%% %% This is file `physymb.sty', %% generated with the docstrip utility. %% %% The original source files were: %% %% physymb.dtx (with options: `package') %% This is a generated file. %% Copyright (C) 2005-2011 by David Zaslavsky %% This file may be distributed and/or modified under the %% conditions of the LaTeX Project Public License, either %% version 1.3 of this license or (at your option) any later %% version. The latest version of this license is in: %% http://www.latex-project.org/lppl.txt %% and version 1.3 or later is part of all distributions of %% LaTeX version 2005/12/01 or later. \NeedsTeXFormat{LaTeX2e}[1999/12/01] \ProvidesPackage{physymb}[2011/05/09 v0.2 Physics symbol definitions] %% \CharacterTable %% {Upper-case \A\B\C\D\E\F\G\H\I\J\K\L\M\N\O\P\Q\R\S\T\U\V\W\X\Y\Z %% Lower-case \a\b\c\d\e\f\g\h\i\j\k\l\m\n\o\p\q\r\s\t\u\v\w\x\y\z %% Digits \0\1\2\3\4\5\6\7\8\9 %% Exclamation \! Double quote \" Hash (number) \# %% Dollar \$ Percent \% Ampersand \& %% Acute accent \' Left paren \( Right paren \) %% Asterisk \* Plus \+ Comma \, %% Minus \- Point \. Solidus \/ %% Colon \: Semicolon \; Less than \< %% Equals \= Greater than \> Question mark \? %% Commercial at \@ Left bracket \[ Backslash \\ %% Right bracket \] Circumflex \^ Underscore \_ %% Grave accent \` Left brace \{ Vertical bar \| %% Right brace \} Tilde \~} \RequirePackage{ifthen} \newboolean{pparticle} \newboolean{pfeynman} \newboolean{pbraket} \newboolean{punits} \newboolean{pboldvectors} \DeclareOption{braket}{\setboolean{pbraket}{true}} \DeclareOption{particle}{\setboolean{pparticle}{true}} \DeclareOption{units}{\setboolean{punits}{true}} \DeclareOption{feynman}{\setboolean{pfeynman}{true}} \DeclareOption{arrowvectors}{\setboolean{pboldvectors}{false}} \DeclareOption{boldvectors}{\setboolean{pboldvectors}{true}} \ProcessOptions\relax \RequirePackage{amsbsy} \RequirePackage{amsmath} \RequirePackage{amsfonts} \RequirePackage{amssymb} \allowdisplaybreaks[2] \RequirePackage{accents} \RequirePackage{calligra} \DeclareMathAlphabet{\mathcalligra}{T1}{calligra}{m}{n} \DeclareFontShape{T1}{calligra}{m}{n}{<->s*[2.2]callig15}{} \newcommand{\scriptr}{\mathcalligra{r}} \ifthenelse{\boolean{pbraket}} { \RequirePackage{braket} } {} \ifthenelse{\boolean{punits}} { \RequirePackage{siunitx} \DeclareSIUnit{\torr}{torr} \DeclareSIUnit{\mmhg}{mmHg} \DeclareSIUnit{\amu}{amu} \DeclareSIUnit{\yr}{yr} \DeclareSIUnit{\erg}{erg} \DeclareSIUnit{\gauss}{Ga} \DeclareSIUnit{\molar}{\textsc{M}} % this follows the style set up in the siunitx manual \DeclareSIUnit{\poise}{P} \DeclareSIUnit{\foot}{ft} \DeclareSIUnit{\mileperhour}{mph} \DeclareSIUnit{\pound}{lb} \DeclareSIUnit{\poundforce}{lbf} } {} \newcommand{\orderof}[1]{\ensuremath{\mathcal{O}\left(#1\right)}} \DeclareMathOperator{\asin}{\sin^{-1}} \DeclareMathOperator{\acos}{\cos^{-1}} \DeclareMathOperator{\atan}{\tan^{-1}} \DeclareMathOperator{\asec}{\sec^{-1}} \DeclareMathOperator{\acsc}{\csc^{-1}} \DeclareMathOperator{\acot}{\cot^{-1}} \DeclareMathOperator{\sech}{sech} \DeclareMathOperator{\csch}{csch} \DeclareMathOperator{\asinh}{\sinh^{-1}} \DeclareMathOperator{\acosh}{\cosh^{-1}} \DeclareMathOperator{\atanh}{\tanh^{-1}} \DeclareMathOperator{\asech}{\sech^{-1}} \DeclareMathOperator{\acsch}{\csch^{-1}} \DeclareMathOperator{\acoth}{\coth^{-1}} \DeclareMathOperator{\diag}{diag} \DeclareMathOperator{\realop}{Re} \DeclareMathOperator{\imagop}{Im} \newcommand{\real}[1]{\realop\{#1\}} \newcommand{\imag}[1]{\imagop\{#1\}} \DeclareMathOperator{\sgn}{sgn} \newcommand{\abs}[1]{\left\lvert#1\right\rvert} \newcommand{\norm}[1]{\left\lVert#1\right\rVert} \newcommand{\evalat}[3]{\left.#1\right|_{#2}^{#3}} \newcommand{\pbrac}[2]{\left\{#1,#2\right\}} \newcommand{\pbracvars}[4]{\left\{#1,#2\right\}_{#3,#4}} \ifthenelse{\boolean{pboldvectors}}% {\renewcommand{\vec}[1]{\mathbf{#1}}}% {\renewcommand{\vec}[1]{\accentset{\rightharpoonup}{#1}}} \newcommand{\vecvar}[1]{\vec{#1}} \newcommand{\tnsvar}[1]{\mathbf{#1}} \newcommand{\matvar}[1]{\mathbf{#1}} \newcommand{\identitym}{\mathbf{1}} \newcommand{\determinant}[1]{\left\lvert#1\right\rvert} \DeclareMathOperator{\trace}{Tr} \newcommand{\unitd}{\hat{d}} \newcommand{\unite}{\hat{e}} \newcommand{\uniti}{\hat{\imath}} \newcommand{\unitj}{\hat{\jmath}} \newcommand{\unitk}{\hat{k}} \newcommand{\unitl}{\hat{\ell}} \newcommand{\unitn}{\hat{n}} \newcommand{\unitp}{\hat{p}} \newcommand{\unitq}{\hat{q}} \newcommand{\unitr}{\hat{r}} \newcommand{\units}{\hat{s}} \newcommand{\unitt}{\hat{t}} \newcommand{\unitu}{\hat{u}} \newcommand{\unitv}{\hat{v}} \newcommand{\unitw}{\hat{w}} \newcommand{\unitx}{\hat{x}} \newcommand{\unity}{\hat{y}} \newcommand{\unitz}{\hat{z}} \newcommand{\unitphi}{\hat{\phi}} \newcommand{\unitrho}{\hat{\rho}} \newcommand{\unittheta}{\hat{\theta}} \newcommand{\unitomega}{\hat{\omega}} \newcommand{\unitvec}[1]{\hat{#1}} \newcommand{\udc}{\mathrm{d}} \newcommand{\uddc}{\mathrm{d}^2} \newcommand{\udddc}{\mathrm{d}^3} \newcommand{\pdc}{\partial} \newcommand{\pddc}{\partial^2} \newcommand{\pdddc}{\partial^3} \newcommand{\uds}{\,\mathrm{d}} \newcommand{\udds}{\,\mathrm{d}^2} \newcommand{\uddds}{\,\mathrm{d}^3} \newcommand{\pds}{\,\partial} \newcommand{\pdds}{\,\partial^2} \newcommand{\pddds}{\,\partial^3} \newcommand{\ud}[2]{\frac{\mathrm{d}#1}{\mathrm{d}#2}} \newcommand{\udd}[2]{\frac{\mathrm{d}^2#1}{\mathrm{d} #2^2}} \newcommand{\uddd}[2]{\frac{\mathrm{d}^3#1}{\mathrm{d} #2^3}} \newcommand{\pd}[2]{\frac{\partial #1}{\partial #2}} \newcommand{\pdd}[2]{\frac{\partial^2#1}{\partial #2^2}} \newcommand{\pddd}[2]{\frac{\partial^3#1}{\partial #2^3}} \newcommand{\grad}{\accentset{\rightharpoonup}{\nabla}} \renewcommand{\div}{\grad\cdot} \newcommand{\curl}{\grad\times} \newcommand{\lapl}{\nabla^2} \newcommand{\conj}[1]{{#1 ^{*}}} \newcommand{\herm}[1]{{#1 ^{\dagger}}} \newcommand{\transpose}[1]{{#1 ^{T}}} \newcommand{\natset}{\mathbb{N}} \newcommand{\intset}{\mathbb{Z}} \newcommand{\cpxset}{\mathbb{C}} \newcommand{\whlset}{\mathbb{Q}} \newcommand{\realset}{\mathbb{R}} \newcommand{\imagset}{\mathbb{I}} \newcommand{\commut}[2]{\left[ #1, #2 \right]} \newcommand{\acommut}[2]{\left\{ #1, #2 \right\}} \DeclareMathOperator{\round}{round} \DeclareMathOperator{\exd}{\mathbf{d}} \newcommand{\hodge}{\star} \ifthenelse{\boolean{pparticle}} { \newcommand{\upq}{\ensuremath{\mathrm{u}}{}} \newcommand{\dnq}{\ensuremath{\mathrm{d}}{}} \newcommand{\srq}{\ensuremath{\mathrm{s}}{}} \newcommand{\chq}{\ensuremath{\mathrm{c}}{}} \newcommand{\btq}{\ensuremath{\mathrm{b}}{}} \newcommand{\tpq}{\ensuremath{\mathrm{t}}{}} \newcommand{\upaq}{\ensuremath{\bar{\mathrm{u}}}{}} \newcommand{\dnaq}{\ensuremath{\bar{\mathrm{d}}}{}} \newcommand{\sraq}{\ensuremath{\bar{\mathrm{s}}}{}} \newcommand{\chaq}{\ensuremath{\bar{\mathrm{c}}}{}} \newcommand{\btaq}{\ensuremath{\bar{\mathrm{b}}}{}} \newcommand{\tpaq}{\ensuremath{\bar{\mathrm{t}}}{}} \newcommand{\elp}{\ensuremath{\mathrm{e}^-}{}} \newcommand{\enu}{\ensuremath{\nu_\mathrm{e}}{}} \newcommand{\ulp}{\ensuremath{\mu^-}{}} \newcommand{\unu}{\ensuremath{\nu_{\mu}}{}} \newcommand{\tlp}{\ensuremath{\tau^-}{}} \newcommand{\tnu}{\ensuremath{\nu_{\tau}}{}} \newcommand{\ealp}{\ensuremath{\mathrm{e}^+}{}} \newcommand{\eanu}{\ensuremath{\bar{\nu}_\mathrm{e}}{}} \newcommand{\ualp}{\ensuremath{\mu^+}{}} \newcommand{\uanu}{\ensuremath{\bar{\nu}_{\mu}}{}} \newcommand{\talp}{\ensuremath{\tau^+}{}} \newcommand{\tanu}{\ensuremath{\bar{\nu}_{\tau}}{}} \newcommand{\prbr}{\ensuremath{\mathrm{p}^+}{}} \newcommand{\nebr}{\ensuremath{\mathrm{n}^0}{}} \newcommand{\lmzbr}{\ensuremath{\Lambda^0}{}} \newcommand{\sgpbr}{\ensuremath{\Sigma^+}{}} \newcommand{\sgzbr}{\ensuremath{\Sigma^0}{}} \newcommand{\sgmbr}{\ensuremath{\Sigma^-}{}} \newcommand{\dlppbr}{\ensuremath{\Delta^{++}}{}} \newcommand{\dlpbr}{\ensuremath{\Delta^+}{}} \newcommand{\dlzbr}{\ensuremath{\Delta^0}{}} \newcommand{\dlmbr}{\ensuremath{\Delta^-}{}} \newcommand{\xizbr}{\ensuremath{\Xi^0}{}} \newcommand{\ximbr}{\ensuremath{\Xi^-}{}} \newcommand{\ommbr}{\ensuremath{\Omega^-}{}} \newcommand{\sgspbr}{\ensuremath{\Sigma^{*+}}{}} \newcommand{\sgszbr}{\ensuremath{\Sigma^{*0}}{}} \newcommand{\sgsmbr}{\ensuremath{\Sigma^{*-}}{}} \newcommand{\xiszbr}{\ensuremath{\Xi^{*0}}{}} \newcommand{\xismbr}{\ensuremath{\Xi^{*-}}{}} \newcommand{\prabr}{\ensuremath{\mathrm{p}^-}{}} \newcommand{\neabr}{\ensuremath{\bar{\mathrm{n}}^0}{}} \newcommand{\dlpabr}{\ensuremath{\bar{\Delta}^{+}}{}} \newcommand{\dlzabr}{\ensuremath{\bar{\Delta}^{0}}{}} \newcommand{\dlmabr}{\ensuremath{\bar{\Delta}^{-}}{}} \newcommand{\dlmmabr}{\ensuremath{\bar{\Delta}^{--}}{}} \newcommand{\pipm}{\ensuremath{\pi^+}{}} \newcommand{\pizm}{\ensuremath{\pi^0}{}} \newcommand{\pimm}{\ensuremath{\pi^-}{}} \newcommand{\kapm}{\ensuremath{K^+}{}} \newcommand{\kazm}{\ensuremath{K^0}{}} \newcommand{\kazam}{\ensuremath{\bar{K}^0}{}} \newcommand{\kamm}{\ensuremath{K^-}{}} \newcommand{\ropm}{\ensuremath{\rho^+}{}} \newcommand{\rozm}{\ensuremath{\rho^0}{}} \newcommand{\romm}{\ensuremath{\rho^-}{}} \newcommand{\etam}{\ensuremath{\eta}{}} \newcommand{\etapm}{\ensuremath{\eta'}{}} \newcommand{\kaspm}{\ensuremath{\mathrm{K}^{*+}}{}} \newcommand{\kaszm}{\ensuremath{\mathrm{K}^{*0}}{}} \newcommand{\kaszam}{\ensuremath{\bar{\mathrm{K}}^{*0}}{}} \newcommand{\kasmm}{\ensuremath{\mathrm{K}^{*-}}{}} \newcommand{\omm}{\ensuremath{\omega}{}} \newcommand{\phim}{\ensuremath{\phi}{}} \newcommand{\phbsn}{\ensuremath{\gamma}{}} \newcommand{\Wbsn}{\ensuremath{\mathrm{W}}{}} \newcommand{\Wpbsn}{\ensuremath{\mathrm{W}^{+}}{}} \newcommand{\Wmbsn}{\ensuremath{\mathrm{W}^{-}}{}} \newcommand{\Zzbsn}{\ensuremath{\mathrm{Z}^{0}}{}} \newcommand{\hbsn}{\ensuremath{\mathrm{h}}{}} \newcommand{\photon}{\phbsn} } {} \ifthenelse{\boolean{pfeynman}}% {\RequirePackage{feynmp}}% {} \endinput %% %% End of file `physymb.sty'.