The inverse tangent integral is defined by:

${\displaystyle \operatorname {Ti} _{2}(x)=\int _{0}^{x}{\frac {\arctan t}{t}}\,dt}$ 

The arctangent is taken to be the principal branch; that is, −π/2 < arctan(t) < π/2 for all real t.^[1]

Its power series representation is

${\displaystyle \operatorname {Ti} _{2}(x)=x-{\frac {x^{3}}{3^{2}}}+{\frac {x^{5}}{5^{2}}}-{\frac {x^{7}}{7^{2}}}+\cdots }$ 

which is absolutely convergent for ${\displaystyle |x|\leq 1.}$ ^[1]

The inverse tangent integral is closely related to the dilogarithm ${\textstyle \operatorname {Li} _{2}(z)=\sum _{n=1}^{\infty }{\frac {z^{n}}{n^{2}}}}$  and can be expressed simply in terms of it:

${\displaystyle \operatorname {Ti} _{2}(z)={\frac {1}{2i}}\left(\operatorname {Li} _{2}(iz)-\operatorname {Li} _{2}(-iz)\right)}$ 

That is,

${\displaystyle \operatorname {Ti} _{2}(x)=\operatorname {Im} (\operatorname {Li} _{2}(ix))}$ 

for all real x.^[1]

The inverse tangent integral is an odd function:^[1]

${\displaystyle \operatorname {Ti} _{2}(-x)=-\operatorname {Ti} _{2}(x)}$ 

The values of Ti₂(x) and Ti₂(1/x) are related by the identity

${\displaystyle \operatorname {Ti} _{2}(x)-\operatorname {Ti} _{2}\left({\frac {1}{x}}\right)={\frac {\pi }{2}}\log x}$ 

valid for all x > 0 (or, more generally, for Re(x) > 0). This can be proven by differentiating and using the identity ${\displaystyle \arctan(t)+\arctan(1/t)=\pi /2}$ .^[2][3]

The special value Ti₂(1) is Catalan's constant ${\textstyle 1-{\frac {1}{3^{2}}}+{\frac {1}{5^{2}}}-{\frac {1}{7^{2}}}+\cdots \approx 0.915966}$ .^[3]

Similar to the polylogarithm ${\textstyle \operatorname {Li} _{n}(z)=\sum _{k=1}^{\infty }{\frac {z^{k}}{k^{n}}}}$ , the function

${\displaystyle \operatorname {Ti} _{n}(x)=\sum \limits _{k=0}^{\infty }{\frac {(-1)^{k}x^{2k+1}}{\left(2k+1\right)^{n}}}=x-{\frac {x^{3}}{3^{n}}}+{\frac {x^{5}}{5^{n}}}-{\frac {x^{7}}{7^{n}}}+\cdots }$ 

is defined analogously. This satisfies the recurrence relation:^[4]

${\displaystyle \operatorname {Ti} _{n}(x)=\int _{0}^{x}{\frac {\operatorname {Ti} _{n-1}(t)}{t}}\,dt}$ 

By this series representation it can be seen that the special values ${\displaystyle \operatorname {Ti} _{n}(1)=\beta (n)}$ , where ${\displaystyle \beta (s)}$  represents the Dirichlet beta function.

The inverse tangent integral is related to the Legendre chi function ${\textstyle \chi _{2}(x)=x+{\frac {x^{3}}{3^{2}}}+{\frac {x^{5}}{5^{2}}}+\cdots }$  by:^[1]

${\displaystyle \operatorname {Ti} _{2}(x)=-i\chi _{2}(ix)}$ 

Note that ${\displaystyle \chi _{2}(x)}$  can be expressed as ${\textstyle \int _{0}^{x}{\frac {\operatorname {artanh} t}{t}}\,dt}$ , similar to the inverse tangent integral but with the inverse hyperbolic tangent instead.

The inverse tangent integral can also be written in terms of the Lerch transcendent ${\textstyle \Phi (z,s,a)=\sum _{n=0}^{\infty }{\frac {z^{n}}{(n+a)^{s}}}:}$ ^[5]

${\displaystyle \operatorname {Ti} _{2}(x)={\frac {1}{4}}x\Phi (-x^{2},2,1/2)}$ 

The notation Ti₂ and Ti_n is due to Lewin. Spence (1809)^[6] studied the function, using the notation ${\displaystyle {\overset {n}{\operatorname {C} }}(x)}$ . The function was also studied by Ramanujan.^[2]

• Lewin, L. (1958). Dilogarithms and Associated Functions. London: Macdonald. MR 0105524. Zbl 0083.35904.
• Lewin, L. (1981). Polylogarithms and Associated Functions. New York: North-Holland. ISBN 978-0-444-00550-2.