Legendre chi function

Template:Short description In mathematics, the Legendre chi function (named after Adrien-Marie Legendre) is a special function whose Taylor series is also a Dirichlet series, given by $${\chi }_{\nu }(z)=\sum _{k=0}^{\mathrm{\infty }}\frac{z^{2k+1}}{(2k+1{)}^{\nu }}.$$

File:LegendreChi.svg

Legendre chi function

As such, it resembles the Dirichlet series for the polylogarithm, and, indeed, is trivially expressible in terms of the polylogarithm as $${\chi }_{\nu }(z)=\frac{1}{2}[{\mathrm{Li}}_{\nu }(z)-{\mathrm{Li}}_{\nu }(-z)].$$

The Legendre chi function appears as the discrete Fourier transform, with respect to the order ν, of the Hurwitz zeta function, and also of the Euler polynomials, with the explicit relationships given in those articles.

The Legendre chi function is a special case of the Lerch transcendent, and is given by $${\chi }_{\nu }(z)=2^{-\nu }z\mathrm{\Phi }(z^2,\nu ,1/2).$$

Identities

$${\chi }_2(x)+{\chi }_2(1/x)=\frac{{\pi }^2}{4}-\frac{i\pi }{2}\ln |x|.$$ $$\frac{d}{dx}{\chi }_2(x)=\frac{\mathrm{a}\mathrm{r}\mathrm{c}\mathrm{t}\mathrm{a}\mathrm{n}\mathrm{h}x}{x}.$$

Special Values

It takes the special values:

$${\chi }_2(i)=iK$$ $${\chi }_2(\sqrt{2}-1)=\frac{{\pi }^2}{16}-\frac{[\ln (\sqrt{2}+1){]}^2}{4}$$ $${\chi }_2(\frac{\sqrt{5}-1}{2})=\frac{{\pi }^2}{12}-\frac{3[\ln (\frac{\sqrt{5}+1}{2}){]}^2}{4}$$ $${\chi }_2(\sqrt{5}-2)=\frac{{\pi }^2}{24}-\frac{3[\ln (\frac{\sqrt{5}+1}{2}){]}^2}{4}$$ $${\chi }_2(-1)=-\frac{{\pi }^2}{8}$$ $${\chi }_2(1)=\frac{{\pi }^2}{8},$$

where $i$ is the imaginary unit and K is Catalan's constant. Other special values include:

$${\chi }_n(1)=\lambda (n)$$ $${\chi }_n(i)=i\beta (n),$$

where $\lambda (n)$ is the Dirichlet lambda function and $\beta (n)$ is the Dirichlet beta function.

Integral relations

$$\underset{0}{\overset{\pi /2}{\int }}\arcsin (r\sin \theta )d\theta ={\chi }_2\left(r\right),\underset{0}{\overset{\pi /2}{\int }}\arccos (r\cos \theta )d\theta ={\left(\frac{\pi }{2}\right)}^2-{\chi }_2\left(r\right)\mathrm{i}\mathrm{f}|r|\le 1$$ $$\underset{0}{\overset{\pi /2}{\int }}\arctan (r\sin \theta )d\theta =-\frac{1}{2}\underset{0}{\overset{\pi }{\int }}\frac{r\theta \cos \theta }{1+r^2{\sin }^2\theta }d\theta =2{\chi }_2\left(\frac{\sqrt{1+r^2}-1}{r}\right)$$ $$\underset{0}{\overset{\pi /2}{\int }}\arctan (p\sin \theta )\arctan (q\sin \theta )d\theta =\pi {\chi }_2(\frac{\sqrt{1+p^2}-1}{p}\cdot \frac{\sqrt{1+q^2}-1}{q})$$ $$\underset{0}{\overset{\alpha }{\int }}\underset{0}{\overset{\beta }{\int }}\frac{dxdy}{1-x^2{y}^2}={\chi }_2(\alpha \beta )\mathrm{i}\mathrm{f}|\alpha \beta |\le 1$$

References

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