\documentclass[times,10pt,twocolumn]{article}
\usepackage{latexsym}
% Style definitions that can be overridden in a user
% input file
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\newcommand{\stylelegendtitle}[1]{{\bf #1:}}
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\newcommand{\styletitle}[2]{#1\ifEq{#2}{}\else:\\ {\Large #2}\fi}
\newcommand{\styletopictitle}[1]{{\bf #1}}
\input{docsize}
\usepackage{amssymb}
\usepackage{dsfont}
\frenchspacing
\begin{document}
This document tests the use of mathml math to produce latex.
$\hat{x}$
$\bar{x}$
$\underline{x}$
$\vec{x}$
$\dot{x}$
$\ddot{x}$
$\uparrow$
$\downarrow$
$\to$
$\to$
$\mapsto$
$\leftarrow$
$\leftrightarrow$
$\Rightarrow$
$\Leftarrow$
$\Leftrightarrow$
$a$
$12$
$- 4$
$12 - 4$
$\mbox{a}$
$\mbox{ }$
$\frac{d}{d x} f ( x ) = \lim_{h \to 0} \frac{f ( x + h ) - f ( x )}{h}$
$\frac{d}{d x} f ( x ) = \lim_{h \to 0} \frac{f ( x + h ) - f ( x )}{h}$
$\int_0^1 f ( x ) d x$
$\int_0^{\frac{\pi}{2}} \sin x \, d x = 1$
$\sum_{i = 1}^n i^3 = \left( \frac{n ( n + 1 )}{2} \right)^2$
$\int_{- 1}^1 \sqrt{1 - x^2} d x = \frac{\pi}{2}$
$x^2 + \frac{b}{a} x + \frac{c}{a} = 0$
$x^2 + \frac{b}{a} x + \left( \frac{b}{2 a} \right)^2 - \left( \frac{b}{2 a} \right)^2 + \frac{c}{a} = 0$
$\left( x + \frac{b}{2 a} \right)^2 = \frac{b^2}{4 a^2} - \frac{c}{a}$
$x + \frac{b}{2 a} = \pm \sqrt{\frac{b^2}{4 a^2} - \frac{c}{a}}$
$\frac{b}{2 a}$
$x_{1 , 2} = \frac{- b \pm \sqrt{b^2 - 4 a c}}{2 a}$
$f ( x ) = \sum_{n = 0}^{\infty} \frac{f^{( n )} ( a )}{n !} ( x - a )^n$
$\frac{\frac{a}{b}}{\frac{c}{d}}$
$\frac{a}{b} / \frac{c}{d}$
$\frac{( a \cdot b )}{c}$
$\sum_{i = 1}^n i = \frac{n ( n + 1 )}{2}$
$\frac{x + 1}{y}$
$\,\, | A | = \left| \begin{array}{ll}
a & b \\
c & d \\
\end{array}
\right| = a d - b c \,\,$
$| A | = \left| \begin{array}{ll}
a & b \\
c & d \\
\end{array}
\right| = a d - b c \,\,$
$\bf{A}$
$A$
$A$
$\tt{A}$
$A$
$\sf{A}$
$\bf{A B 3} . A B . A B . A B . \tt{A B} . \sf{A B}$
$\sin$
$\cos$
$\tan$
$\csc$
$\sec$
$\cot$
$\sinh$
$\cosh$
$\tanh$
$\log$
$\ln$
$\det$
$\dim$
$\lim$
$\bmod$
$\gcd ( m , n ) = a \bmod b$
$x \equiv y \pmod{a + b}$
$\gcd$
$\mbox{lcm}$
$\min$
$\max$
$\alpha$
$\beta$
$\chi$
$\delta$
$\Delta$
$\epsilon$
$\varepsilon$
$\eta$
$\gamma$
$\Gamma$
$\iota$
$\kappa$
$\lambda$
$\Lambda$
$\mu$
$\nu$
$\omega$
$\Omega$
$\phi$
$\varphi$
$\Phi$
$\pi$
$\Pi$
$\psi$
$\Psi$
$\rho$
$\sigma$
$\Sigma$
$\tau$
$\theta$
$\vartheta$
$\Theta$
$\upsilon$
$\xi$
$\Xi$
$\zeta$
$($
$)$
$[$
$]$
$\{$
$\}$
$\langle$
$\rangle$
$ $
$:\}$
$ $
$- a$
$E = m c^2$
$e^{i \pi} = - 1$
$a ! \leq b ! \geq c$
$a \ne 0$
$a x^2 + b x + c = 0$
$x^2 + y_1 + z_{12}^{34}$
$a / b$
$\sqrt{\sqrt{\sqrt[3]{x}}}$
$a b c - 123.45^{- 1.1}$
$\stackrel{\mbox{def}}{=}$
$\stackrel{\Delta}{=} \mbox{ } ( \mbox{or } := )$
$\mbox{}_{\, 92}^{238} U$
$a_{m n}$
$a_{m n}$
$\sqrt{x}$
$x^2$
$S '$
$\sinh x = \frac{e^x - e^{- x}}{2}$
$f ( x ) = \sum_{n = 0}^{\infty} \frac{f^{( n )} ( a )}{n !} ( x - a )^n$
$\frac{d}{d x} \, f ( x )$
$\mbox{ and }$
$\mbox{ or }$
$\neg$
$\Rightarrow$
$\mbox{if }$
$\Leftrightarrow$
$\forall$
$\exists$
$\bot$
$\top$
$\vdash$
$\models$
$\left( \begin{array}{cc}
a & b \\
c & d \\
\end{array}
\right)^{- 1} = \frac{1}{a d - b c} \left( \begin{array}{cc}
d & - b \\
- c & a \\
\end{array}
\right)$
$\left[ \begin{array}{cc}
a & b \\
c & d \\
\end{array}
\right] \left( \begin{array}{c}
n \\
k \\
\end{array}
\right)$
$\frac{x}{x} = \left\{ \begin{array}{ll}
1 & \mbox{if } x \ne 0 \\
\mbox{undefined} & \mbox{if } x = 0 \\
\end{array}
\right.$
$\langle a , b \rangle \mbox{ and } \begin{array}{ll}
x & y \\
u & v \\
\end{array}
$
$\left\{ \begin{array}{ccc}
S_{11} & \ldots & S_{1 n} \\
\vdots & \ddots & \vdots \\
S_{m 1} & \ldots & S_{m n} \\
\end{array}
\right]$
$a \not\le b$
$a \not\le b$
$\frac{d}{d x} f ( x ) = f ' ( x )$
newcommand ``FUNKY'' ``''
$\mbox{newcommand} \mbox{NAME} b a d$
$+$
$-$
$\cdot$
$\star$
$/$
$a \backslash b$
$\times$
$\div$
$\circ$
$\oplus$
$\otimes$
$\odot$
$\sum$
$\prod$
$\wedge$
$\bigwedge$
$\vee$
$\bigvee$
$\cap$
$\bigcap$
$\cup$
$\bigcup$
$=$
$\ne$
$<$
$>$
$\leq$
$\geq$
$\prec$
$\succ$
$\in$
$\notin$
$\subset$
$\supset$
$\subseteq$
$\supseteq$
$\equiv$
$\cong$
$\approx$
$\propto$
$y = x^2$
$y = \frac{1}{x}$
$y = \sqrt{x}$
$E = m c^{3 + e^{i \pi}}$
$a^2 + b^2 = c^2$
$\forall x \in \mathds{C} \left( \sin^2 x + \cos^2 x = 1 \right)$
$\left( \forall x : x \in \mathds{C} : \sin^2 x + \cos^2 x = 1 \right)$
$\sum_{i = 1}^n i^3 = \left( \sum_{i = 1}^n i^2 \right)^2$
$( a , b )$
$f$
$\Delta x = \frac{b - a}{n}$
$\int_a^b f ( x ) d x = \lim_{n \to \infty} \sum_{i = 1}^n f \left( x_i^{\star} \right) \Delta x$
$x_i = a + i \Delta x$
$x_i^{\star} \in \left[ x_{i - 1} , x_i \right]$
$\int_0^{\infty} e^{- x^2} d x = \frac{1}{2} \sqrt{\pi} .$
$\frac{x}{x} = ( 1 \mbox{if } x \ne 0 )$
$\int_0^{\pi} \sin x d x = - \cos x ]_0^{\pi} = - \cos \pi - ( - \cos 0 ) = - ( - 1 ) - ( - 1 ) = 2$
$- 0.123 .456$
$\epsilon = .001 \,\, h = - .01 \,\, \pi \approx 3.14159 \,\,$
$u . v$
$\mathds{R} = \bigcup_{n = 0}^{\infty} [ - n , n ]$
$\{ 0 \} = \bigcap_{n = 1}^{\infty} \left( - \frac{1}{n} , \frac{1}{n} \right)$
$\bigwedge_{i = 1}^n \phi_i = \phi_1 \wedge \phi_2 \wedge \cdots \wedge \phi_n$
$\bigvee_{i = 1}^n \phi_i = \phi_1 \vee \phi_2 \vee \cdots \vee \phi_n$
$\pi \approx 3.141592653589793$
$\int_{- 1}^1 \sqrt{1 - x^2} d x = \frac{\pi}{2}$
$\lim_{x \to a} f ( x ) = l \Leftrightarrow \forall \epsilon > 0 \exists \delta > 0 : 0 < | x - a | < \delta \Rightarrow | f ( x ) - l | < \epsilon$
$\frac{1}{1 + \frac{1}{1 + \ldots}}$
$x := y$
$\int \vec{A} \cdot \vec{d l} = \int \int \vec{B} \cdot \vec{d S}$
$\frac{1}{1 + \frac{1}{1 + \frac{1}{1 + \frac{1}{1 + \ldots}}}} = \frac{\sqrt{5} - 1}{2}$
$\left[ a_0 , a_1 \ldots a_{n - 1} \right]$
$\left[ d_0 , d_1 \ldots d_{n - 1} \right]$
$n$
$o$
$o = \sum_{i = 0}^n \left( a_i \cdot \prod_{j = 0}^{i - 1} d_j \right)$
$a = [ 1 , 1 , 1 ] ; n = 3 ; d = [ 2 , 3 , 2 ] ; o = \sum_{i = 0}^3 \left( a_i \cdot \prod_{j = 0}^{i - 1} d_j \right) = ( 1 ) + ( 1 \cdot ( 2 ) ) + ( 1 \cdot ( 2 \cdot 3 ) ) = 1 + 2 + 6 = 9$
$o = i_0 + d_0 \left[ i_1 + d_1 \left[ \ldots \left[ i_{n - 1} \right] \right] \right]$
$g o f = I d_e$
$\max$
$\sin^{- 1} ( x )$
$\int$
$\oint$
$\partial$
$\nabla$
$\pm$
$\emptyset$
$\infty$
$\aleph$
$\angle$
$\therefore$
$\ldots$
$\cdots$
$\vdots$
$\ddots$
$a \, b$
$\,\,$
$\diamond$
$\square$
$\lfloor$
$\rfloor$
$\lceil$
$\rceil$
$\mathds{C}$
$\mathds{N}$
$\mathds{Q}$
$\mathds{R}$
$\mathds{Z}$
\end{document}