Rodrigues' formula

Template:Short description Template:For In mathematics, Rodrigues' formula (formerly called the Ivory–Jacobi formula) generates the Legendre polynomials. It was independently introduced by Template:Harvs, Template:Harvs and Template:Harvs. The name "Rodrigues formula" was introduced by Heine in 1878, after Hermite pointed out in 1865 that Rodrigues was the first to discover it. The term is also used to describe similar formulas for other orthogonal polynomials. Template:Harvtxt describes the history of the Rodrigues formula in detail.

Statement

Let $(P_n(x){)}_{n=0}^{\mathrm{\infty }}$ be a sequence of orthogonal polynomials on the interval $[a,b]$ with respect to weight function $w(x)$. That is, they have degrees $\mathrm{deg}(P_n)=n$, satisfy the orthogonality condition $${\int }_a^b{P}_m(x)P_n(x)w(x)dx=K_n{\delta }_{m,n}$$ where $K_n$ are nonzero constants depending on $n$, and ${\delta }_{m,n}$ is the Kronecker delta. The interval $[a,b]$ may be infinite in one or both ends.

More abstractly, this can be viewed through Sturm–Liouville theory. Define an operator $Lf:=-\frac{1}{w}(W{f}^{\prime }{)}^{\prime }$, then the differential equation is equivalent to $L{P}_n={\lambda }_n{P}_n$. Define the functional space $X=L^2([a,b],w(x)dx)$ as the Hilbert space of functions over $[a,b]$, such that $⟨f,g⟩:={\int }_a^{b}fgw$. Then the operator $L$ is self-adjoint on functions satisfying certain boundary conditions, allowing us to apply the spectral theorem.

Generating function

A simple argument using Cauchy's integral formula shows that the orthogonal polynomials obtained from the Rodrigues formula have a generating function of the form

$G(x,u)=\sum _{n=0}^{\mathrm{\infty }}{u}^n{P}_n(x)$

The $P_n(x)$ functions here may not have the standard normalizations. But we can write this equivalently as

$G(x,u)=\sum _{n=0}^{\mathrm{\infty }}\frac{u^n}{N_n}{N}_n{P}_n(x)$

where the $N_n$ are chosen according to the application so as to give the desired normalizations. The variable u may be replaced by a constant multiple of u so that

$G(x,\alpha u)=\sum _{n=0}^{\mathrm{\infty }}\frac{{\alpha }^n{u}^n}{N_n}{N}_n{P}_n(x)$

This gives an alternate form of the generating function.

By Cauchy's integral formula, Rodrigues’ formula is equivalent to$$P_n(x)=\frac{n!}{2\pi i}\frac{c_n}{w(x)}{\oint }_C\frac{B^n(t)w(t)}{(t-x{)}^{n+1}}dt$$where the integral is along a counterclockwise closed loop around $x$. Let

$u=\frac{t-x}{B(t)}$

Then the complex path integral takes the form

$P_n(x)=\frac{n!}{2\pi i}{c}_n{\oint }_C\frac{G(x,u)}{u^{n+1}}du$

$G(x,u)=\frac{w(t)\frac{dt}{du}}{w(x)B(t)}$

where now the closed path C encircles the origin. In the equation for $G(x,u)$, $t$ is an implicit function of $u$. Expanding $G(x,u)$ in the power series given earlier gives

$\frac{1}{2\pi i}{\oint }_C\frac{G(x,u)}{u^{n+1}}du=\frac{1}{2\pi i}{\oint }_C\frac{\sum _{m=0}^{\mathrm{\infty }}{u}^m{P}_m(x)}{u^{n+1}}du=P_n(x)$

Only the $m=n$ term has a nonzero residue, which is $P_n(x)$. The $n!c_n$ coefficient was dropped since normalizations are conventions which can be inserted afterwards as discussed earlier.

By expressing t in terms of u in the general formula just given for $G(x,u)$, explicit formulas for $G(x,u)$ may be found. As a simple example, let $B(x)=1$ and $A(x)=-x$ (Hermite polynomials) so that $w(x)=\exp (-\frac{x^2}{2})$, $t=u+x$, $w(t)=\exp (-\frac{(u+x{)}^2}{2})$ and so $G(x,u)=\exp (-xu-\frac{u^2}{2})$.

Examples

Family	$[a,b]$	$w$	$W$	$A$	$B$	$c_n$
Legendre $P_n$	$[-1,+1]$	$1$	$1-x^2$	$-2x$	$1-x^2$	$\frac{(-1{)}^n}{2^{n}n!}$
Chebyshev (of the first kind) $T_n$	$[-1,+1]$	$1/\sqrt{1-x^2}$	$\sqrt{1-x^2}$	$-x$	$1-x^2$	$\frac{(-1{)}^n}{(2n-1)!!}$
Chebyshev (of the second kind) $U_n$	$[-1,+1]$	$\sqrt{1-x^2}$	$(1-x^2{)}^{3/2}$	$-3x$	$1-x^2$	$\frac{(-1{)}^n(n+1)}{(2n+1)!!}$
Gegenbauer/ultraspherical $C_n^{(\alpha )}(x)$	$[-1,+1]$	$(1-x{)}^{\alpha -1/2}(1+x{)}^{\alpha -1/2}$	$(1-x{)}^{\alpha +1/2}(1+x{)}^{\alpha +1/2}$	$-(2\alpha +1)x$	$1-x^2$	$\frac{(-1{)}^n(2\alpha {)}_n}{(\alpha +\frac{1}{2}{)}_n{2}^{n}n!}$
Jacobi $P_n^{(\alpha ,\beta )}$	$[-1,+1]$	$(1-x{)}^{\alpha }(1+x{)}^{\beta }$	$(1-x{)}^{\alpha +1}(1+x{)}^{\beta +1}$	$(\beta -\alpha )-(\alpha +\beta +2)x$	$1-x^2$	$\frac{(-1{)}^n}{2^{n}n!}$
associated Laguerre $L_n^{(\alpha )}$	$[0,\mathrm{\infty })$	$x^{\alpha }{e}^{-x}$	$x^{\alpha +1}{e}^{-x}$	$\alpha +1-x$	$x$	$\frac{1}{n!}$
physicist's Hermite $H_n$	$(-\mathrm{\infty },+\mathrm{\infty })$	$e^{-x^2}$	$e^{-x^2}$	$-2x$	$1$	$(-1{)}^n$

These formulae are for the classical orthogonal polynomials. Similar formulae hold for many other sequences of orthogonal functions arising from Sturm–Liouville equations, and these are also called the Rodrigues formula (or Rodrigues' type formula), especially when the resulting sequence is polynomial.

Legendre

Source:

Rodrigues stated his formula for Legendre polynomials $P_n$:

$$P_n(x)=\frac{1}{2^{n}n!}\frac{d^n}{d{x}^n}[(x^2-1{)}^n].$$ $$(1-x^2){P_n}^{″}(x)-2x{P_n}^{\prime }(x)+n(n+1)P_n(x)=0$$

For Legendre polynomials, the generating function is defined as

$G(x,u)=\sum _{n=0}^{\mathrm{\infty }}{u}^n{P}_n(x)$.

The contour integral gives the Schläfli integral for Legendre polynomials:

$$P_n(x)=\frac{1}{2\pi i{2}^n}{\oint }_C\frac{(t^2-1{)}^n}{(t-x{)}^{n+1}}dt$$

Summing up the integrand

$$G(x,u)=\frac{1}{\sqrt{1-2ux+u^2}}\frac{1}{2\pi i}{\oint }_C(\frac{1}{t-t_{-}}-\frac{1}{t-t_{+}})dt$$

where $t_{\pm }=\frac{1}{u}(1\pm \sqrt{1-2ux+u^2})$. For small $u$, we have $t_{-}\approx x,t_{+}\to \mathrm{\infty }$, which heuristically suggests that the integral should be the residue around $t_{-}$, thus giving

$$G(x,u)=\frac{1}{\sqrt{1-2ux+u^2}}$$

Hermite

Source:

Physicist's Hermite polynomials:

$$H_n(x)=(-1{)}^n{e}^{x^2}\frac{d^n}{d{x}^n}\left[e^{-x^2}\right]={(2x-\frac{d}{dx})}^n\cdot 1.$$$${H_n}^{″}-2x{H_n}^{\prime }+2n{H}_n=0$$

The generating function is defined as

$$G(x,u)=\sum _{n=0}^{\mathrm{\infty }}\frac{H_n(x)}{n!}{u}^n.$$

The contour integral gives

$$H_n(x)=(-1{)}^n{e}^{x^2}\frac{n!}{2\pi i}{\oint }_C\frac{e^{-t^2}}{(t-x{)}^{n+1}}dt.$$

$$\begin{array}{cc}G(x,u)& =\sum _{n=0}^{\mathrm{\infty }}\frac{(-1{)}^n{e}^{x^2}}{n!}\frac{n!}{2\pi i}{u}^n{\oint }_C\frac{e^{-t^2}}{(t-x{)}^{n+1}}dt\\ & =e^{x^2}\frac{1}{2\pi i}{\oint }_C{e}^{-t^2}\left(\sum _{n=0}^{\mathrm{\infty }}\frac{(-1{)}^n{u}^n}{(t-x{)}^{n+1}}\right)dt\\ & =e^{x^2}\frac{1}{2\pi i}{\oint }_C{e}^{-t^2}\frac{1}{t-x+u}\\ & =e^{x^2}{e}^{-(x-u{)}^2}\\ & =e^{2xu-u^2}\end{array}$$

Laguerre

Source:

For associated Laguerre polynomials

$$L_n^{(\alpha )}(x)=\frac{x^{-\alpha }{e}^x}{n!}\frac{d^n}{d{x}^n}\left(e^{-x}{x}^{n+\alpha }\right)=\frac{x^{-\alpha }}{n!}{(\frac{d}{dx}-1)}^n{x}^{n+\alpha }.$$

$$x{L}_n^{(\alpha )}(x{)}^{″}+(\alpha +1-x)L_n^{(\alpha )}(x{)}^{\prime }+n{L}_n^{(\alpha )}(x)=0.$$

The generating function is defined as

$$G(x,u):=\sum _{n=0}^{\mathrm{\infty }}{u}^n{L}_n^{(\alpha )}(x)$$

By the same method, we have $G(x,u)=\frac{1}{(1-u{)}^{\alpha +1}}{e}^{-\frac{ux}{1-u}}$.

Jacobi

Source:

$$P_n^{(\alpha ,\beta )}(x)=\frac{(-1{)}^n}{2^{n}n!}(1-x{)}^{-\alpha }(1+x{)}^{-\beta }\frac{d^n}{d{x}^n}\{(1-x{)}^{\alpha }(1+x{)}^{\beta }{(1-x^2)}^n\}.$$$$(1-x^2)P_n^{(\alpha ,\beta )}{}^{″}+(\beta -\alpha -(\alpha +\beta +2)x)P_n^{(\alpha ,\beta )}{}^{\prime }+n(n+\alpha +\beta +1)P_n^{(\alpha ,\beta )}=0.$$

$\sum _{n=0}^{\mathrm{\infty }}{P}_n^{(\alpha ,\beta )}(x)u^n=2^{\alpha +\beta }{R}^{-1}(1-u+R{)}^{-\alpha }(1+u+R{)}^{-\beta },$

where $R=\sqrt{1-2ux+u^2}$, and the branch of square root is chosen so that $R(x,0)=1$.

See also

• Classical orthogonal polynomials

References

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