Datasets:
deepcopy
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Azu-Handwritten-Mathematical-Expression

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v _ { c } = v _ { c - 1 } ( \frac { r - c } { c } )
train
\sum \sqrt { x }
train
- f ( x ) g ( x _ { 0 } ) + g ( x _ { 0 } ) f ( x )
train
| \int d ^ { 4 } x A ^ { a } ( x ) | < \infty
2019
\sum _ { a } n _ { a }
2016
g ( x , y ) = \sqrt [ 3 ] { x - y } + \sqrt { | x + y | }
train
\pi
train
\frac { 2 \tan \alpha } { 1 - \tan ^ { 2 } \alpha }
train
m _ { 0 } ( g _ { \alpha } ) = m _ { 0 } ( f )
train
\sum _ { n } \sin n \theta = 0
2016
\beta \leq P
train
\cos ( n X )
2019
- u - \sqrt { e }
train
4
train
R = \lim _ { n \rightarrow \infty } a _ { n } / a _ { n + 2 }
2016
[ a ] \times [ a ] \times [ a ]
2016
\frac { a _ { 1 } + a _ { 2 } + a ^ { 3 } } { 1 - x }
train
\sqrt [ n ] { 1 } = \cos \frac { 2 k \pi } { n } + i \sin \frac { 2 k \pi } { n }
train
( x _ { 1 } , x _ { 2 } , x _ { 3 } , \ldots ) + ( y _ { 1 } , y _ { 2 } , y _ { 3 } , \ldots ) = ( x _ { 1 } + y _ { 1 } , x _ { 2 } + y _ { 2 } , x _ { 3 } + y _ { 3 } , \ldots )
train
\lim _ { x \rightarrow - \infty } p _ { 2 } ( x ) > 0
2014
x ^ { 5 } - x + 1 = 0
train
x = y ^ { 2 }
train
n _ { 1 } \sin i _ { 1 } = n _ { 2 } \sin i _ { 2 }
train
( x + 1 ) ^ { n + 1 } = ( x + 1 ) ( x + 1 ) ^ { n }
train
\lim _ { y \rightarrow \infty } y \sin ( \frac { c } { y } ) = c
train
\frac { x ^ { 4 } } { 2 ^ { 3 } } - ( \frac { 2 } { x } ) ^ { - 4 }
train
- s + \frac { T } { L }
train
I V
train
\tan \theta = f
2019
\frac { 1 } { 2 } + \frac { 2 } { 3 } + \frac { 3 } { 4 } + \frac { 4 } { 5 } + \frac { 5 } { 6 }
train
s
train
f _ { p } ( X ) = \frac { 1 } { 1 - f ( p ) X }
train
[ A + H ]
train
d _ { q 2 } ^ { 2 } + d _ { 2 3 } ^ { 2 } + d _ { 3 4 } ^ { 2 }
train
\cdots + g - w
train
[ \sum h ] < \sum b + n
train
E - ( f )
train
\cos ( a )
2016
6 . 2
train
F ( x , y , z ) = G ( x , y ) + H ( y , z ) + 2 1
train
( a _ { 1 } b _ { 2 } + a _ { 2 } b _ { 1 } + a _ { 3 } b _ { 4 } - a _ { 4 } b _ { 3 } ) ^ { 2 }
train
( 9 - 0 )
train
3 6
train
2 , 7 \times 1 0 ^ { 4 4 }
train
a = a _ { 0 } + a _ { 1 } + \ldots + a _ { k }
2016
\frac { 1 } { \sin ( x ) + 1 }
train
\lim _ { n \rightarrow \infty } x _ { n } = L
train
q _ { a } ^ { d + I } ( \pi )
train
\frac { 1 } { a } F ( a x + b ) + C
train
A ( x ) = \frac { 1 } { x } + \frac { 1 } { x ^ { 2 } } + B ( x )
train
1 7 0 \pm 3 \div ( 1 5 6 + 1 8 0 )
train
\sqrt { x } ^ { k \Delta } ( i _ { L } )
train
v
train
1
train
\frac { a } { b } + \frac { c } { b } = \frac { a + c } { b }
2014
\frac { 1 } { \sin ( x ) + 1 }
train
z _ { 1 } ^ { 2 } + 1 ^ { z } - z _ { 2 } ^ { 2 } + 2 ^ { z }
train
\sin \frac { \pi } { 4 } = \cos \frac { \pi } { 4 } = \frac { \sqrt { 2 } } { 2 }
train
v _ { c } = v _ { c - 1 } ( \frac { r - c } { c } )
train
\int ( 2 ^ { x } - 3 e ^ { x } ) d x
train
x \in A
2019
y ^ { 4 } + y + 1 = 0
train
\frac { x ^ { i } _ { n } } { y ^ { b } _ { n } }
2019
3 ^ { 2 } - 1 = 8
train
u = \cos ( t )
train
k x = k _ { 0 } x ^ { 0 } + k _ { 1 } x ^ { 1 }
2016
P ( x ) = \sum _ { i = 0 } ^ { n } a _ { j } x ^ { j }
train
x = 3 i
train
1 + 2
train
n - 2 = 3
train
2 ^ { 1 8 }
train
\frac { n ^ { 2 } - n - 4 } { 2 n ( k + n + 1 ) } + \frac { 2 } { n k }
2016
( 2 0 0 1 ) 4 3 7 3 - 4 3 9 4
2019
i R
train
\tan ( \frac { \pi } { 2 } ) = \infty
train
l \sin y _ { 0 }
2019
F _ { n } = F _ { n - 1 } + F _ { n - 2 }
train
\sum _ { n = 1 } ^ { N } ( - 1 ) ^ { n } \sin ( n x )
train
\sum _ { a } j _ { a } + 1
2016
x _ { 1 } + x _ { 2 } = x _ { 3 }
train
\sum _ { n = 0 } ^ { \infty } f _ { n } ( x )
train
\sqrt { 1 + \sqrt { 2 + \sqrt { 3 + \sqrt { 4 } } } }
train
\sum v S
train
t
train
\frac { 3 } { 4 } = - \frac { 1 } { 2 } ( \frac { 1 } { 2 } + 1 )
2019
a ^ { p } + b ^ { p } = c ^ { p }
2014
t = \frac { t _ { 0 } } { \sqrt { 1 - \frac { v ^ { 2 } } { c ^ { 2 } } } }
train
\frac { a } { \sin A } = \frac { b } { \sin B } = \frac { c } { \sin C }
train
r = \sqrt { n }
train
\sqrt { 7 5 }
2014
R \sin \theta
2019
1 0 a _ { 5 } a _ { 2 } - 2 a _ { 4 } a _ { 3 } = 0
train
b = - c = \sin \alpha
2016
( 2 9 - 2 4 + 1 6 9 ) \times 8 8 \leq - 1 4 4 3 1
train
s
train
\lim _ { x \rightarrow 0 } \frac { 1 - \cos x } { x } = 0
train
\frac { 1 } { x } x = 1
2019
\int 2 x d x = x ^ { 2 } + C
train
\frac { 1 } { 2 } ( 3 x ^ { 2 } - 1 )
train
r _ { i } + d r _ { i } , p _ { i } + d p _ { i }
2014