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atlasphysics.sty
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atlasphysics.sty
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%
% atlasphysics.sty for ATLAS papers
%
% In your own directory, you may of course change this
% as you like. If you don't understand it or want to change
% or add something publicly, contact the ATLAS Publications
% Committee.
%
%
%\usepackage{xspace}
%
\let\sst=\scriptscriptstyle % Needed for some definitions (psi and eta prime, etc.) (EE)
\chardef\letterchar=11
\chardef\otherchar=12
\chardef\eolinechar=5
%
% +--------------------------------------------------------------------+
% | |
% | Hours:minutes macro |
% | |
% +--------------------------------------------------------------------+
%
\newcount\hrs\newcount\minu\newcount\temptime
\def\hm{\hrs=\time \divide\hrs by 60 \minu=\time\temptime=\hrs
\multiply\temptime by 60%
\advance\minu by -\temptime
\ifnum\minu<10 \let\zerofill=0\else \let\zerofill=\relax\fi
\the\hrs:\zerofill\the\minu}
%
% +--------------------------------------------------------------------+
% | |
% | My own stuff |
% | |
% +--------------------------------------------------------------------+
%
\def\bj{\ensuremath{b\mathrm{-jet}}}
\def\bjs{\ensuremath{b\mathrm{-jets}}}
\def\cj{\ensuremath{c\mathrm{-jet}}}
\def\cjs{\ensuremath{c\mathrm{-jets}}}
\newcommand{\pp}{\emph{pp}}
%
% +--------------------------------------------------------------------+
% | |
% | Analysis-specific shortcuts |
% | |
% +--------------------------------------------------------------------+
%
\def\mubar{\ensuremath{\langle\mu\rangle}}
\def\antikt{anti-\ensuremath{k_{t}}}
\def\dphi{\ensuremath{\Delta\phi}}
\def\mev{\ensuremath{\,\mathrm{MeV}}\ }
\def\gev{\ensuremath{\,\mathrm{GeV}}\ }
\def\tev{\ensuremath{\,\mathrm{TeV}}\ }
\def\ptzero{\ensuremath{p_{\mathrm{T}}^{0}}}
\def\ptone{\ensuremath{p_{\mathrm{T}}^{1}}}
\def\pttwo{\ensuremath{p_{\mathrm{T}}^{2}}}
\def\ptthree{\ensuremath{p_{\mathrm{T}}^{3}}}
\def\ptfour{\ensuremath{p_{\mathrm{T}}^{4}}}
\def\ptfive{\ensuremath{p_{\mathrm{T}}^{5}}}
\def\ptsix{\ensuremath{p_{\mathrm{T}}^{6}}}
\def\ptjet{\ensuremath{p_{\mathrm{T}}^{\mathrm{jet}}}}
\def\ptjeti{\ensuremath{p_{\mathrm{T}}^{\mathrm{jet},i}}}
\def\pthat{\ensuremath{\hat{\pT}}}
\def\trigc{{\tt EF\_j75\_a4tc\_EFFS\linebreak[1]\_xe45\_loose\_noMu}}
\def\mettrig2015{{\tt EF\_xe70\_tclcw}}
\def\mettrig2016{{\tt EF\_xe100\_mht}}
\newcommand{\ptmiss}{\ensuremath{\mathbf{p}_\mathrm{T}^\mathrm{miss}}\xspace}
\def\ptmisstrk{\ensuremath{\mathbf{p}_{\mathrm{T}}^{\mathrm{miss, track}}}}
%\def\totallumi{\ensuremath{\int\!\!{\cal L}\,dt = \left(20.5~\pm~0.7\right)\,\ifb}}
%\def\totalluminoerr{\ensuremath{\int\!\!{\cal L}\,dt = 20.5\,\ifb}}
%\def\totallumi{\ensuremath{\int\!\!{\cal L}\,dt = \left(20.3~\pm~0.7\right)\,\ifb}}
%\def\totallumi{\ensuremath{\int\!\!{\cal L}\,dt = \left(14.8~\pm~0.4\right)\,\ifb}}
%\def\totalluminoerr{\ensuremath{\int\!\!{\cal L}\,dt = 14.8\,\ifb}}
\def\totallumi{\ensuremath{\int\!\!{\cal L}\,dt = \left(36.1~\pm~1.2\right)\,\ifb}}
\def\totalluminoerr{\ensuremath{\int\!\!{\cal L}\,dt = 36.1\,\ifb}}
\def\lumi{\ensuremath{36.1\,\ifb}}
\def\stopLimLowLSP{\ensuremath{450\mathrm{-}950}}
\def\stopLimLowLSPLow{\ensuremath{450}}
\def\stopLimLowLSPHigh{\ensuremath{950}}
\def\stopLimDiag{\ensuremath{235\mathrm{-}590}}
\def\n90{\ensuremath{n_{90}}}
\def\fqual{\ensuremath{f_{\mathrm{quality}}}}
\def\fqualhec{\ensuremath{f_{\mathrm{quality,HEC}}}}
\def\fem{\ensuremath{f_{\mathrm{EM}}}}
\def\fch{\ensuremath{f_{\mathrm{ch}}}}
\def\fhec{\ensuremath{f_{\mathrm{HEC}}}}
\def\fmax{\ensuremath{f_{\mathrm{max}}}}
\def\tjet{\ensuremath{t_{\mathrm{jet}}}}
\def\tNj{\ensuremath{t_{N_j}}}
\def\cms{\ensuremath{7\tev}}
\def\sumet{\ensuremath{\Sigma E_T}}
%\def\metsig{\ensuremath{\met / \frac{1}{2}\sqrt{\sumet}}}
\def\metsig{\ensuremath{\met / \sqrt{\sumet}}}
\def\ns{\ensuremath{\,\mathrm{ns}}}
\def\mt{\ensuremath{m_{\mathrm{T}}}}
\def\mT{\mt}
\def\mttwo{\ensuremath{m_{\mathrm{T2}}^{\chi^2}}}
\def\meff{\ensuremath{m_{\mathrm{eff}}}}
\def\dphijetmet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet},\met\right)\right|}}
\def\dphijetimet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^i,\met\right)\right|}}
%\def\dphijettwomet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^{0,1},\met\right)\right|}}
\def\dphijettwomet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^{0,1},\ptmiss\right)\right|}}
%\def\dphijetthreemet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^{0,1,2},\met\right)\right|}}
\def\dphijetthreemet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^{0,1,2},\ptmiss\right)\right|}}
\def\dphijetzeromet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^0,\met\right)\right|}}
\def\dphijetonemet{\ensuremath{\left|\Delta\phi\left(\mathrm{jet}^1,\met\right)\right|}}
%\def\mindphijetthreemet{\ensuremath{\min \left|\Delta\phi\left(\mathrm{jet}^{0-2},\met\right)\right|}}
\def\mindphijetthreemet{\ensuremath{\min \left|\Delta\phi\left(\mathrm{jet}^{0-2},\ptmiss\right)\right|}}
%\def\mindphijettwomet{\ensuremath{\min \left|\Delta\phi\left(\mathrm{jet}^{0-1},\met\right)\right|}}
\def\mindphijettwomet{\ensuremath{\min \left|\Delta\phi\left(\mathrm{jet}^{0-1},\ptmiss\right)\right|}}
%\def\dphimettrk{\ensuremath{\left|\Delta\phi\left(\met,\mettrk\right)\right|}}
\def\dphimettrk{\ensuremath{\left|\Delta\phi\left(\ptmiss,\ptmisstrk\right)\right|}}
\def\dphiWmet{\ensuremath{\left|\Delta\phi\left(\Wboson_{\mathrm{away}},\met\right)\right|}}
\def\dphibb{\ensuremath{\left|\Delta\phi\left(b,b\right)\right|}}
\def\drbb{\ensuremath{\Delta R\left(b,b\right)}}
\def\mbb{\ensuremath{m_{bb}}}
\def\drblmin{\ensuremath{\Delta R\left(b,\ell\right)_{\mathrm{min}}}}
\def\mttaumet{\ensuremath{\mt\left(\tau\,\mathrm{candidate},\met\right)}}
\def\fakemet{\ensuremath{E_{\mathrm{T}}^{\mathrm{miss, fake}}}}
\def\mettrk{\ensuremath{E_{\mathrm{T}}^{\mathrm{miss, track}}}}
\def\mbyptjets{\ensuremath{m_{\mathrm{jets}}/\left|\vec{p}_{\mathrm{T,jets}}\right|}}
\def\drmin{\ensuremath{\Delta R_{\mathrm{min}}}}
\def\drbmin{\ensuremath{\Delta R_{b,\mathrm{min}}}}
\def\mtopcand{\ensuremath{m_{jjj}}}
\def\mtopcandzero{\ensuremath{m^{0}_{jjj}}}
\def\mtopcandone{\ensuremath{m^{1}_{jjj}}}
\def\mtopcandaway{\ensuremath{m_{jjj}^{\mathrm{away}}}}
\def\pttopcand{\ensuremath{p_{\mathrm{T},jjj}}}
%\def\minmtjfourmet{\ensuremath{\min\left[\mt\left(\textrm{jet}^{0-3},\met\right)\right]}}
\def\mtjetmet{\ensuremath{\mt\left(\textrm{jet},\met\right)}}
%\def\mtjetimet{\ensuremath{\mt\left(\textrm{jet}^i,\met\right)}}
\def\mtjetimet{\ensuremath{m_{\mathrm{T}}^{i}}}
\def\mtlepmet{\ensuremath{\mt\left(\ell,\met\right)}}
%\def\minmtjfourmet{\ensuremath{\min\left[m_{\mathrm{T}}^{i}]}}
\def\minmtjfourmet{\ensuremath{\min(m_{\mathrm{T}}^{i})}}
\newcommand{\ptb}{\ensuremath{p_\mathrm{T}^b}\xspace}
\newcommand{\ptbzero}{\ensuremath{p_{\mathrm{T}}^{0,b}}}
\newcommand{\ptbone}{\ensuremath{p_{\mathrm{T}}^{1,b}}}
\newcommand{\vecptb}{\ensuremath{\mathbf{p}_\mathrm{T}^b}\xspace}
\newcommand{\vecpt}{\ensuremath{\mathbf{p}_\mathrm{T}}\xspace}
\def\mtbmin{\ensuremath{m_{\mathrm{T}}^{b,\mathrm{min}}}}
\def\mtbmax{\ensuremath{m_{\mathrm{T}}^{b,\mathrm{max}}}}
\def\mtbminprime{\ensuremath{m_{\mathrm{T}}^{b,\mathrm{min'}}}}
\def\mtbmaxprime{\ensuremath{m_{\mathrm{T}}^{b,\mathrm{max'}}}}
\def\mtbmetmindphi{\ensuremath{\mt\left(b_{\min[\Delta\phi \left(b,\met\right)]},\met\right)}}
\def\mtbmetmaxdphi{\ensuremath{\mt\left(b_{\max[\Delta\phi \left(b,\met\right)]},\met\right)}}
\def\mtjmetmindphi{\ensuremath{\mt\left(j_{\min[\Delta\phi \left(j,\met\right)]},\met\right)}}
\def\drbjetbjet{\ensuremath{\Delta R\left(b,b\right)}}
\def\mbjetbjet{\ensuremath{m\left(b,b\right)}}
\def\topmassasym{\ensuremath{\mathcal{A}_{m_t}}}
\def\htsig{\ensuremath{\met/\sqrt{\HT}}}
\def\htsigprime{\ensuremath{\metprime/\sqrt{\HT}}}
\def\mantikttwelve{\ensuremath{m_{\mathrm{jet,}R=1.2}}}
\def\mantikttwelvezero{\ensuremath{m^{0}_{\mathrm{jet,}R=1.2}}}
\def\mantikttwelveone{\ensuremath{m^{1}_{\mathrm{jet,}R=1.2}}}
\def\mantikteight{\ensuremath{m_{\mathrm{jet,}R=0.8}}}
\def\mantikteightzero{\ensuremath{m^{0}_{\mathrm{jet,}R=0.8}}}
\def\mantikteightone{\ensuremath{m^{1}_{\mathrm{jet,}R=0.8}}}
\def\ptantikttwelve{\ensuremath{p^_{\mathrm{T},\mathrm{akt}12}}}
\def\ptantikttwelvezero{\ensuremath{p^{0}_{\mathrm{T},\mathrm{akt}12}}}
\def\ptantikttwelveone{\ensuremath{p_{0}{\mathrm{T},\mathrm{akt}12}}}
\def\ptantikteight{\ensuremath{p^_{\mathrm{T},\mathrm{akt}8}}}
\def\ptantikteightzero{\ensuremath{p^{0}_{\mathrm{T},\mathrm{akt}8}}}
\def\ptantikteightone{\ensuremath{p^{1}_{\mathrm{T},\mathrm{akt}8}}}
\def\mtuntagmetmindphi{\ensuremath{\mt\left(jet^{untag}_{\min[\Delta\phi \left(jet^{untag},\met\right)]},\met\right)}}
\def\mtlowestptmet{\ensuremath{\mt\left(jet_{lowest-\pt},\met\right)}}
\def\mindrblep{\ensuremath{\Delta R(b_{0,1},\ell)_{\mathrm{min}}}}
\def\nBJet{\ensuremath{N_{b\mathrm{-jet}}}}
\def\mS{\ensuremath{m_{\mathrm{S}}}}
\def\mV{\ensuremath{m_{\mathrm{V}}}}
\def\mISR{\ensuremath{m_{\mathrm{ISR}}}}
\def\mcm{\ensuremath{m_{\mathrm{CM}}}}
\def\nJetS{\ensuremath{N_{\mathrm{jet}}^{\mathrm{S}}}}
\def\nBJetS{\ensuremath{N_{b\mathrm{-jet}}^{\mathrm{S}}}}
\def\pTSBZero{\ensuremath{p_{\mathrm{T},b}^{0,\mathrm{S}}}}
\def\mTS{\ensuremath{m_{\mathrm{T}}^{\mathrm{S}}}}
\def\dPhiISRMET{\ensuremath{\Delta\phi_{\mathrm{ISR},\met}}}
\def\pTISR{\ensuremath{\pt^{\mathrm{ISR}}}}
\def\pTSFour{\ensuremath{\pt^{4,\mathrm{S}}}}
\def\pTSThree{\ensuremath{\pt^{3,\mathrm{S}}}}
\def\rISR{\ensuremath{R_{\mathrm{ISR}}}}
\def\PTISR{\ensuremath{\pT^{\mathrm{ISR}}}\xspace}
\def\RISR{\ensuremath{R_{\mathrm{ISR}}}\xspace}
\def\dphiISRI{\ensuremath{\Delta\phi_{\mathrm{ISR}}}\xspace}
\def\NbV{\ensuremath{N_{b\textrm{-tag}}^{\mathrm{S}}}\xspace}
\def\NjV{\ensuremath{N_{\mathrm{jet}}^{\mathrm{S}}}\xspace}
\def\NbISR{\ensuremath{N_{b\textrm{-tag}}^{\mathrm{ISR}}}\xspace}
\def\NjISR{\ensuremath{N_{\mathrm{jet}}^{\mathrm{ISR}}}\xspace}
\def\MS{\ensuremath{M_{\mathrm{T}}^{S}}\xspace}
\def\MV{\ensuremath{M_{\mathrm{T}}^{S,\mathrm{Vis}}}\xspace}
\def\pTjV{\ensuremath{\pT^{\mathrm{jet\,4},S}}\xspace}
\def\pTbV{\ensuremath{\pT^{b\textrm{-tag},S}}\xspace}
\def\mstop{\ensuremath{m_{\stop}}}
\def\mstopone{\ensuremath{m_{\tilde{t}_1}}}
\def\mninoone{\ensuremath{m_{\ninoone}}}
\def\msbottom{\ensuremath{m_{\sbottom}}}
\def\mqlthree{\ensuremath{m_{\tilde{qL3}}}}
\def\mtr{\ensuremath{m_{\tilde{tR}}}}
\def\mone{\ensuremath{M_{1}}}
\def\mtwo{\ensuremath{M_{2}}}
\def\mthree{\ensuremath{M_{3}}}
\def\ms{\ensuremath{M_{S}}}
\def\xtms{\ensuremath{X_{t}/M_{S}}}
\def\at{\ensuremath{A_{t}}}
\def\tanb{\ensuremath{\mathrm{tan}\beta}}
\def\mgluino{\ensuremath{m_{\gluino}}}
\def\mLSP{\ensuremath{m_{\nino}}}
\def\LSP{\ninoone}
\def\SRA{Signal Region A}
\def\SRB{Signal Region B}
\def\SRC{Signal Region C}
\def\SRD{Signal Region D}
\def\SRE{Signal Region E}
\def\SRF{Signal Region F}
\def\CRgamma{CR{\ensuremath{\gamma}}}
\def\SRBoost{SRF}
\def\SRI{I}
\def\SRII{II}
\def\SRIII{III}
\def\mcatnloSF{0.88}
\def\alpSF{0.65}
\def\ttV{\ttbar+\Wboson/\Zboson}
\def\ttW{\ttbar+\Wboson}
\def\ttZ{\ttbar+\Zboson}
\def\ttgamma{\ttbar+\ensuremath{\gamma}}
\def\Vjets{\ensuremath{\Wboson/\Zboson\,+\,\mathrm{jets}}}
\def\Wjets{\ensuremath{\Wboson\,+\,\mathrm{jets}}}
\def\Wenujets{\ensuremath{\Wboson(\to e\nu)\,+\,\mathrm{jets}}}
\def\Wmunujets{\ensuremath{\Wboson(\to \mu\nu)\,+\,\mathrm{jets}}}
\def\Wtaunujets{\ensuremath{\Wboson(\to\tau\nu)\,+\,\mathrm{jets}}}
\def\Zjets{\ensuremath{\Zboson\,+\,\mathrm{jets}}}
\def\Zeejets{\ensuremath{\Zboson(\to ee)\,+\,\mathrm{jets}}}
\def\Zmumujets{\ensuremath{\Zboson(\to\mu\mu)\,+\,\mathrm{jets}}}
\def\Ztautaujets{\ensuremath{\Zboson(\to\tau\tau)\,+\,\mathrm{jets}}}
\def\Znunujets{\ensuremath{\Zboson(\to\nu\nu)\,+\,\mathrm{jets}}}
\def\gammajets{\ensuremath{\gamma+\mathrm{jets}}}
\def\mtopval{\ensuremath{171.2\gev}}
\def\mtoplow{\ensuremath{80\gev}}
\def\mtophigh{\ensuremath{270\gev}}
\def\fastjet{FASTJET}
\def\geant{GEANT}
\def\afii{AFII}
\def\pythia{PYTHIA}
\def\powheg{PowHeg}
\def\mcatnlo{MC@NLO}
\def\pythiaeight{PYTHIA8}
\def\herwig{HERWIG}
\def\jimmy{JIMMY}
\def\herwigpp{HERWIG++}
\def\alpgen{ALPGEN}
\def\sherpa{SHERPA}
\def\acer{ACER MC}
\def\madgraph{MadGraph}
\def\nllfast{{\tt NLL-fast}}
%
% +--------------------------------------------------------------------+
% | |
% | Useful symbols for use in or out of math mode |
% | |
% +--------------------------------------------------------------------+
%
\def\ra{\ensuremath{\rightarrow}}% "GOES TO" arrow.
\def\la{\ensuremath{\leftarrow}}% "GETS" arrow.
\let\rarrow=\ra
\let\larrow=\la
\def\lapprox{\ensuremath{\sim\kern-1em\raise 0.65ex\hbox{$<$}}}% Or use \lsim
\def\rapprox{\ensuremath{\sim\kern-1em\raise 0.65ex\hbox{$>$}}}% and \rsim.
\def\gam{\ensuremath{\gamma}}
\def\rts {\ensuremath{\sqrt{s}}}
\def\stat{\mbox{$\;$(stat.)}}
\def\syst{\mbox{$\;$(syst.)}}
%
% +--------------------------------------------------------------------+
% | |
% | sin2thetaW m_W m_Z etc. |
% | |
% +--------------------------------------------------------------------+
%
\def\Mtau{\ensuremath{m_{\tau}}}
\def\swsq{\ensuremath{\sin^2\!\theta_{W}}}
\def\swel{\ensuremath{\sin^2\!\theta_{\mathrm{eff}}^{\mathrm{lept}}}}
\def\swsqb{\ensuremath{\sin^2\!\overline{\theta}_{W}}}
\def\swsqon{\ensuremath{\swsq\equiv 1-\mW^2/\mZ^2}} % Lower-case masses (EE)
\def\gv{\ensuremath{g_{\mathrm{V}}}} % Subscripts roman not italic (EE)
\def\ga{\ensuremath{g_{\mathrm{A}}}} % Subscripts roman not italic (EE)
\def\gvbar{\ensuremath{\bar{g}_\mathrm{V}}} % Subscripts roman not italic (EE)
\def\gabar{\ensuremath{\bar{g}_\mathrm{A}}} % Subscripts roman not italic (EE)
%
% +--------------------------------------------------------------------+
% | |
% | Particle-antiparticle pair notations |
% | |
% +--------------------------------------------------------------------+
%
\def\antibar#1{\ensuremath{#1\bar{#1}}}
\def\tbar{\ensuremath{\bar{t}}}
\def\ttbar{\antibar{t}}
\def\bbar{\ensuremath{\bar{b}}}
\def\bbbar{\antibar{b}}
\def\cbar{\ensuremath{\bar{c}}}
\def\ccbar{\antibar{c}}
\def\sbar{\ensuremath{\bar{s}}}
\def\ssbar{\antibar{s}}
\def\ubar{\ensuremath{\bar{u}}}
\def\uubar{\antibar{u}}
\def\dbar{\ensuremath{\bar{d}}}
\def\ddbar{\antibar{d}}
\def\fbar{\ensuremath{\bar{f}}}
\def\ffbar{\antibar{f}}
\def\qbar{\ensuremath{\bar{q}}}
\def\qqbar{\antibar{q}}
\def\nbar{\ensuremath{\bar{\nu}}}
\def\nnbar{\antibar{\nu}}
%
% +--------------------------------------------------------------------+
% | |
% | e+e-, etc. |
% | |
% +--------------------------------------------------------------------+
%
\def\ee{\ensuremath{e^+ e^-}}%
\def\epm{\ensuremath{e^{\pm}}}%
\def\epem{\ensuremath{e^+ e^-}}%
\def\mumu{\ensuremath{\mathrm{\mu^+ \mu^-}}}%
\def\tautau{\ensuremath{\mathrm{\tau^+ \tau^-}}}%
\let\muchless=\ll
\def\ll{\ensuremath{\ell^+ \ell^-}}%
\def\lnu{\ensuremath{\ell \nu}}%
%
% +--------------------------------------------------------------------+
% | |
% | Useful Z0 type stuff Gammas, asymmetries |
% | |
% +--------------------------------------------------------------------+
\def\Zzero{\ensuremath{Z}}
\def\Zboson{\ensuremath{Z}}
\def\Wplus{\ensuremath{W^+}}
\def\Wminus{\ensuremath{W^-}}
\def\Wboson{\ensuremath{W}}%
\def\Wpm{\ensuremath{W^{\pm}}}%
\def\Wmp{\ensuremath{W^{\mp}}}%
\def\Zzv{\ensuremath{\Zzero^{\textstyle *}}}
\def\Abb{\ensuremath{A_{\bbbar}}}
\def\Acc{\ensuremath{A_{\ccbar}}}
\def\Aqq{\ensuremath{A_{\qqbar}}}
\def\Afb{\ensuremath{A_{{fb}}}} % Subscript italic not roman (EE)
\def\GZ{\ensuremath{\Gamma_{Z}}}
\def\GW{\ensuremath{\Gamma_{W}}}
\def\GH{\ensuremath{\Gamma_{H}}}
\def\GamHad{\ensuremath{\Gamma_{\mathrm{had}}}}
\def\Gbb{\ensuremath{\Gamma_{\bbbar}}}
\def\Rbb{\ensuremath{R_{\bbbar}}}
\def\Gcc{\ensuremath{\Gamma_{\ccbar}}}
\def\Gvis{\ensuremath{\Gamma_{\mathrm{vis}}}}
\def\Ginv{\ensuremath{\Gamma_{\mathrm{inv}}}}
% +--------------------------------------------------------------------+
% | |
% | B-physics |
% | |
% +--------------------------------------------------------------------+
%
\def\Bstar{\ensuremath{B^{*}}}
\def\chic{\ensuremath{\raise.4ex\hbox{$\chi$}_{{c}}}} % Raised & tightened, as chib (EE)
\def\BoBo{\ensuremath{B^{0}\mbox{--}\bar{B}^{0}}} % en-dash not hyphen (EE)
\def\BodBod{\ensuremath{B^{0}_{d}\mbox{--}\bar{B}^{0}_{d}}} % en-dash not hyphen (EE)
\def\BosBos{\ensuremath{B^{0}_{s}\mbox{--}\bar{B}^{0}_{s}}} % en-dash not hyphen (EE)
\def\chib{\ensuremath{\raise.4ex\hbox{$\chi$}_{{b}}}} % Bit of space removed (EE)
\def\Epsb {\ensuremath{\epsilon_{b}}} % Subscript italic not roman (EE)
\def\Epsc {\ensuremath{\epsilon_{c}}} % Subscript italic not roman (EE)
\def\Kstar {\ensuremath{K^{*}}}
\def\Dstar {\ensuremath{D^{*}}} % Italic not roman (EE)
\def\Dsstar {\ensuremath{D^{**}}} % Italic not roman (EE)
\def\etpt {\ensuremath{1/p_{\mathrm{T}} - 1/E_{\mathrm{T}}}}
% p not P, and subscripts roman not italic (EE)
\def\etptsig {\ensuremath{(1/p_{\mathrm{T}} - 1/E_{\mathrm{T}})/(\sigma(1/p_{\mathrm{T}}))}}
% p not P, and subscripts roman not italic (EE)
\newcommand{\Bd} {\ensuremath{B_d^0}}
\newcommand{\Bs} {\ensuremath{B_s^0}}
\newcommand{\Bu} {\ensuremath{B_u}}
\newcommand{\Bc} {\ensuremath{B_c}}
\newcommand{\Lb} {\ensuremath{\Lambda_b}}
\newcommand{\btol} {\ensuremath{b \rightarrow \ell}} % Italic not roman (EE)
\newcommand{\ctol} {\ensuremath{c \rightarrow \ell}} % Italic not roman (EE)
\newcommand{\btoctol} {\ensuremath{b \rightarrow c \rightarrow \ell}} % Italic not roman (EE)
%
% +--------------------------------------------------------------------+
% | |
% | J/psi, psi prime, etc. |
% | |
% +--------------------------------------------------------------------+
%
\let\psii=\psi % Save normal "\psi" definition, since I redefine it.
%\def\psi{\ensuremath{\psii}}%
\def\jpsi{\ensuremath{J/\psi}}
\def\Jpsi{\ensuremath{J/\psi}}
\def\Jee{\ensuremath{\Jpsi\ra\epem}}
\def\Jmm{\ensuremath{\Jpsi\ra\mu\mu}}
\def\Jmumu{\ensuremath{\Jpsi\ra\mumu}}
\def\Brjl{\ensuremath{\mathrm{Br}(\Jpsi \ra \ll)}} % Italic not roman (EE)
\def\psip{\ensuremath{\psi^{\sst\prime}}}
%
% +--------------------------------------------------------------------+
% | |
% | QCD (Simplified all of these: no hbox, etc.) (EE) |
% | |
% +--------------------------------------------------------------------+
%
\def\alphas{\ensuremath{\alpha_{\mathrm{S}}}} % Subscript roman not italic (EE)
\def\NF{\ensuremath{N_{\mathrm{F}}}}
\def\NC{\ensuremath{N_{\mathrm{C}}}}
\def\CF{\ensuremath{C_{\mathrm{F}}}}
\def\CA{\ensuremath{C_{\mathrm{A}}}}
\def\TF{\ensuremath{T_{\mathrm{F}}}}
\def\Lms{\ensuremath{\Lambda_{\overline{\mathrm{MS}}}}}
\def\Lmsfive{\ensuremath{\Lambda^{(5)}_{\overline{\mathrm{MS}}}}}
\def\KT{\ensuremath{k_{\perp}}}
%
% +--------------------------------------------------------------------+
% | |
% | CKM matrix |
% | |
% +--------------------------------------------------------------------+
%
\def\Vcb{\ensuremath{\vert V_{cb} \vert}}
\def\Vub{\ensuremath{\vert V_{ub} \vert}}
\def\Vtd{\ensuremath{\vert V_{td} \vert}}
\def\Vts{\ensuremath{\vert V_{ts} \vert}}
\def\Vtb{\ensuremath{\vert V_{tb} \vert}}
\def\Vcs{\ensuremath{\vert V_{cs} \vert}}
\def\Vud{\ensuremath{\vert V_{ud} \vert}}
\def\Vus{\ensuremath{\vert V_{us} \vert}}
\def\Vcd{\ensuremath{\vert V_{cd} \vert}}
%
% +--------------------------------------------------------------------+
% | |
% | New particle stuff |
% | |
% +--------------------------------------------------------------------+
%
\def\Azero{\ensuremath{A^0}}%
\def\hzero{\ensuremath{h^0}}%
\def\Hzero{\ensuremath{H^0}}%
\def\Hboson{\ensuremath{H}}%
\def\Hplus{\ensuremath{H^+}}%
\def\Hminus{\ensuremath{H^-}}%
\def\Hpm{\ensuremath{H^{\pm}}}%
\def\Hmp{\ensuremath{H^{\mp}}}%
\def\susy#1{\ensuremath{\tilde{#1}}}%
\def\ellell{\ensuremath{\mathrm{\ell^+ \ell^-}}}%
\def\ggino{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi$}}}}
\def\chinop{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^+$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^+$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^+$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^+$}}}}
\def\chinom{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^-$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^-$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^-$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^-$}}}}
\def\chinopm{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^\pm$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^\pm$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^\pm$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^\pm$}}}}
\def\chinomp{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^\mp$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^\mp$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^\mp$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^\mp$}}}}
\def\chinoonep{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^+_1$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^+_1$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^+_1$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^+_1$}}}}
\def\chinoonem{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^-_1$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^-_1$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^-_1$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^-_1$}}}}
\def\chinoonepm{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^\pm_1$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^\pm_1$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^\pm_1$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^\pm_1$}}}}
\def\chinotwop{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^+_2$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^+_2$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^+_2$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^+_2$}}}}
\def\chinotwom{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^-_2$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^-_2$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^-_2$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^-_2$}}}}
\def\chinotwopm{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^\pm_2$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^\pm_2$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^\pm_2$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^\pm_2$}}}}
\def\nino{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^0$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^0$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^0$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^0$}}}}
\def\ninoone{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^0_1$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^0_1$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^0_1$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^0_1$}}}}
\def\ninotwo{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^0_2$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^0_2$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^0_2$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^0_2$}}}}
\def\ninothree{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^0_3$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^0_3$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^0_3$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^0_3$}}}}
\def\ninofour{\ensuremath{\mathchoice%
{\displaystyle\raise.4ex\hbox{$\displaystyle\tilde\chi^0_4$}}%
{\textstyle\raise.4ex\hbox{$\textstyle\tilde\chi^0_4$}}%
{\scriptstyle\raise.3ex\hbox{$\scriptstyle\tilde\chi^0_4$}}%
{\scriptscriptstyle\raise.3ex\hbox{$\scriptscriptstyle\tilde\chi^0_4$}}}}
\def\gravino{\ensuremath{\tilde{G}}}%
\def\Zprime{\ensuremath{Z^\prime}}
\def\Zstar{\ensuremath{Z^{*}}}
\def\squark{\ensuremath{\tilde{q}}}
\def\squarkL{\ensuremath{\tilde{q}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\squarkR{\ensuremath{\tilde{q}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\gluino{\ensuremath{\tilde{g}}}
\def\stop{\ensuremath{\tilde{t}}}
\def\stopone{\ensuremath{\tilde{t}_1}}
\def\stoptwo{\ensuremath{\tilde{t}_2}}
\def\stopL{\ensuremath{\tilde{t}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\stopR{\ensuremath{\tilde{t}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\sbottom{\ensuremath{\tilde{b}}}
\def\sbottomone{\ensuremath{\tilde{b}_1}}
\def\sbottomtwo{\ensuremath{\tilde{b}_2}}
\def\sbottomL{\ensuremath{\tilde{b}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\sbottomR{\ensuremath{\tilde{b}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\slepton{\ensuremath{\tilde{\ell}}}
\def\sleptonL{\ensuremath{\tilde{\ell}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\sleptonR{\ensuremath{\tilde{\ell}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\sel{\ensuremath{\tilde{e}}}
\def\selL{\ensuremath{\tilde{e}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\selR{\ensuremath{\tilde{e}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\smu{\ensuremath{\tilde{\mu}}}
\def\smuL{\ensuremath{\tilde{\mu}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\smuR{\ensuremath{\tilde{\mu}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\stau{\ensuremath{\tilde{\tau}}}
\def\stauL{\ensuremath{\tilde{\tau}_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\stauR{\ensuremath{\tilde{\tau}_{\mathrm{R}}}} % Subscript roman not italic (EE)
\def\stauone{\ensuremath{\tilde{\tau}_1}}
\def\stautwo{\ensuremath{\tilde{\tau}_2}}
\def\snu{\ensuremath{\tilde{\nu}}}
%
% +--------------------------------------------------------------------+
% | |
% | pi, pi0, pi+, pi-, pi+-, eta, eta1, etc. |
% | |
% +--------------------------------------------------------------------+
%
\let\pii=\pi
%\def\pi{\ensuremath{\pii}}%
\def\pizero{\ensuremath{\pii^0}}%
\def\piplus{\ensuremath{\pii^+}}%
\def\piminus{\ensuremath{\pii^-}}%
\def\pipm{\ensuremath{\pii^{\pm}}}%
\def\pimp{\ensuremath{\pii^{\mp}}}%
\let\etaa=\eta
%\def\eta{\ensuremath{\etaa}}%
\def\etaprime{\ensuremath{\eta^{\sst\prime}}}%
%
% +--------------------------------------------------------------------+
% | |
% | K0, K+, K-, K0L, K0S |
% | |
% +--------------------------------------------------------------------+
%
\def\kzero{\ensuremath{K^0}}%
\def\kzerobar{\ensuremath{\overline{K}\vphantom{K}^0}}%
%
\def\kaon{\ensuremath{K}}%
\def\kplus{\ensuremath{K^+}}%
\def\kminus{\ensuremath{K^-}}%
\def\kzeroL{\ensuremath{K^0_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\kzerol{\ensuremath{K^0_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\klong{\ensuremath{K^0_{\mathrm{L}}}} % Subscript roman not italic (EE)
\def\kzeroS{\ensuremath{K^0_{\mathrm{S}}}} % Subscript roman not italic (EE)
\def\kzeros{\ensuremath{K^0_{\mathrm{S}}}} % Subscript roman not italic (EE)
\def\kshort{\ensuremath{K^0_{\mathrm{S}}}} % Subscript roman not italic (EE)
%
% +--------------------------------------------------------------------+
% | |
% | Upsilons of various sorts |
% | |
% +--------------------------------------------------------------------+
%
\def\Ups{\ensuremath{\mit\Upsilon}} % Should be italic (EE)
\def\Upsp{\ensuremath{\mit\Upsilon^{\sst\prime}}} % Should be italic (EE)
\def\Upspp{\ensuremath{\mit\Upsilon^{\sst\prime\prime}}} % Should be italic (EE)
\def\Upsppp{\ensuremath{\mit\Upsilon^{\sst\prime\prime\prime}}} % Should be italic (EE)
\def\Upspppp{\ensuremath{\mit\Upsilon^{\sst\prime\prime\prime\prime}}} % Should be italic (EE)
\def\itUpsp{\ensuremath{\mit\Upsilon^{\sst\prime}}}%
\def\UoneS{\ensuremath{\Upsilon(\mathrm{1S})}}%
%
% +--------------------------------------------------------------------+
% | |
% | Things like \ups4 --> Y(4S) |
% | |
% +--------------------------------------------------------------------+
%
\def\ups#1{\ensuremath{\mit{\Upsilon}(\mathrm{#1S})}} % Italic, fixed and simplified (EE)
%
% +--------------------------------------------------------------------+
% | |
% | Notation for the P-lines: \nspj211 --> 2 1P1, etc. |
% | |
% +--------------------------------------------------------------------+
%
\def\nsPj#1#2#3{\ensuremath{#1\,^{#2}\!P_{#3}}}%
\let\nspj=\nsPj
\def\nsSj#1#2#3{\ensuremath{#1\,^{#2}\!S_{#3}}}%
\let\nssj=\nsSj
%
% +--------------------------------------------------------------------+
% | |
% | Useful things for proton-proton physics |
% | |
% +--------------------------------------------------------------------+
%
\def\pt{\ensuremath{p_{\mathrm{T}}}} % Subscript roman not italic (EE)
\def\pT{\ensuremath{p_{\mathrm{T}}}} % Subscript roman not italic (EE)
\def\et{\ensuremath{E_{\mathrm{T}}}} % Subscript roman not italic (EE)
\def\eT{\ensuremath{E_{\mathrm{T}}}} % Subscript roman not italic (EE)
\def\ET{\ensuremath{E_{\mathrm{T}}}} % Subscript roman not italic (EE)
\def\HT{\ensuremath{H_{\mathrm{T}}}} % Subscript roman not italic (EE)
\def\ptsq{\ensuremath{p^2_{\mathrm{T}}}} % Fixed so it works correctly (EE)
\def\degr{\ensuremath{^\circ}} % Removed mbox - caused problems and not needed (EE)
\def\abseta{\ensuremath{|\eta|}}
\def\Hgg{\ensuremath{H\to\gamma\gamma}}
\def\mh{\ensuremath{m_h}}
\def\mW{\ensuremath{m_W}}
\def\mZ{\ensuremath{m_Z}}
\def\mH{\ensuremath{m_H}}
\def\mA{\ensuremath{m_A}}
\def\MET{\ensuremath{E_{\mathrm{T}}^{\mathrm{miss}}}} % Sub/superscript roman not italic (EE)
\def\met{\ensuremath{E_{\mathrm{T}}^{\mathrm{miss}}}} % Sub/superscript roman not italic (EE)
\def\metprime{\ensuremath{E_{\mathrm{T}}^{\mathrm{miss'}}}} % Sub/superscript roman not italic (EE) added \metprime definition
\def\Wjj{\ensuremath{W \rightarrow jj}}
\def\tjjb{\ensuremath{t \rightarrow jjb}}
\def\Hbb{\ensuremath{H \rightarrow b\bar b}}
\def\Zmm{\ensuremath{Z \rightarrow \mu\mu}}
\def\Zee{\ensuremath{Z \rightarrow ee}}
\def\Zll{\ensuremath{Z \rightarrow \ell\ell}}
\def\Znunu{\ensuremath{Z \rightarrow \nu\bar{\nu}}}
\def\Wln{\ensuremath{W \rightarrow \ell\nu}}
\def\Wen{\ensuremath{W \rightarrow e\nu}}
\def\Wmn{\ensuremath{W \rightarrow \mu\nu}}
\def\Hllll{\ensuremath{H \rightarrow ZZ^{(*)} \rightarrow \mu\mu\mu\mu}}
\def\Hmmmm{\ensuremath{H \rightarrow \mu\mu\mu\mu}}
\def\Heeee{\ensuremath{H \rightarrow eeee}}
\def\Amm{\ensuremath{A \rightarrow \mu\mu}}
\def\Ztau{\ensuremath{Z \rightarrow \tau\tau}}
\def\Wtau{\ensuremath{W \rightarrow \tau\nu}}
\def\Atau{\ensuremath{A \rightarrow \tau\tau}}
\def\Htau{\ensuremath{H \rightarrow \tau\tau}}
\def\begL{10$^{31}$~cm$^{-2}$~s$^{-1}$}
\def\lowL{10$^{33}$~cm$^{-2}$~s$^{-1}$}
\def\highL{10$^{34}$~cm$^{-2}$~s$^{-1}$}
\newcommand{\EjetRec}{\ensuremath{E_{\mathrm{rec}}}} % Subscript roman not italic (EE)
\newcommand{\PjetRec}{\ensuremath{p_{\mathrm{rec}}}} % Subscript roman not italic (EE)
\newcommand{\EjetTru}{\ensuremath{E_{\mathrm{truth}}}} % Subscript roman not italic (EE)
\newcommand{\PjetTru}{\ensuremath{p_{\mathrm{truth}}}} % Subscript roman not italic (EE)
\newcommand{\EjetDM}{\ensuremath{E_{\mathrm{DM}}}} % Subscript roman not italic (EE)
\newcommand{\Rcone}{\ensuremath{R_{\mathrm{cone}}}} % Subscript roman not italic (EE)
%
% +--------------------------------------------------------------------+
% | |
% | Some useful units |
% | |
% +--------------------------------------------------------------------+
%
\def\TeV{\ifmmode {\mathrm{\ Te\kern -0.1em V}}\else
\textrm{Te\kern -0.1em V}\fi}%
\def\GeV{\ifmmode {\mathrm{\ Ge\kern -0.1em V}}\else
\textrm{Ge\kern -0.1em V}\fi}%
\def\MeV{\ifmmode {\mathrm{\ Me\kern -0.1em V}}\else
\textrm{Me\kern -0.1em V}\fi}%
\def\keV{\ifmmode {\mathrm{\ ke\kern -0.1em V}}\else
\textrm{ke\kern -0.1em V}\fi}%
\def\eV{\ifmmode {\mathrm{\ e\kern -0.1em V}}\else
\textrm{e\kern -0.1em V}\fi}%
\let\tev=\TeV
\let\gev=\GeV
\let\mev=\MeV
\let\kev=\keV
\let\ev=\eV
\def\TeVc{\ifmmode {\mathrm{\ Te\kern -0.1em V}/c}\else
{\textrm{Te\kern -0.1em V}/$c$}\fi}%
\def\GeVc{\ifmmode {\mathrm{\ Ge\kern -0.1em V}/c}\else
{\textrm{Ge\kern -0.1em V}/$c$}\fi}%
\def\MeVc{\ifmmode {\mathrm{\ Me\kern -0.1em V}/c}\else
{\textrm{Me\kern -0.1em V}/$c$}\fi}%
\def\keVc{\ifmmode {\mathrm{\ ke\kern -0.1em V}/c}\else
{\textrm{ke\kern -0.1em V}/$c$}\fi}%
\def\eVc{\ifmmode {\mathrm{\ e\kern -0.1em V}/c}\else
{\textrm{e\kern -0.1em V}/$c$}\fi}%
\let\tevc=\TeVc
\let\gevc=\GeVc
\let\mevc=\MeVc
\let\kevc=\keVc
\let\evc=\eVc
\def\TeVcc{\ifmmode {\mathrm{\ Te\kern -0.1em V}/c^2}\else
{\textrm{Te\kern -0.1em V}/$c^2$}\fi}%
\def\GeVcc{\ifmmode {\mathrm{\ Ge\kern -0.1em V}/c^2}\else
{\textrm{Ge\kern -0.1em V}/$c^2$}\fi}%
\def\MeVcc{\ifmmode {\mathrm{\ Me\kern -0.1em V}/c^2}\else
{\textrm{Me\kern -0.1em V}/$c^2$}\fi}%
\def\keVcc{\ifmmode {\mathrm{\ ke\kern -0.1em V}/c^2}\else
{\textrm{ke\kern -0.1em V}/$c^2$}\fi}%
\def\eVcc{\ifmmode {\mathrm{\ e\kern -0.1em V}/c^2}\else
{\textrm{e\kern -0.1em V}/$c^2$}\fi}%
\let\tevcc=\TeVcc
\let\gevcc=\GeVcc
\let\mevcc=\MeVcc
\let\kevcc=\keVcc
\let\evcc=\eVcc
\def\cm{\ifmmode {\mathrm{\ cm}}\else
\textrm{~cm}\fi}%
%
\def\ifb{\mbox{fb$^{-1}$}}% Inverse femtobarns.
\def\ipb{\mbox{pb$^{-1}$}}% Inverse picobarns.
\def\inb{\mbox{nb$^{-1}$}}% Inverse nanobarns.
%
\def\mass#1{\ensuremath{m_{#1#1}}}% "\mass{\mu}" produces "msub{mumu}".
\def\twomass#1#2{\ensuremath{m_{#1#2}}}%
%
\def\Ecm{\ensuremath{E_{\mathrm{cm}}}} % Subscript roman not italic (EE)
%
% +--------------------------------------------------------------------+
% | |
% | "Box-squared" operator, as in Klein-Gordon. Command is "\boxsq". |
% | |
% +--------------------------------------------------------------------+
%
\newbox\boxsqbox
\newdimen\boxsize\boxsize=1.2ex%
\def\boxop{%
\setbox\boxsqbox=\vbox{\hrule depth0.8pt width0.8\boxsize height0pt%
\kern0.8\boxsize
\hrule height0.8pt width0.8\boxsize depth0pt}%
\hbox{%
\vrule height1.0\boxsize width0.8pt depth0pt%
\copy\boxsqbox
\vrule height1.0\boxsize width0.8pt depth0pt\kern1.5pt}}%
\def\boxsq{\ensuremath{\boxop^2}}%
% +--------------------------------------------------------------------+
% | |
% | Theoretical notations |
% | |
% +--------------------------------------------------------------------+
%
\def\spinor#1{\ensuremath{\left(\matrix{#1_1\cr#1_2\cr#1_3\cr#1_4\cr}\right)}} % Math mode (EE)
\def\pmb#1{\setbox0=\hbox{$#1$}% This is "poor man's boldface".
\kern-.025em\copy0\kern-1.0\wd0%
\kern.05em\copy0\kern-1.0\wd0%
\kern-.025em\raise.0433em\box0}%
\def\grad{\pmb{\nabla}}%
%
% +--------------------------------------------------------------------+
% | |
% | The decay symbol, to be used in \eqalign. |
% | It works like: \[\eqalign{a\ra &b+c\cr &\dk &e+f\cr &&\dk g+h}\] |
% | |
% | a --> b + c |
% | | |
% | | |
% | +----> e + f |
% | | |
% | | |
% | +----> g + h |
% | |
% +--------------------------------------------------------------------+
%
\newdimen\dkwidth
\def\dk{%
\dkwidth=\baselineskip
{\def\to{\rightarrow}% allows "\rightarrowfill" to work.
\kern 3pt%
\hbox{%
\raise 3pt%
\hbox{%
\vrule height 0.8\dkwidth width 0.7pt depth0pt%
}%
\kern-0.4pt%
\hbox to 1.5\dkwidth{%
\rightarrowfill
}%
\kern0.6em%
}}%
}%
%
% +--------------------------------------------------------------------+
% | |
% | Redefine \eqalign to allow more than one column; very |
% | useful for multiple decays as defined above. |
% | |
% +--------------------------------------------------------------------+
%
%\unlock
\def\eqalign#1{%
\,
\vcenter{%
\openup\jot\m@th
\ialign{%
\strut\hfil$\displaystyle{##}$&&$%
\displaystyle{{}##}$\hfil\crcr#1\crcr%
}%
}%
\,
}%
%\lock
%
% +--------------------------------------------------------------------+
% | |
% | JOURNALS (for MISC definitions, see also ../biblio/ATLASstyle.bst)|
% | |
% +--------------------------------------------------------------------+
%
\newcommand {\AcPA} {Acta Phys. Austriaca{} }
\newcommand {\ARevNS} {Ann.{} Rev.{} Nucl.{} Sci.{} }
\newcommand {\CPC} {Comp.{} Phys.{} Comm.{} }
\newcommand {\FortP} {Fortschr.{} Phys.{} }
\newcommand {\IJMP} {Int.{} J.{} Mod.{} Phys.{} }
\newcommand {\JETP} {Sov.{} Phys.{} JETP{} }
\newcommand {\JETPL} {JETP Lett.{} }
\newcommand {\JaFi} {Jad.{} Fiz.{} }
\newcommand {\JMP} {J.{} Math.{} Phys.{} }
\newcommand {\MPL} {Mod.{} Phys.{} Lett.{} }
\newcommand {\NCim} {Nuovo Cimento{} }
\newcommand {\NIM} {Nucl.{} Instrum.{} Meth.{} }
\newcommand {\NP} {Nucl.{} Phys.{} }
\newcommand {\PL} {Phys.{} Lett.{} }
\newcommand {\PR} {Phys.{} Rev.{} }
\newcommand {\PRL} {Phys.{} Rev.{} Lett.{} }
\newcommand {\PRep} {Phys.{} Rep.{} }
\newcommand {\RMP} {Rev.{} Mod.{} Phys.{} }
\newcommand {\ZfP} {Z.{} Phys.{} }
\newcommand {\EPJ} {Eur.{} Phys.{} J.{} }
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%
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