% Macros for the General Meeting talk of Nov 9, 1998. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % % % The generic thesis macro include file % % % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \typeout{Thesis macros `../higgs_input'. .} \NeedsTeXFormat{LaTeX2e} \ProvidesPackage{../higgs_input}[11/9/98 Macros for your thesis, dude.] % % +--------------------------------------------------------------------+ % | | % | 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} % +--------------------------------------------------------------------+ % | | % | Particle-antiparticle pair notations. | % | | % +--------------------------------------------------------------------+ % \def\antibar#1{\ensuremath{#1\bar{#1}}}% \def\bbar{\ensuremath{\bar{\mathrm{b}}}} \def\bbbar{\antibar{\mathrm{b}}\yspace}% \def\cbar{\ensuremath{\bar{\mathrm{c}}}} \def\ccbar{\antibar{\mathrm{c}}\yspace}% \def\sbar{\ensuremath{\bar{\mathrm{s}}}} \def\ssbar{\antibar{\mathrm{s}}\yspace}% \def\ubar{\ensuremath{\bar{\mathrm{u}}}} \def\uubar{\antibar{\mathrm{u}}\yspace}% \def\dbar{\ensuremath{\bar{\mathrm{d}}}} \def\ddbar{\antibar{\mathrm{d}}\yspace}% \def\f{\ensuremath{\mathrm{f}}\yspace} \def\fbar{\ensuremath{\bar{\mathrm{f}}}\yspace} \def\ffbar{\antibar{\mathrm{f}}\yspace}% \def\qbar{\ensuremath{\bar{\mathrm{q}}}} \def\qqbar{\antibar{\mathrm{q}}\yspace}% \def\nbar{\ensuremath{\bar{\nu}}} \def\nnbar{\antibar{\nu}\yspace}% % % +--------------------------------------------------------------------+ % | | % | Here are e+, e-, e+e-, etc. | % | | % +--------------------------------------------------------------------+ % \def\e{\ensuremath{\mathrm{e}}}% \def\epm{\ensuremath{\mathrm{e^{\pm}}}\yspace}% \def\epem{\ensuremath{\mathrm{e^+e^-}}\yspace}% \def\mumu{\ensuremath{\mathrm{\mu^+ \mu^-}}\yspace}% \def\tautau{\ensuremath{\mathrm{\tau^+ \tau^-}}\yspace}% \def\ll{\ensuremath{\ell^+ \ell^-}\yspace}% \def\nunubar{\ensuremath{\nu\bar{\nu}}\yspace}% % % +--------------------------------------------------------------------+ % | | % | Particles and whatnot. | % | | % +--------------------------------------------------------------------+ % \newcommand{\Z}{\ensuremath{\mathrm{Z}}\yspace} \newcommand{\W}{\ensuremath{\mathrm{W}}\yspace} \newcommand{\ZZ}{\ensuremath{\mathrm{ZZ}}\yspace} \newcommand{\Wpm}{\ensuremath{\mathrm{W^{\pm}}}\yspace} \newcommand{\WW}{\ensuremath{\mathrm{W}^+\mathrm{W}^-}\yspace} \newcommand{\pion}{\ensuremath{\pi}\yspace} \newcommand{\quark}{\ensuremath{\mathrm{q}}\yspace} \newcommand{\antiquark}{\ensuremath{\mathrm{\bar{q}}}\yspace} \newcommand{\bquark}{\ensuremath{\mathrm{b}}\yspace} \newcommand{\uquark}{\ensuremath{\mathrm{u}}\yspace} \newcommand{\dquark}{\ensuremath{\mathrm{d}}\yspace} \newcommand{\cquark}{\ensuremath{\mathrm{c}}\yspace} \newcommand{\squark}{\ensuremath{\mathrm{s}}\yspace} \newcommand{\tquark}{\ensuremath{\mathrm{t}}\yspace} \newcommand{\bantiquark}{\ensuremath{\mathrm{\bar{b}}}\yspace} \newcommand{\kaon}{\ensuremath{\mathrm{K}}\yspace} \newcommand{\kshort}{\ensuremath{\mathrm{K}^0_S}\yspace} \newcommand{\klong}{\ensuremath{\mathrm{K}^0_L}\yspace} \newcommand{\lambdazero}{\ensuremath{\Lambda^0}\yspace} \newcommand{\Bzero}{\ensuremath{\mathrm{B}^0}\yspace} \newcommand{\Bpm}{\ensuremath{\mathrm{B}^{\pm}}\yspace} \newcommand{\Bzeros}{\ensuremath{\mathrm{B}^0_{\squark}}\yspace} \newcommand{\Dzero}{\ensuremath{\mathrm{D}^0}\yspace} \newcommand{\Dpm}{\ensuremath{\mathrm{D}^{\pm}}\yspace} \newcommand{\Dpms}{\ensuremath{\mathrm{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{\mathrm{H^{+}H^{-}}}\yspace} \newcommand{\Hpm}{\ensuremath{\mathrm{H^{\pm}}}\yspace} \newcommand{\h}{\ensuremath{\mathrm{h}}\yspace} \newcommand{\A}{\ensuremath{\mathrm{A}}\yspace} \newcommand{\bigH}{\ensuremath{\mathrm{H}}\yspace} \newcommand{\hZ}{\ensuremath{\mathrm{hZ}}\yspace} \newcommand{\hA}{\ensuremath{\mathrm{hA}}\yspace} \newcommand{\SMHZ}{\ensuremath{\mathrm{HZ}}\yspace} \newcommand{\hboson}{\ensuremath{\mathrm{h^{0}}}\yspace} \newcommand{\Hboson}{\ensuremath{\mathrm{H^{0}}}\yspace} \newcommand{\Aboson}{\ensuremath{\mathrm{A^{0}}}\yspace} % % +--------------------------------------------------------------------+ % | | % | Particles masses | % | | % +--------------------------------------------------------------------+ % \newcommand{\mtau}{\ensuremath{m_\tau}\yspace} \newcommand{\mt}{\ensuremath{m_\mathrm{t}}\yspace} \newcommand{\mZ}{\ensuremath{m_\mathrm{Z}}\yspace} \newcommand{\mW}{\ensuremath{m_\mathrm{W}}\yspace} \newcommand{\mHplusminus}{\ensuremath{m_\mathrm{H^\pm}}\yspace} \newcommand{\mh}{\ensuremath{m_\mathrm{h}}\yspace} \newcommand{\mH}{\ensuremath{m_\mathrm{H}}\yspace} \newcommand{\mA}{\ensuremath{m_\mathrm{A}}\yspace} \newcommand{\mX}{\ensuremath{m_\mathrm{X}}\yspace} % % +--------------------------------------------------------------------+ % | | % | LEP and Z decays | % | | % +--------------------------------------------------------------------+ % \newcommand{\epemtoZ}{\ensuremath{\epem\!\rightarrow\!\Z}\yspace} \newcommand{\epemtoZg}{\ensuremath{\epem\!\rightarrow\!\Z(\gamma)}\yspace} \newcommand{\Zto}{\ensuremath{\Z\!\rightarrow\!}} \newcommand{\Zgto}{\ensuremath{\Z^{*}/\gamma^{*}\!\rightarrow\!}} \newcommand{\Zsto}{\ensuremath{\Z^{*}\!\rightarrow\!}} \newcommand{\Ztoll}{\ensuremath{\Zto \, \ell^+\ell^-}\yspace} \newcommand{\Ztonunu}{\ensuremath{\Zto\nunubar }\yspace} \newcommand{\Ztoee}{\ensuremath{\Zto e^+e^-}\yspace} \newcommand{\Ztomm}{\ensuremath{\Zto \mu^+\mu^-}\yspace} \newcommand{\Ztott}{\ensuremath{\Zto \tau^+\tau^-}\yspace} \newcommand{\Ztottg}{\ensuremath{\Zto \tau^+\tau^-(\gamma)}\yspace} \newcommand{\Ztoqq}{\ensuremath{\Zto \mathrm{ q\bar{q}}}\yspace} \newcommand{\Ztobb}{\ensuremath{\Zto \mathrm{ b\bar{b}}}\yspace} \newcommand{\Zgtoqq}{\ensuremath{\Zgto \mathrm{ q\bar{q}}}\yspace} \newcommand{\Ztoqqqq}{\ensuremath{\Zto \mathrm{q\bar{q}q\bar{q}}}\yspace} \newcommand{\Ztoqqgg}{\ensuremath{\Zto \mathrm{q\bar{q}gg}}\yspace} \newcommand{\ZtoHplusminus}{\ensuremath{\Zto \Hplusminus}\yspace} \newcommand{\epemtoZgtohA}{\ensuremath{\epem\!\rightarrow\!\Zgto \hA}\yspace} \newcommand{\epemtoZgtohZ}{\ensuremath{\epem\!\rightarrow\!\Zgto \hZ}\yspace} \newcommand{\epemtoZgtoSMHZ}{\ensuremath{\epem\!\rightarrow\!\Zgto \SMHZ}\yspace} \newcommand{\epemtoZgtoqq}{\ensuremath{\epem\!\rightarrow\!\Zgto \mathrm{ q\bar{q}}}\yspace} \newcommand{\epemtohA}{\ensuremath{\epem\!\rightarrow\!\Zsto \hA}\yspace} \newcommand{\epemtohZ}{\ensuremath{\epem\!\rightarrow\!\Zsto \hZ}\yspace} \newcommand{\epemtoSMHZ}{\ensuremath{\epem\!\rightarrow\!\Zsto \SMHZ}\yspace} \newcommand{\epemtoqq}{\ensuremath{\epem\!\rightarrow\!\qqbar}\yspace} \newcommand{\epemtoqqg}{\ensuremath{\epem\!\rightarrow\!\qqbar(\gamma)}\yspace} \newcommand{\epemtoWW}{\ensuremath{\epem\!\rightarrow\!\mathrm{W^+W^-}}\yspace} \newcommand{\epemtoZZ}{\ensuremath{\epem\!\rightarrow\!\mathrm{\Z\Z}}\yspace} \newcommand{\epemtoeeqq}{\ensuremath{\epem\!\rightarrow\!\epem\qqbar}\yspace} \newcommand{\epemtoffff}{\ensuremath{\epem\!\rightarrow\!\mathrm{f\bar{f}'}\mathrm{f''\bar{f}'''}}\yspace} \newcommand{\epemtoZee}{\ensuremath{\epem\!\rightarrow\!\Z\epem}\yspace} \newcommand{\epemtotautau}{\ensuremath{\epem\!\rightarrow\!\tautau}\yspace} \newcommand{\bhabha}{\ensuremath{\epemtoZ\!\rightarrow\!\epem}\yspace} \newcommand{\dimuon}{\ensuremath{\epemtoZ\!\rightarrow\!\mumu}\yspace} \newcommand{\ditau}{\epemtotautau} % % +--------------------------------------------------------------------+ % | | % | 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 \mathrm{ b\bar{b}}}\yspace} \newcommand{\Htobb}{\ensuremath{\Hto \mathrm{ b\bar{b}}}\yspace} \newcommand{\htocc}{\ensuremath{\hto \mathrm{ c\bar{c}}}\yspace} \newcommand{\Htocc}{\ensuremath{\Hto \mathrm{ c\bar{c}}}\yspace} \newcommand{\htogg}{\ensuremath{\hto \mathrm{gg}}\yspace} \newcommand{\Htogg}{\ensuremath{\Hto \mathrm{gg}}\yspace} \newcommand{\htott}{\ensuremath{\hto \tautau}\yspace} \newcommand{\Htott}{\ensuremath{\Hto \tautau}\yspace} \newcommand{\Atobb}{\ensuremath{\Ato \mathrm{ b\bar{b}}}\yspace} \newcommand{\Atott}{\ensuremath{\Ato \tautau}\yspace} \newcommand{\HplustoLep}{\ensuremath{\mathrm{H^{+}}\!\!\!\rightarrow\! \tau^+\nutau}\yspace} \newcommand{\HplustoHad}{\ensuremath{\mathrm{H^{+}}\!\!\!\rightarrow\! \mathrm{c\bar{s}}}\yspace} \newcommand{\ZtoHplusminusHad}{\ensuremath{\Zto\Hplusminus\!\!\! \rightarrow\!\mathrm{c\bar{s}\bar{c}s}}\yspace} \newcommand{\ZtoHplusminusSemi}{\ensuremath{\Zto\Hplusminus\!\!\! \rightarrow\!\tau^+\nutau\mathrm{ \bar{c}s} \, (\mathrm{\bar{c}s}\tau^-\nubartau)}\yspace} \newcommand{\ZtoHplusminusLep}{\ensuremath{\Zto \Hplusminus\!\!\! \rightarrow\!\tau^+\nutau\tau^-\nubartau}\yspace} \newcommand{\hAtobbbb}{\ensuremath{\mathrm{\hA\!\rightarrow\! b\bar{b}b\bar{b}}}\yspace} \newcommand{\hAtobbbbToo}{\ensuremath{\mathrm{\hA\rightarrow b\bar{b}b\bar{b}}}\yspace} \newcommand{\hAtobbtt}{\ensuremath{\mathrm{\hA\!\rightarrow\! b\bar{b}\tau^+\tau^-}}\yspace} \newcommand{\hAtottbb}{\ensuremath{\mathrm{\hA\!\rightarrow\! \tau^+\tau^-b\bar{b}}}\yspace} \newcommand{\hZtobbqq}{\ensuremath{\mathrm{\hZ\!\rightarrow\! b\bar{b}q\bar{q}}}\yspace} \newcommand{\hZtoAAff}{\ensuremath{\mathrm{\hZ\!\rightarrow\! AAf\bar{f}}}\yspace} \newcommand{\hZtobbqqToo}{\ensuremath{\mathrm{\hZ\rightarrow b\bar{b}q\bar{q}}}\yspace} \newcommand{\hZtoqqqq}{\ensuremath{\mathrm{\hZ\!\rightarrow\! q\bar{q}q\bar{q}}}\yspace} \newcommand{\hZtoccqq}{\ensuremath{\mathrm{\hZ\!\rightarrow\! c\bar{c}q\bar{q}}}\yspace} \newcommand{\hZtoggqq}{\ensuremath{\mathrm{\hZ\!\rightarrow\! ggq\bar{q}}}\yspace} \newcommand{\hZtobbnn}{\ensuremath{\mathrm{\hZ\!\rightarrow\! b\bar{b}\nu\bar{\nu}}}\yspace} \newcommand{\hZtobbll}{\ensuremath{\mathrm{\hZ\!\rightarrow\! b\bar{b}\ell^+\ell^-}}\yspace} \newcommand{\hZtobbee}{\ensuremath{\mathrm{\hZ\!\rightarrow\! b\bar{b}\e^+\e^-}}\yspace} \newcommand{\hZtobbmm}{\ensuremath{\mathrm{\hZ\!\rightarrow\! b\bar{b}\mu^+\mu^-}}\yspace} \newcommand{\hZtoqqll}{\ensuremath{\mathrm{\hZ\!\rightarrow\! q\bar{q}\ell^+\ell^-}}\yspace} \newcommand{\hZtobbtt}{\ensuremath{\mathrm{\hZ\!\rightarrow\! b\bar{b}\tau^+\tau^-}}\yspace} \newcommand{\hZtottbb}{\ensuremath{\mathrm{\hZ\!\rightarrow\! \tau^+\tau^-b\bar{b}}}\yspace} \newcommand{\hZtottqq}{\ensuremath{\mathrm{\hZ\!\rightarrow\! \tau^+\tau^-q\bar{q}}}\yspace} \newcommand{\hZtoqqtt}{\ensuremath{\mathrm{\hZ\!\rightarrow\! q\bar{q}\tau^+\tau^-}}\yspace} \newcommand{\htoAA}{\ensuremath{\hto\A\A}\yspace} % Standard Model specific stuff just like the MSSM little h \newcommand{\SMHZtobbqq}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! b\bar{b}q\bar{q}}}\yspace} \newcommand{\SMHZtobbqqToo}{\ensuremath{\mathrm{\SMHZ\rightarrow b\bar{b}q\bar{q}}}\yspace} \newcommand{\SMHZtoqqqq}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! q\bar{q}q\bar{q}}}\yspace} \newcommand{\SMHZtoccqq}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! c\bar{c}q\bar{q}}}\yspace} \newcommand{\SMHZtoggqq}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! ggq\bar{q}}}\yspace} \newcommand{\SMHZtobbnn}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! b\bar{b}\nu\bar{\nu}}}\yspace} \newcommand{\SMHZtobbll}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! b\bar{b}\ell^+\ell^-}}\yspace} \newcommand{\SMHZtobbee}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! b\bar{b}\epem}}\yspace} \newcommand{\SMHZtobbmm}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! b\bar{b}\mumu}}\yspace} \newcommand{\SMHZtoqqll}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! q\bar{q}\ell^+\ell^-}}\yspace} \newcommand{\SMHZtobbtt}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! b\bar{b}\tau^+\tau^-}}\yspace} \newcommand{\SMHZtottbb}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! \tau^+\tau^-b\bar{b}}}\yspace} \newcommand{\SMHZtottqq}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! \tau^+\tau^-q\bar{q}}}\yspace} \newcommand{\SMHZtoqqtt}{\ensuremath{\mathrm{\SMHZ\!\rightarrow\! q\bar{q}\tau^+\tau^-}}\yspace} % % +--------------------------------------------------------------------+ % | | % | Tag and tracking related stuff | % | | % +--------------------------------------------------------------------+ % \newcommand{\DCArf}{\ensuremath{\delta_{r\phi}}\yspace} \newcommand{\DCAsz}{\ensuremath{\delta_{sz}}\yspace} \newcommand{\phiin}{\ensuremath{\phi_{\mathrm{inner}}}\yspace} \newcommand{\phiout}{\ensuremath{\phi_{\mathrm{outer}}}\yspace} \newcommand{\zout}{\ensuremath{z_{\mathrm{outer}}}\yspace} \newcommand{\zin}{\ensuremath{z_{\mathrm{inner}}}\yspace} \newcommand{\efflad}{\ensuremath{\varepsilon_l}\yspace} % So-called SMD efficiency \newcommand{\effsvx}{\ensuremath{\varepsilon_s}\yspace} % So-called SMD efficiency \newcommand{\Lrf}{\ensuremath{{\mathrm{L}}_{r\phi}}\yspace} \newcommand{\Lsz}{\ensuremath{{\mathrm{L}}_{sz}}\yspace} \newcommand{\Ltot}{\ensuremath{{\mathrm{L}}}\yspace} \newcommand{\Btag}{\ensuremath{B_{\mathrm{tag}}}\yspace} % Generic b-tag \newcommand{\Bwt}{\ensuremath{B^{\mathrm{w}}_n}\yspace} % Weighted event tag \newcommand{\Bjet}{\ensuremath{B^{\mathrm{w}}_{\mathrm{jet}}}\yspace} % Weighted b-tag \newcommand{\Bevtag}{\ensuremath{B_{\mathrm{tag}}^{\mathrm{event}}}\yspace} % Event tag. % % +--------------------------------------------------------------------+ % | | % | Higgs analysis variables and their friends | % | | % +--------------------------------------------------------------------+ % \newcommand{\chim}{\ensuremath{\chi}\yspace} \newcommand{\chimZ}{\ensuremath{\chi_{\mathrm{hZ}}}\yspace} \newcommand{\chimSM}{\ensuremath{\chi_{\mathrm{HZ}}}\yspace} \newcommand{\chimA}{\ensuremath{\chi_{\mathrm{hA}}}\yspace} \newcommand{\chimW}{\ensuremath{\chi_{\mathrm{WW}}}\yspace} \newcommand{\tanb}{\ensuremath{\tan\!\beta}\yspace} \newcommand{\tanbma}{\ensuremath{(\tan\beta,\mA)}\yspace} \newcommand{\Evis}{\ensuremath{E_{\mathrm{vis}}}\yspace} \newcommand{\Mvis}{\ensuremath{M_{\mathrm{vis}}}\yspace} \newcommand{\Epar}{\ensuremath{P_{\parallel}^{\mathrm{miss}}}\yspace} \newcommand{\Eperp}{\ensuremath{P_{\perp}^{\mathrm{miss}}}\yspace} \newcommand{\Ytf}{\ensuremath{Y_{34}^{\mathrm{D}}}\yspace} \newcommand{\Mi}{\ensuremath{M_i}\yspace} \newcommand{\Meq}{\ensuremath{M_\mathrm{eq}^\mathrm{5C}}\yspace} \newcommand{\MfiveC}{\ensuremath{M_\mathrm{H}^\mathrm{5C}}\yspace} \newcommand{\Emin}{\ensuremath{\min(E_{\mathrm{jet}})}\yspace} \newcommand{\DEmax}{\ensuremath{\max(\Delta E_{\mathrm{jet}})}\yspace} % Names of the different 4-jet hA and hZ analyses \newcommand{\HA}{\ensuremath{\mathrm{hA}_{\bbbar\bbbar}}\yspace} \newcommand{\HZ}{\ensuremath{\mathrm{hZ}_{\bbbar\qqbar}}\yspace} \newcommand{\AZHA}{\ensuremath{\mathrm{hA}_{\bbbar\bbbar}'}\yspace} \newcommand{\AZHZ}{\ensuremath{\mathrm{hZ}_{\bbbar\qqbar}'}\yspace} % Final variables \newcommand{\FhA}{\ensuremath{F(\mA,\mh)}\yspace} \newcommand{\FhZ}{\ensuremath{F(\MZ,\mh)}\yspace} % % +--------------------------------------------------------------------+ % | | % | Confidence levels and optimized functions used in analyses | % | | % +--------------------------------------------------------------------+ % \newcommand{\CL}{\ensuremath{C\kern -0.1em L}\yspace} \newcommand{\CLopt}{\ensuremath{\widehat{\CL}}\yspace} \newcommand{\CLb}{\ensuremath{\CL_b}\yspace} \newcommand{\CLbayes}{\ensuremath{\widetilde{\CL}}\yspace} \newcommand{\CLavg}{\ensuremath{< \kern -0.4em \CL \kern -0.4em >}\yspace} \newcommand{\CLmed}{\ensuremath{\overline{\CL}}\yspace} \newcommand{\mhavg}{\ensuremath{< \kern -0.4em \mh \kern -0.4em >}\yspace} \newcommand{\mAavg}{\ensuremath{< \kern -0.4em \mA \kern -0.4em >}\yspace} \newcommand{\mhmed}{\ensuremath{\overline{m}_{\mathrm{h}}}\yspace} \newcommand{\mAmed}{\ensuremath{\overline{m}_{\mathrm{A}}}\yspace} % % +--------------------------------------------------------------------+ % | | % | Random shite. | % | | % +--------------------------------------------------------------------+ % \newcommand{\rts}{\ensuremath{\sqrt{s}}\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{\mrad}{\ensuremath{\mathrm{\ mrad}}\yspace} \newcommand{\rad}{\ensuremath{\mathrm{\ rad}}\yspace} \newcommand{\etal}{\textit{et~al.}}% For author lists in bibliography. % % +--------------------------------------------------------------------+ % | | % | Field Theory Crapola | % | | % +--------------------------------------------------------------------+ % \newcommand{\SUthreeC}{\ensuremath{\mathrm{SU(3)_{color}}}\yspace} \newcommand{\SUtwoL}{\ensuremath{\mathrm{SU(2)}_L}\yspace} \newcommand{\SUtwo}{\ensuremath{\mathrm{SU(2)}}\yspace} \newcommand{\UoneY}{\ensuremath{\mathrm{U(1)}_Y}\yspace} \newcommand{\UoneEM}{\ensuremath{\mathrm{U(1)}_{\mathrm{EM}}}\yspace} \newcommand{\Dweak}{\ensuremath{D_{\mu}^{\SUtwoL\otimes\UoneY}}\yspace} \newcommand{\DY}{\ensuremath{D_{\mu}^{\UoneY}}\yspace} \newcommand{\Dcolor}{\ensuremath{D_{\mu}^{\SUthreeC}}\yspace} \newcommand{\Dsm}{\ensuremath{D_{\mu}}\yspace} % % +--------------------------------------------------------------------+ % | | % | InsertPlot - The plot insertion macro | % | | % +--------------------------------------------------------------------+ % % #1 is the filename % #2 x coord. of lower left corner of plot in pts % #3 y coord. of lower left corner of plot in pts % #4 x coord. of upper right corner of plot in pts % #5 y coord. of upper right corner of plot in pts % \newcount\dx \newcount\dy \def\dim_in_pt#1{#1 true pt} \def\psneg#1{#1 neg} \def\InsertPlot#1#2#3#4#5{ \message { Inserting plot file in figures/#1.ps} \dx=#4 \advance\dx by -#2 \dy=#5 \advance\dy by -#3 \centerline{ \hbox to \dim_in_pt{\number\dx}{\hfil \vbox to \dim_in_pt{\number\dy}{\vfil \special{ps::[asis,begin] 0 SPB /InsertPlot save def Xpos Ypos translate \psneg{\number\dx} 0 translate \psneg{#2} \psneg{#3} translate } \special{ps: plotfile #1.ps asis} \special{ps::[asis,end] InsertPlot restore 0 SPE } } } } } % % +--------------------------------------------------------------------+ % | | % | FakePlot - Just makes the border of InsertPlot above for | % | previewing purposes | % | | % +--------------------------------------------------------------------+ % \def\FakePlot#1#2#3#4#5{ \message { Faking plot file in figures/#1.ps} \dx=#4 \advance\dx by -#2 \dy=#5 \advance\dy by -#3 \centerline{\fbox{ \hbox to \dim_in_pt{\number\dx}{\hfil \vbox to \dim_in_pt{\number\dy}{\vfil}}}} } % % +--------------------------------------------------------------------+ % | | % | Fake2 - just the captions - for drafts | % | | % +--------------------------------------------------------------------+ % \def\Fake2#1#2#3#4#5{ \message { Fake2ing plot file in figures/#1.ps} \vskip 10pt } % % +--------------------------------------------------------------------+ % | | % | Cuts and Trig environments to display things in a standard box | % | | % +--------------------------------------------------------------------+ % \newcounter{cutn} \newcounter{cndn} \def\OrdinaryBorder#1{\vbox{\hrule\hbox{\vrule\kern10pt \vbox{\kern3pt#1\kern3pt}\kern10pt\vrule}\hrule}} \def\CutBoxBorder#1{\hspace{0.22222in} \vbox{\hrule\hbox{\vrule\kern10pt \vbox{\kern3pt#1\kern3pt}\kern10pt\vrule}\hrule}} \newenvironment{Cuts}{\begin{list}{\bf Cut \arabic{cutn}}{\usecounter{cutn}\setlength{\labelwidth}{0.5in} \setlength{\labelsep}{0.2in}\setlength{\leftmargin}{0.7in}\setlength{\rightmargin}{1.0in}}}{\end{list}} \newenvironment{Trig}{\begin{list}{\bf Condition \arabic{cndn}}{\usecounter{cndn}\setlength{\labelwidth}{1.0in} \setlength{\labelsep}{0.2in}\setlength{\leftmargin}{1.2in}\setlength{\rightmargin}{1.0in}}}{\end{list}} % % +--------------------------------------------------------------------+ % | | % | Fraction with slanted division line | % | | % +--------------------------------------------------------------------+ % \def\slfrac#1#2{\kern.1em \raise.5ex\hbox{\the\scriptfont0 #1}\kern-.1em /\kern-.15em\lower.25ex\hbox{\the\scriptfont0 #2} } % These were here from jregan era. \renewcommand{\topfraction}{0.8} \renewcommand{\bottomfraction}{0.8} \renewcommand{\textfraction}{0.2} %%% Local Variables: %%% mode: latex %%% TeX-master: "higgs" %%% End: