凌宮数学の数式プラグイン## eq ##で使用可能な$$ \text{\TeX} $$コマンド
###
### tex
\newcommand{\disp}[1]{{\displaystyle {#1}}}
%% Width Alignment
\newcommand{\spc}[2]{{\ooalign{{\hss{$#1$}\hss}\crcr{\phantom{\hss{$#2$}\hss}}}}}
\newcommand{\clap}[2]{{\ooalign{{\hss{$#1$}\hss}\crcr{\hss{$#2$}\hss}}}}
%% Bector
\renewcommand{\b}[1]{{\bm {#1}}}
\def\:#1{{\b#1}}
\def\bi{{\bm i}}
\newcommand{\sx}{ \mathbin{\bm \cdot}} % Dot Product
\newcommand{\Sx}{ \mathbin{\spc{\bm \cdot}{\times}}} % Dot Product (Alignment as cross product)
\newcommand{\vx}{ \mathbin \times } % Cross Product
\newcommand{\wx}{ \mathbin \wedge } % Widge Product
\newcommand{\tx}{ \mathbin \otimes } % Tensor Product
\newcommand{\wxv}{\mathbin{\clap{\wx}{{}_{{}_v}}}} % Widge Product of Macro vector
\newcommand{\wxb}{\mathbin{\clap{\wx}{{}_{{}_b}}}} % Base Product
\newcommand{\grad }{\mathrm{grad}}
\newcommand{\rot }{\mathrm{rot}}
\newcommand{\diver}{\mathrm{div}}
%%\newcommand{\yaku}{\approx}
\newcommand{\perct}{\%}
\newcommand{\pr}{\partial}
\newcommand{\dl}{\delta}
\newcommand{\Dl}{\varDelta}
\newcommand{\ff} [2]{\frac{\,{#1}\,}{\,{#2}\,}}
\newcommand{\dd} [2]{\frac{\,d{#1}\,}{\,d{#2}\,}}
\newcommand{\pp} [2]{\frac{\,\pr{#1}\,}{\,\pr{#2}\,}}
\newcommand{\ffd}[2]{\disp{\ff{\disp{#1}\mathstrut}{\disp{#2}\mathstrut}}}
\newcommand{\ddd}[2]{\disp{\dd{\disp{#1}\mathstrut}{\disp{#2}\mathstrut}}}
\newcommand{\ppd}[2]{\disp{\pp{\disp{#1}\mathstrut}{\disp{#2}\mathstrut}}}
\newcommand{\rt}[2][{\;\;}]{\sqrt[#1]{#2\,}}
\newcommand{\Inte}[2][]{\!\int_{#1}^{#2}}
\newcommand{\inte}[1][\,\,]{\!\int_{#1\!}}
\newcommand{\nte}[1][\,\,]{\!\!\int_{#1\!}}
\newcommand{\hindent}{\hspace{2em}}
\newcommand{\bs}[1]{{\scriptstyle(#1)}}
\newcommand{\fracstrut}{\vphantom{\frac{\mathstrut}{\mathstrut}}}
\newcommand{\ffdstrut}{\vphantom{\ffd{\mathstrut}{\mathstrut}}}
\renewcommand{\arraystretch}{1}
\newcommand{\arr}[2][c]{{}\!\begin{array}{#1}#2\end{array}\!{}}
\newcommand{\arrc}[2][c]{{}\!\left(\arr[#1]{#2}\right)\!{}}
\newcommand{\arrs}[2][c]{{}\!\left[\arr[#1]{#2}\right]\!{}}
\newcommand{\arrw}[2][c]{{}\!\left\{\arr[#1]{#2}\right\}\!{}}
\newcommand{\arrb}[2][c|c]{\!\left[{}\!\arr[#1]{#2}\right]\!\!{}}
\newcommand{\iro}[2][ak]{{\color{#1}#2}}
\newcommand{\clr}[2][red]{{\color{#1}#2}}
%%Itaric Greek Alphabet
\newcommand{\omicron }{o}
\newcommand{\varAlpha }{A}
\newcommand{\varBega }{B}
\newcommand{\varEpsilon}{E}
\newcommand{\varZeta }{Z}
\newcommand{\varEta }{H}
\newcommand{\varIota }{I}
\newcommand{\varKapper }{K}
\newcommand{\varMu }{M}
\newcommand{\varNu }{N}
\newcommand{\varOmicron}{O}
\newcommand{\varRho }{P}
\newcommand{\varTau }{T}
\newcommand{\varChi }{X}
%%Itaric Greek Alphabet 3char
\newcommand{\gal}{\alpha }
\newcommand{\gbt}{\beta }
\newcommand{\ggm}{\gamma }
\newcommand{\gdl}{\delta }
\newcommand{\gep}{\varepsilon}
\newcommand{\gzt}{\zeta }
\newcommand{\get}{\eta }
\newcommand{\gth}{\theta }
\newcommand{\gio}{\iota }
\newcommand{\gkp}{\kappa }
\newcommand{\glm}{\lambda }
\newcommand{\gmu}{\mu }
\newcommand{\gnu}{\nu }
\newcommand{\gxi}{\xi }
\newcommand{\gom}{ o }
\newcommand{\gpi}{\pi }
\newcommand{\grh}{\rho }
\newcommand{\gsg}{\sigma }
\newcommand{\gta}{\tau }
\newcommand{\gup}{\upsilon }
\newcommand{\gph}{\varphi }
\newcommand{\gch}{\chi }
\newcommand{\gps}{\psi }
\newcommand{\goM}{\omega }
\newcommand{\gks}{\xi }
\newcommand{\gAl}{ A }
\newcommand{\gBt}{ B }
\newcommand{\gGm}{\varGamma }
\newcommand{\gDl}{\varDelta }
\newcommand{\gEp}{ E }
\newcommand{\gZt}{ Z }
\newcommand{\gEt}{ H }
\newcommand{\gTh}{\varTheta }
\newcommand{\gIo}{ I }
\newcommand{\gKp}{ K }
\newcommand{\gLm}{\varLambda }
\newcommand{\gMu}{ M }
\newcommand{\gNu}{ N }
\newcommand{\gXi}{\varXi }
\newcommand{\gOm}{ O }
\newcommand{\gPi}{\varPi }
\newcommand{\gRh}{ P }
\newcommand{\gSg}{\varSigma }
\newcommand{\gTa}{ T }
\newcommand{\gUp}{\varUpsilon}
\newcommand{\gPh}{\varPhi }
\newcommand{\gCh}{ X }
\newcommand{\gPs}{\varPsi }
\newcommand{\gOM}{\varOmega }
\newcommand{\gKs}{\varXi }
%% alimented function
\newcommand{\wsin}{\spc{\sin}{\cos}}
\newcommand{\wcos}{\spc{\cos}{\cos}}
\newcommand{\wtan}{\spc{\tan}{\cos}}
%% colored function
\newcommand{\csin}{\spc{{\color{ak}\sin}}{\cos}}
\newcommand{\ccos}{\spc{{\color{ao}\cos}}{\cos}}
\newcommand{\ctan}{\spc{{\color{md}\tan}}{\cos}}
\newcommand{\ci}{\clr[ak]{\bm i}} % i
%% undetermind operator
%\newcommand{\ccossin}{\clr[mr]{\subarray{c} \displaystyle \cos \\ \displaystyle \sin \endsubarray}}
\newcommand{\tri}{\textrm{tri}}
\newcommand{\ctri}{\clr[mr]{\tri}}
\newcommand{\cpm}{\clr[mr]{\pm}}
\newcommand{\cmp}{\clr[mr]{\mp}}
%% unit %% cf http://www.kuee.kyoto-u.ac.jp/~eel/qty/node7.html
\def\u#1{{%
\def\O{\textrm{O}}%
\def\u{\textrm{u}}%
\mathcode`\u=\mu
\mathcode`\O=\Omega
\rm #1}}
%%http://www.biwako.shiga-u.ac.jp/sensei/kumazawa/tex/web0028.html
\newcommand{\overparenthesis}[2][3pt]%
{\mathop{\,\vbox{%
\baselineskip0ex\lineskip#1\ialign{##%
\crcr{\downparenthfill}%
\crcr{$\!\displaystyle{#2}\!$}%
\crcr%
}%
}\,}\limits}%
\newcommand{\underparenthesis}[2][3.5pt]%
{\mathop{\,\vtop{%
\baselineskip0ex\lineskip#1\ialign{##%
\crcr{$\!\displaystyle{#2}\!$}%
\crcr{\upparenthfill}%
\crcr%
}%
}\,}\limits}%
\newcommand{\overbracket}[2][3pt]%
{\mathop{\,\vbox{%
\baselineskip0ex\lineskip#1\ialign{##%
\crcr{\downbracketfill}%
\crcr{$\!\displaystyle{#2}\!$}%
\crcr%
}%
}\,}\limits}%
\newcommand{\underbracket}[2][3.5pt]%
{\mathop{\,\vtop{%
\baselineskip0ex\lineskip#1\ialign{##%
\crcr{$\!\displaystyle{#2}\!$}%
\crcr{\upbracketfill}%
\crcr%
}%
}\,}\limits}%
\def\downparenthfill{$\m@th\braceld\leaders\vrule\hfill\bracerd$}
\def\upparenthfill{$\m@th\bracelu\leaders\vrule\hfill\braceru$}
\def\upbracketfill{$\m@th\makesm@sh{\llap{\vrule\@height3\p@\@width.7\p@}}%
\leaders\vrule\@height.7\p@\hfill
\makesm@sh{\rlap{\vrule\@height3\p@\@width.7\p@}}$}
\def\downbracketfill{$\m@th
\makesm@sh{\llap{\vrule\@height.7\p@\@depth2.3\p@\@width.7\p@}}%
\leaders\vrule\@height.7\p@\hfill
\makesm@sh{\rlap{\vrule\@height.7\p@\@depth2.3\p@\@width.7\p@}}$}
###