% % 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. % % Version 2.4 - 6/11/08 % Modifications from version 2.2 by Eric Eisenhandler % All changes commented with initials (EE) % % Change from version 2.3 to 2.4 is to eliminate all \xspace after definitions. % If a space is needed after the symbol, then use \ followed by a space. (EE) % %\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} % % +--------------------------------------------------------------------+ % | | % | 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\mumu}} \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}}}% % % +--------------------------------------------------------------------+ % | | % | 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\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\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.{} Inst.{} 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.{} } %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%