\ProvidesPackage{abhep}[2005/01/17] \RequirePackage{amsmath} \RequirePackage{cancel} \RequirePackage{abhepexpt} \RequirePackage{hepnicenames} \RequirePackage{hepunits} \RequirePackage{maybemath} \RequirePackage{abmath} %C++ macro (to be moved!) \DeclareRobustCommand{\CC}{C\nolinebreak\hspace{-.05em}\raisebox{.4ex}{\tiny\bf +}\nolinebreak\hspace{-.10em}\raisebox{.4ex}{\tiny\bf +}} \def\CCtwo{{C\nolinebreak[4]\hspace{-.05em}\raisebox{.4ex}{\tiny\bf ++}}} \DeclareRobustCommand{\Rplus}{\protect\nolinebreak\hspace{-.07em}\protect\raisebox{.25ex}{\small\textbf{+}}} \DeclareRobustCommand{\Cpp}{C\Rplus\Rplus\xspace} \DeclareRobustCommand{\rescatter}{re-scatter\xspace} \DeclareRobustCommand{\electroweak}{electro-weak\xspace} \DeclareRobustCommand{\StandardModel}{Standard Model\xspace} \DeclareRobustCommand{\SM}{Standard Model\xspace} % General lagrangian formalism \DeclareRobustCommand{\matrixelementM}{\mymath{ \mathcal{M} }\xspace} \DeclareRobustCommand{\matrixelementA}{\mymath{ \mathcal{A} }\xspace} \DeclareRobustCommand{\Amplitude}[1]{\mymath{ \mathcal{A}% \begingroup% \def\@empty{}% \def\@arg{#1}% \ifx\@arg\@empty{}\else\parenths{#1}\fi% \endgroup% }} % also want Rate and BranchingRatio \DeclareRobustCommand{\Lagrangian}{\mymath{ \mathcal{L} }\xspace} \DeclareRobustCommand{\Hamiltonian}{\mymath{ \mathcal{H} }\xspace} \DeclareRobustCommand{\lagrangian}{\Lagrangian} \DeclareRobustCommand{\hamiltonian}{\Hamiltonian} \DeclareRobustCommand{\RenormalisationScale}{\mymath{ \mu }\xspace} \DeclareRobustCommand{\adjointField}[1]{\mymath{ \bar{#1} }\xspace} \DeclareRobustCommand{\scalarField}{\mymath{ \phi }\xspace} \DeclareRobustCommand{\spinorField}{\mymath{ \psi }\xspace} \DeclareRobustCommand{\pathD}{\mymath{ \mathcal{D} }\xspace} \DeclareRobustCommand{\VEV}{VEV\xspace} \DeclareRobustCommand{\QCD}{QCD\xspace} \DeclareRobustCommand{\EW}{EW\xspace} \DeclareRobustCommand{\EM}{EM\xspace} \DeclareRobustCommand{\PDG}{PDG\xspace} % covariant derivative % covariant vectors, tensors, vectors % Common Feynman rules %% photon propagator %% external vector boson %% Z,W propagator \DeclareRobustCommand{\pseudorapidity}{pseudo-rapidity\xspace} % Rates and measurements \DeclareRobustCommand{\BR}[1]{\mymath{% \def\empty{}% \def\thearg{#1}% \mathcal{B}% \ifx\thearg\empty{}\else{(\HepProcess{#1})}\fi% }\xspace} \DeclareRobustCommand{\efficiency}[1]{\mymath{ \def\empty{}% \def\thearg{#1}% \varepsilon% \ifx\thearg\empty{}\else{(\text{#1})}\fi% }\xspace} \DeclareRobustCommand{\purity}{\mymath{p}\xspace} \DeclareRobustCommand{\luminosity}{\mymath{\mathcal{L}}\xspace} \DeclareRobustCommand{\sqrtS}{\mymath{\sqrt{s}}\xspace} %% CP violation %% \DeclareRobustCommand{\opC}{\mymath{\maybebm{\mathcal{C}}}\xspace} %% \DeclareRobustCommand{\opP}{\mymath{\maybebm{\mathcal{P}}}\xspace} %% \DeclareRobustCommand{\opT}{\mymath{\maybebm{\mathcal{T}}}\xspace} \DeclareRobustCommand{\opC}{\texorpdfstring{\mymath{\maybebm{\mathcal{C}}}}{C}\xspace} \DeclareRobustCommand{\opP}{\texorpdfstring{\mymath{\maybebm{\mathcal{P}}}}{P}\xspace} \DeclareRobustCommand{\opT}{\texorpdfstring{\mymath{\maybebm{\mathcal{T}}}}{T}\xspace} \DeclareRobustCommand{\opCP}{\mymath{\opC\opP}\xspace} \DeclareRobustCommand{\opCPT}{\mymath{\opC\opP\opT}\xspace} %% and for convenience... \DeclareRobustCommand{\CP}{\opCP} \DeclareRobustCommand{\CPT}{\opCPT} %% symmetry violation shorthands \DeclareRobustCommand{\CPv}{\mymath{\cancel{\opCP}}\xspace} \DeclareRobustCommand{\CPViolation}{\mymath{\opCP\text{-violation}}\xspace} \DeclareRobustCommand{\CPTv}{\mymath{\cancel{\opCPT}}\xspace} \DeclareRobustCommand{\CPTViolation}{\mymath{\opCPT\text{-violation}}\xspace} %% Important names (of effects, params, theories etc.) and suchlike \DeclareRobustCommand{\Cabibbo}{\ensuremath{\text{Cabibbo}}\xspace} \DeclareRobustCommand{\Maskawa}{\ensuremath{\text{Maskawa}}\xspace} \DeclareRobustCommand{\Kobayashi}{\ensuremath{\text{Kobayashi}}\xspace} \DeclareRobustCommand{\Jarlskog}{\ensuremath{\text{Jarlskog}}\xspace} \DeclareRobustCommand{\Sakharov}{\ensuremath{\text{Sakharov}}\xspace} \DeclareRobustCommand{\Majorana}{\ensuremath{\text{Majorana}}\xspace} \DeclareRobustCommand{\Planck}{\ensuremath{\text{Planck}}\xspace} \DeclareRobustCommand{\Dirac}{\ensuremath{\text{Dirac}}\xspace} \DeclareRobustCommand{\Weyl}{\ensuremath{\text{Weyl}}\xspace} %% Theories \DeclareRobustCommand{\SUSY}{\ensuremath{\text{SUSY}}\xspace} \DeclareRobustCommand{\AMSB}{\ensuremath{\text{AMSB}}\xspace} \DeclareRobustCommand{\mSUGRA}{\ensuremath{\text{mSUGRA}}\xspace} \DeclareRobustCommand{\JarlskogParam}{\mymath{J_{\CP}}\xspace} \DeclareRobustCommand{\thetaCabibbo}{\mymath{\maybebm{\theta_c}}} %% CKM matrix stuff \DeclareRobustCommand{\Vckm}{\mymath{ \boldmatrix{V}_{\!\mathrm{CKM}} }\xspace} \DeclareRobustCommand{\VckmFull}{\mymath{% \begin{pmatrix} \Vud & \Vus & \Vub \\ \Vcd & \Vcs & \Vcb \\ \Vtd & \Vts & \Vtb \\ \end{pmatrix} }} \DeclareRobustCommand{\alphaCKM}{\mymath{\alpha}\xspace} \DeclareRobustCommand{\betaCKM}{\mymath{\beta}\xspace} \DeclareRobustCommand{\gammaCKM}{\mymath{\gamma}\xspace} \DeclareRobustCommand{\CkmElementConj}[2]{\mymath{V_{{#1}{#2}}^{*}}\xspace} \DeclareRobustCommand{\CkmElement}[2]{\mymath{V_{{#1}{#2}}^{\phantom{*}}}\xspace} \DeclareRobustCommand{\Vud}{\CkmElement{\mathrm{u}}{\mathrm{d}}} \DeclareRobustCommand{\Vus}{\CkmElement{\mathrm{u}}{\mathrm{s}}} \DeclareRobustCommand{\Vub}{\CkmElement{\mathrm{u}}{\mathrm{b}}} \DeclareRobustCommand{\Vcd}{\CkmElement{\mathrm{c}}{\mathrm{d}}} \DeclareRobustCommand{\Vcs}{\CkmElement{\mathrm{c}}{\mathrm{s}}} \DeclareRobustCommand{\Vcb}{\CkmElement{\mathrm{c}}{\mathrm{b}}} \DeclareRobustCommand{\Vtd}{\CkmElement{\mathrm{t}}{\mathrm{d}}} \DeclareRobustCommand{\Vts}{\CkmElement{\mathrm{t}}{\mathrm{s}}} \DeclareRobustCommand{\Vtb}{\CkmElement{\mathrm{t}}{\mathrm{b}}} \DeclareRobustCommand{\VudConj}{\CkmElementConj{\mathrm{u}}{\mathrm{d}}} \DeclareRobustCommand{\VusConj}{\CkmElementConj{\mathrm{u}}{\mathrm{s}}} \DeclareRobustCommand{\VubConj}{\CkmElementConj{\mathrm{u}}{\mathrm{b}}} \DeclareRobustCommand{\VcdConj}{\CkmElementConj{\mathrm{c}}{\mathrm{d}}} \DeclareRobustCommand{\VcsConj}{\CkmElementConj{\mathrm{c}}{\mathrm{s}}} \DeclareRobustCommand{\VcbConj}{\CkmElementConj{\mathrm{c}}{\mathrm{b}}} \DeclareRobustCommand{\VtdConj}{\CkmElementConj{\mathrm{t}}{\mathrm{d}}} \DeclareRobustCommand{\VtsConj}{\CkmElementConj{\mathrm{t}}{\mathrm{s}}} \DeclareRobustCommand{\VtbConj}{\CkmElementConj{\mathrm{t}}{\mathrm{b}}} %% CKM element pairing for unitarity relations \newlength{\CKMPairWidth} \settowidth{\CKMPairWidth}{\Vtd\VtbConj} \DeclareRobustCommand{\@Vbox}[1]{\makebox[\CKMPairWidth]{#1}} \DeclareRobustCommand{\VCkmPair}[2]{\ensuremath{\@Vbox{{#1}{#2}}}} %% Theory acronyms \DeclareRobustCommand{\SCET}{SCET\xspace} \DeclareRobustCommand{\HQET}{HQET\xspace} \DeclareRobustCommand{\CKM}{CKM\xspace} \DeclareRobustCommand{\KM}{KM\xspace} \DeclareRobustCommand{\BSM}{BSM\xspace} \DeclareRobustCommand{\FCNC}{FCNC\xspace} %% Typical analysis concepts \DeclareRobustCommand{\PV}{\MathUpright{PV}} \DeclareRobustCommand{\IP}{\MathUpright{IP}} \DeclareRobustCommand{\pT}{\mymath{p_\MathUpright{T}}\xspace} \DeclareRobustCommand{\missingpT}{\mymath{\cancel{\pT}}\xspace} \DeclareRobustCommand{\Et}{\mymath{E_\MathUpright{T}}\xspace} \DeclareRobustCommand{\missingEt}{\mymath{\cancel{\Et}}\xspace} \DeclareRobustCommand{\p}{\mymath{p}\xspace} \DeclareRobustCommand{\chisq}{\mymath{\chi^2}\xspace} \DeclareRobustCommand{\tuple}[1]{\ensuremath{#1}-tuple\xspace} \DeclareRobustCommand{\tuples}[1]{\ensuremath{#1}-tuples\xspace} \DeclareRobustCommand{\ntuple}{\tuple{n}\xspace} \DeclareRobustCommand{\ntuples}{\tuples{n}\xspace} \DeclareRobustCommand{\dataset}{data set\xspace} \DeclareRobustCommand{\cutset}{cut set\xspace} \DeclareRobustCommand{\CoM}{CoM\xspace}