Associated Legendre function

In mathematics and physics, an associated Legendre function P_l^(m) is related to a Legendre polynomial P_l by the following equation

$P_{\ell }^{(m)}(x)=(1-x^{2})^{m/2}{\frac {dP_{\ell }(x)}{dx^{\ell }}}.$

For even m the associated Legendre function is a polynomial, for odd m the function contains the factor (1-x ² )^½ and hence is not a polynomial.

The associated Legendre polynomials are important in quantum mechanics and potential theory.

Differential equation

Define

$\Pi _{\ell }^{(m)}(x)\equiv {\frac {d^{m}P_{\ell }(x)}{dx^{m}}},$

where P_l(x) is a Legendre polynomial. Differentiating the Legendre differential equation:

$(1-x^{2}){\frac {d^{2}\Pi _{\ell }^{(0)}(x)}{dx^{2}}}-2x{\frac {d\Pi _{\ell }^{(0)}(x)}{dx}}+\ell (\ell +1)\Pi _{\ell }^{(0)}(x)=0,$

m times gives an equation for Π^(m)_l

$(1-x^{2}){\frac {d^{2}\Pi _{\ell }^{(m)}(x)}{dx^{2}}}-2(m+1)x{\frac {d\Pi _{\ell }^{(m)}(x)}{dx}}+\left[\ell (\ell +1)-m(m+1)\right]\Pi _{\ell }^{(m)}(x)=0.$

After substitution of

$\Pi _{\ell }^{(m)}(x)=(1-x^{2})^{-m/2}P_{\ell }^{(m)}(x),$

we find, after multiplying through with $(1-x^{2})^{m/2}$, that the associated Legendre differential equation holds for the associated Legendre functions

$(1-x^{2}){\frac {d^{2}P_{\ell }^{(m)}(x)}{dx^{2}}}-2x{\frac {dP_{\ell }^{(m)}(x)}{dx}}+\left[\ell (\ell +1)-{\frac {m^{2}}{1-x^{2}}}\right]P_{\ell }^{(m)}(x).$

In physical applications usually x = cosθ, then then associated Legendre differential equation takes the form

${\frac {1}{\sin \theta }}{\frac {d}{d\theta }}\sin \theta {\frac {d}{d\theta }}P_{\ell }^{(m)}+\left[\ell (\ell +1)-{\frac {m^{2}}{\sin ^{2}\theta }}\right]P_{\ell }^{(m)}.$

Extension to negative m

By the Rodrigues formula, one obtains

$P_{\ell }^{(m)}(x)={\frac {1}{2^{\ell }\ell !}}(1-x^{2})^{m/2}\ {\frac {d^{\ell +m}}{dx^{\ell +m}}}(x^{2}-1)^{\ell }.$

This equation allows extension of the range of m to: -l ≤ m ≤ l.

Since the associated Legendre equation is invariant under the substitution m → -m, the equations for P_l^{( ±m)}, resulting from this expression, are proportional.

To obtain the proportionality constant we consider

$(1-x^{2})^{-m/2}{\frac {d^{\ell -m}}{dx^{\ell -m}}}(x^{2}-1)^{\ell }=c_{lm}(1-x^{2})^{m/2}{\frac {d^{\ell +m}}{dx^{\ell +m}}}(x^{2}-1)^{\ell },\qquad 0\leq m\leq \ell ,$

and we bring the factor (1-x²)^-m/2 to the other side. Equate the coefficient of the highest power of x on the left and right hand side of

${\frac {d^{\ell -m}}{dx^{\ell -m}}}(x^{2}-1)^{\ell }=c_{lm}(1-x^{2})^{m}{\frac {d^{\ell +m}}{dx^{\ell +m}}}(x^{2}-1)^{\ell },\qquad 0\leq m\leq \ell ,$

and it follows that the proportionality constant is

$c_{lm}=(-1)^{m}{\frac {(\ell -m)!}{(\ell +m)!}},\qquad 0\leq m\leq \ell ,$

so that the associated Legendre functions of same |m| are related to each other by

$P_{\ell }^{(-|m|)}(x)=(-1)^{m}{\frac {(\ell -|m|)!}{(\ell +|m|)!}}P_{\ell }^{(|m|)}(x).$

Note that the phase factor (-1)^m arising in this expression is not due to some arbitrary phase convention, but arises from expansion of (1-x²)^m.

Orthogonality relations

Important integral relations are

$\int _{-1}^{1}P_{\ell }^{(m)}(x)P_{\ell '}^{(m)}(x)dx={\frac {2\delta _{\ell \ell '}(\ell +m)!}{(2\ell +1)(\ell -m)!}}$

$\int _{-1}^{1}P_{\ell }^{(m)}(x)P_{\ell }^{(n)}(x){\frac {dx}{1-x^{2}}}={\frac {\delta _{mn}(\ell +m)!}{m(\ell -m)!}}$