}
\newcommand\ts{\thinspace}
\newcommand\Ra{\Rightarrow}
\newcommand\Lra{\Longrightarrow}
\newcommand\longra{\longrightarrow}
\newcommand\leftra{\leftrightarrow}
\newcommand\llra{\longleftrightarrow}
\newcommand\ol{\bar}
\newcommand\ecm{\sqrt{s}}
\newcommand\rshat{\sqrt{\shat}}
\newcommand\shat{\hat s}
\newcommand\nin{\noindent}
\newcommand\lvac{\langle \Omega \vert}
\newcommand\rvac{\vert \Omega \rangle}
\newcommand\condt{\langle \bar T T\rangle}
\newcommand\condtt{\langle \bar T^t_L T^t_R\rangle}
\newcommand\condtb{\langle \bar T^b_L T^b_R\rangle}
\newcommand\condtl{\langle \bar T^l_L T^l_R\rangle}
\newcommand\condaa{\langle \bar T^1_L T^1_R\rangle}
\newcommand\condbb{\langle \bar T^2_L T^2_R\rangle}
\newcommand\condab{\langle \bar T^1_L T^2_R\rangle}
\newcommand\condba{\langle \bar T^2_L T^1_R\rangle}
\newcommand\condij{\langle \bar T^i_L T^j_R\rangle}
\newcommand\conduij{\langle \bar U_{iL} U_{jR}\rangle}
\newcommand\conddij{\langle \bar D_{iL} D_{jR}\rangle}
\newcommand\condtbt{\langle \bar t t\rangle}
\newcommand\condbbb{\langle \bar b b\rangle}
\newcommand\trho{\rho_T}
\newcommand\toppi{\pi_t}
\newcommand\etmiss{\slashchar{E}_T}
\newcommand\emiss{\slashchar{E}}
\newcommand\cstar{\cos \theta^*}
\newcommand\sscy{10 \ts \fb^{-1}}
\newcommand\hl{10^{33} \ts {\rm cm}^{-2} \ts {\rm s}^{-1}}
\newcommand\hly{10^{40} \ts {\rm cm}^{-2}}
\newcommand\uhl{10^{34} \ts {\rm cm}^{-2} \ts {\rm s}^{-1}}
\newcommand\uhly{10^{41} \ts {\rm cm}^{-2}}
\newcommand\sscd{100 \ts \fb^{-1}}
\newcommand\yr{{\rm yr}}
\newcommand\cmsec{{\rm cm^{-2}sec^{-1}}}
\newcommand\ellm{\ell^-}
\newcommand\ellpm{\ell^\pm}
\newcommand\ellp{\ell^+}
%%% \newcommand\ep{e^+}
\newcommand\mgg{M_{\gamma \gamma}}
\newcommand\mll{M_{\ell^+ \ell^-}}
%
\newcommand\cond{\langle \ol T T\rangle}
\newcommand\getc{g_{ETC}}
\newcommand\Gtc{G_{TC}}
\newcommand\Gew{SU(2)\otimes U(1)}
\newcommand\Getc{G_{ETC}}
\newcommand\su{SU(3)}
\newcommand\suc{SU(3)_C}
\newcommand\Ntc{N_{TC}}
\newcommand\sutc{SU(N_{TC})}
\newcommand\uone{U(1)_1}
\newcommand\utwo{U(1)_2}
\newcommand\uy{U(1)_Y}
\newcommand\suone{SU(3)_1}
\newcommand\sutwo{SU(3)_2}
\newcommand\suthree{SU(3)_3}
\newcommand\aqcd{\alpha_{S}}
\newcommand\atc{\alpha_{TC}}
\newcommand\aetc{\alpha_{ETC}}
\newcommand\Metc{M_{ETC}}
\newcommand\Letc{\Lambda_{ETC}}
\newcommand\Ltc{\Lambda_{TC}}
\newcommand\condtc{{\langle \ol T T \rangle}_{TC}}
\newcommand\condetc{{\langle \ol T T \rangle}_{ETC}}
\newcommand\vev{\langle \phi \rangle}
%
\newcommand\tom{\omega_{T}}
\newcommand\tro{\rho_{T}}
\newcommand\tros{\rho_{T8}^{0}}
\newcommand\troct{\rho_{T8}}
\newcommand\tropm{\rho_{T}^\pm}
\newcommand\trop{\rho_{T}^+}
\newcommand\trom{\rho_{T}^-}
\newcommand\troz{\rho_{T}^0}
%
\newcommand\tpi{\pi_T}
\newcommand\tpipm{\pi_T^\pm}
\newcommand\tpimp{\pi_T^\mp}
\newcommand\tpip{\pi_T^+}
\newcommand\tpim{\pi_T^-}
\newcommand\tpiz{\pi_T^0}
\newcommand\tpipr{\pi_T^{0 \prime}}
\newcommand\tpilq{\pi_{L\ol Q}}
\newcommand\tpiql{\pi_{Q\ol L}}
\newcommand\tpioct{\pi_{T8}}
\newcommand\etat{\eta_{_{T}}}
\newcommand\trou{\rho_{_{\ol U U}}}
\newcommand\trod{\rho_{_{\ol D D}}}
\newcommand\rhol{\rho_{_{\ol L L}}}
\newcommand\rhoq{\rho_{_{\ol Q Q}}}
\newcommand\rhon{\rho_{_{\ol N N}}}
\newcommand\rhoe{\rho_{_{\ol E E}}}
\newcommand\piqq{\pi_{_{\ol Q Q}}}
\newcommand\piql{\pi_{_{\ol Q L}}}
\newcommand\piuu{\pi_{_{\ol U U}}}
\newcommand\pidd{\pi_{_{\ol D D}}}
\newcommand\piud{\pi_{_{\ol U D}}}
\newcommand\pidu{\pi_{_{\ol D U}}}
\newcommand\pinu{\pi_{_{\ol N U}}}
\newcommand\piun{\pi_{_{\ol U N}}}
\newcommand\pieu{\pi_{_{\ol E U}}}
\newcommand\piue{\pi_{_{\ol U E}}}
\newcommand\pind{\pi_{_{\ol N D}}}
\newcommand\pidn{\pi_{_{\ol D N}}}
\newcommand\pied{\pi_{_{\ol E D}}}
\newcommand\pide{\pi_{_{\ol D E}}}
\newcommand\chipr{\chi^{\ts \prime}}
%
\newcommand\afb{A_{FB}}
\newcommand\pbp{\ol p p}
\newcommand\Mh{M_{\eta_{_{T}}}}
\newcommand\Mv{M_{V_8}}
\newcommand\Mtt{\CM_{\ol t t}}
\newcommand\MMtt{\langle \Mtt \rangle}
\newcommand\MSMtt{\langle \Mtt^2 \rangle}
\newcommand\RMStt{{\langle \Mtt^2 \rangle^{1/2}}}
\newcommand\Deltt{\Delta \Mtt}
\newcommand\jet{{\rm jet}}
\newcommand\jets{{\rm jets}}
\newcommand\stt{\sigma(\tbt)}
\newcommand\QbQ{\ol Q Q}
%
%
% D0 varibles
%
\newcommand{\gj}{\ensuremath{\gamma+}jets\yspace}
\newcommand{\gb}{\ensuremath{\gamma+}b\yspace}
\newcommand{\Rj}{\ensuremath{\mathrm{R_j}}\yspace}
\newcommand{\Rb}{\ensuremath{\mathrm{R_b}}\yspace}
\newcommand{\Rc}{\ensuremath{\mathrm{R_c}}\yspace}
\newcommand{\mtrk}{\ensuremath{m_\mathrm{trk}}\yspace}
\newcommand{\CSIP}{{\scshape Csip}\yspace}
\newcommand{\DO}{D\O\yspace}
%
% funny CDF stuff
%
\newcommand{\NONE}{\mbox{$\widetilde{\chi}_1^0$}}
\newcommand{\CONE}{\mbox{$\widetilde{\chi}_1^{\pm}$}}
%
% Things for Fabio's contribution
%
\newcommand{\cp}{\ensuremath{\mathcal CP}\yspace}
\def\citere#1{\mbox{Ref.~\cite{#1}}}
\def\citeres#1{\mbox{Refs.~\cite{#1}}}
\newcommand{\ML}{\left( \begin{array}{cc}}
\newcommand{\MR}{\end{array} \right)}
\newcommand{\edz}{\frac{1}{2}}
\newcommand{\drbar}{\ensuremath{\overline{\mathrm{DR}}}\yspace}
\newcommand{\BE}{\begin{equation}}
\newcommand{\EE}{\end{equation}}
\newcommand{\BEA}{\begin{eqnarray}}
\newcommand{\EEA}{\end{eqnarray}}
\newcommand{\non}{\nonumber}
\def\aeff{\al_{\rm eff}}
\newcommand{\al}{\alpha}
\newcommand{\ga}{\gamma}
\newcommand{\Ga}{\Gamma}
\newcommand{\SM}{\mathrm {SM}}
\newcommand{\MSSM}{\mathrm {MSSM}}
\def\order#1{${\cal O}(#1)$}
\newcommand{\KL}{\left(}
\newcommand{\KR}{\right)}
%%% from Lane's contribution
\def\lsim{\mathrel{\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\def\gsim{\mathrel{\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\newcommand\CC{{\cal C}}\newcommand\CCC{$\CC$}
\newcommand\CH{{\cal H}}\newcommand\CCH{$\CH$}
\newcommand\CM{{\cal M}}\newcommand\CCM{$\CM$}
\newcommand\ifb{{\rm fb}^{-1}}
\newcommand\ba{\begin{array}}
\newcommand\ea{\end{array}}
\newcommand\bea{\begin{eqnarray}}
\newcommand\eea{\end{eqnarray}}
\newcommand\atro{\alpha_{\tro}}
%%% From Hubisz
%NEWUSEFULRULES
\newcommand{\whp}[1]{W_H^{+#1}}
\newcommand{\whm}[1]{W_H^{-#1}}
%\newcommand{\ah}[1]{A_H^{#1}}
\newcommand{\wlp}[1]{W^{+#1}}
\newcommand{\wlm}[1]{W^{-#1}}
\newcommand{\zh}[1]{Z_H^{#1}}
%\newcommand{\cw}{c_w}
%\newcommand{\sw}{s_w}
\newcommand{\phs}{\phi^P}
\newcommand{\php}{\phi^+}
\newcommand{\phm}{\phi^-}
\newcommand{\pho}{\phi^0}
\newcommand{\phpp}{\phi^{++}}
\newcommand{\phmm}{\phi^{--}}
\newcommand{\moms}{\left( p_1 - 2 p_2 \right)_\mu}
\newcommand{\tpb}{\bar{t}'_+}
\newcommand{\tm}{t'_-}
\newcommand{\tmb}{\bar{t}'_-}
\newcommand{\tp}{t'_+}
\newcommand{\EPSs}{\frac{v^2}{f^2}}
\def\w{{\rm w}}
\def\z{{\rm z}}
\def\gev{~{\rm GeV}}
\def\tev{~{\rm TeV}}
\def\fbi{~{\rm fb}^{-1}}
\def\fb{~{\rm fb}}
\def\call{{\cal L}}
\def\calO{{\mathcal{O}}}
\def\rts{\sqrt s}
\def\vev#1{\langle #1 \rangle}
\def\br{{\rm BR}}
%
\def\lsim{\mathrel{\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\def\gsim{\mathrel{\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\def\ifmath#1{\relax\ifmmode #1\else $#1$\fi}
\newcommand{\msbar}{\ensuremath{\overline{\rm{MS}}}\yspace}
\newcommand{\mbms}{\ensuremath{\overline{m}_b}\yspace}
% ========================= Revised RDF DEFINITIONS =========================
\newcommand*{\eg}{\textit{e.g.},\ }
\newcommand*{\ie}{\textit{i.e.},\ }
%%FSC \newcommand*{\etal}{\textit{et al.\ }}
%%FSC \newcommand*{\gev}{\,\textrm{GeV}}
\newcommand*{\gevc}{\,\textrm{GeV/c}}
\newcommand*{\mevc}{\,\textrm{MeV/c}}
%%FSC \newcommand*{\tev}{\,\textrm{TeV}}
%%FSC \newcommand*{\Dzero}{D$0$}
\newcommand*{\pt}{$p_T$}
%%FSC \newcommand*{\bigpt}{$P_T$}
\newcommand*{\UE}{``underlying event"}
\newcommand*{\BBR}{``beam-beam remnants"}
\newcommand*{\MB}{``min-bias"}
\newcommand*{\TR}{``transverse"}
\newcommand*{\tmax}{``transMAX"}
\newcommand*{\tmin}{``transMIN"}
\newcommand*{\tdif}{``transDIF"}
\newcommand*{\LJ}{``leading jet"}
\newcommand*{\BB}{``back-to-back"}
\newcommand*{\Tone}{``transverse $1$"}
\newcommand*{\etone}{$E_T({\rm jet}\#1)$}
\newcommand*{\ptone}{$P_T({\rm jet}\#1)$}
\newcommand*{\Ttwo}{``transverse $2$"}
\newcommand*{\Jone}{jet\#$1$\yspace}
\newcommand*{\Jtwo}{jet\#$2$\yspace}
\newcommand*{\Jthree}{jet\#$3$\yspace}
\newcommand*{\Jfour}{jet\#$4$\yspace}
%\newcommand*{\CJone}{chgjet\#$1$}
\newcommand*{\CJone}{chgjet$1$}
%\newcommand*{\ptcj}{$P_T$(chgjet\#$1)$}
\newcommand*{\ptcj}{$P_T({\rm chgjet}1)$}
\newcommand*{\pthard}{$p_T({\rm hard})$}
%%FSC \newcommand*{\ptmax}{$PT{\rm max}$}
\newcommand*{\ptmaxT}{$PT{\rm max}T$}
%\newcommand*{\ptsum}{$PT_{\rm sum}$}
\newcommand*{\ptsum}{$PT_{sum}$}
\newcommand*{\etsum}{$ET{\rm sum}$}
\newcommand*{\pthcut}{$p_T\!>\!0.9\,{\rm GeV/c}$}
\newcommand*{\ptlcut}{$p_T\!>\!0.5\,{\rm GeV/c}$}
\newcommand*{\etcut}{$E_T\!>\!0.1\,{\rm GeV}$}
\newcommand*{\etacut}{$|\eta|\!<\!1$}
\newcommand*{\aveN}{$\langle\!N_{\rm chg}\!\rangle$}
\newcommand*{\avept}{$\langle\!p_T\!\rangle$}
\newcommand*{\etaphi}{$\eta$-$\phi$}
\newcommand*{\delphi}{$\Delta\phi$}
\newcommand*{\absdelphi}{$|\Delta\phi|$}
\newcommand*{\delphicut}{$|\Delta\phi|>150^\circ$}
%\newcommand*{\nden}{$dN_{chg}/{d\eta}{d\phi}$}
\newcommand*{\nden}{$dN/{d\eta}{d\phi}$}
\newcommand*{\ndenpt}{$dN_{chg}/{d\eta}{d\phi}dp_T$}
%\newcommand*{\ndenpt}{$dN/{d\eta}{d\phi}dp_T$}
%\newcommand*{\ptden}{$dPT_{sum}/{d\eta}{d\phi}$}
\newcommand*{\ptden}{$dPT/{d\eta}{d\phi}$}
\newcommand*{\etden}{$dET_{sum}/{d\eta}{d\phi}$}
\newcommand*{\mpair}{$\mu^+\mu^-$}
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