Legendre function

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In physical science and mathematics, the Legendre functions P_λ, Q_λ and associated Legendre functions P^μ
_λ, Q^μ
_λ, and Legendre functions of the second kind, Q_n, are all solutions of Legendre's differential equation. The Legendre polynomials and the associated Legendre polynomials are also solutions of the differential equation in special cases, which, by virtue of being polynomials, have a large number of additional properties, mathematical structure, and applications. For these polynomial solutions, see the separate Wikipedia articles.

The general Legendre equation reads $${\displaystyle \left(1-x^{2}\right)y''-2xy'+\left[\lambda (\lambda +1)-{\frac {\mu ^{2}}{1-x^{2}}}\right]y=0,}$$ where the numbers λ and μ may be complex, and are called the degree and order of the relevant function, respectively. The polynomial solutions when λ is an integer (denoted n), and μ = 0 are the Legendre polynomials P_n; and when λ is an integer (denoted n), and μ = m is also an integer with |m| < n are the associated Legendre polynomials. All other cases of λ and μ can be discussed as one, and the solutions are written P^μ
_λ, Q^μ
_λ. If μ = 0, the superscript is omitted, and one writes just P_λ, Q_λ. However, the solution Q_λ when λ is an integer is often discussed separately as Legendre's function of the second kind, and denoted Q_n.

This is a second order linear equation with three regular singular points (at 1, −1, and ∞). Like all such equations, it can be converted into a hypergeometric differential equation by a change of variable, and its solutions can be expressed using hypergeometric functions.

Since the differential equation is linear, homogeneous (the right hand side =zero) and of second order, it has two linearly independent solutions, which can both be expressed in terms of the hypergeometric function, ${\displaystyle _{2}F_{1}}$. With ${\displaystyle \Gamma }$ being the gamma function, the first solution is $${\displaystyle P_{\lambda }^{\mu }(z)={\frac {1}{\Gamma (1-\mu )}}\left[{\frac {z+1}{z-1}}\right]^{\mu /2}\,_{2}F_{1}\left(-\lambda ,\lambda +1;1-\mu ;{\frac {1-z}{2}}\right),\qquad {\text{for }}\ |1-z|<2,}$$ and the second is $${\displaystyle Q_{\lambda }^{\mu }(z)={\frac {{\sqrt {\pi }}\ \Gamma (\lambda +\mu +1)}{2^{\lambda +1}\Gamma (\lambda +3/2)}}{\frac {e^{i\mu \pi }(z^{2}-1)^{\mu /2}}{z^{\lambda +\mu +1}}}\,_{2}F_{1}\left({\frac {\lambda +\mu +1}{2}},{\frac {\lambda +\mu +2}{2}};\lambda +{\frac {3}{2}};{\frac {1}{z^{2}}}\right),\qquad {\text{for}}\ \ |z|>1.}$$

These are generally known as Legendre functions of the first and second kind of noninteger degree, with the additional qualifier 'associated' if μ is non-zero. A useful relation between the P and Q solutions is Whipple's formula.

For positive integer ${\displaystyle \mu =m\in \mathbb {N} ^{+}}$ the evaluation of ${\displaystyle P_{\lambda }^{\mu }}$ above involves cancellation of singular terms. We can find the limit valid for ${\displaystyle m\in \mathbb {N} _{0}}$ as^[1]

$${\displaystyle P_{\lambda }^{m}(z)=\lim _{\mu \to m}P_{\lambda }^{\mu }(z)={\frac {(-\lambda )_{m}(\lambda +1)_{m}}{m!}}\left[{\frac {1-z}{1+z}}\right]^{m/2}\,_{2}F_{1}\left(-\lambda ,\lambda +1;1+m;{\frac {1-z}{2}}\right),}$$

with ${\displaystyle (\lambda )_{n}}$ the (rising) Pochhammer symbol.

The nonpolynomial solution for the special case of integer degree ${\displaystyle \lambda =n\in \mathbb {N} _{0}}$, and ${\displaystyle \mu =0}$, is often discussed separately. It is given by $${\displaystyle Q_{n}(x)={\frac {n!}{1\cdot 3\cdots (2n+1)}}\left(x^{-(n+1)}+{\frac {(n+1)(n+2)}{2(2n+3)}}x^{-(n+3)}+{\frac {(n+1)(n+2)(n+3)(n+4)}{2\cdot 4(2n+3)(2n+5)}}x^{-(n+5)}+\cdots \right)}$$

This solution is necessarily singular when ${\displaystyle x=\pm 1}$.

The Legendre functions of the second kind can also be defined recursively via Bonnet's recursion formula $${\displaystyle Q_{n}(x)={\begin{cases}{\frac {1}{2}}\log {\frac {1+x}{1-x}}&n=0\\P_{1}(x)Q_{0}(x)-1&n=1\\{\frac {2n-1}{n}}xQ_{n-1}(x)-{\frac {n-1}{n}}Q_{n-2}(x)&n\geq 2\,.\end{cases}}}$$

The nonpolynomial solution for the special case of integer degree ${\displaystyle \lambda =n\in \mathbb {N} _{0}}$, and ${\displaystyle \mu =m\in \mathbb {N} _{0}}$ is given by $${\displaystyle Q_{n}^{m}(x)=(-1)^{m}(1-x^{2})^{\frac {m}{2}}{\frac {d^{m}}{dx^{m}}}Q_{n}(x)\,.}$$

The Legendre functions can be written as contour integrals. For example, $${\displaystyle P_{\lambda }(z)=P_{\lambda }^{0}(z)={\frac {1}{2\pi i}}\int _{1,z}{\frac {(t^{2}-1)^{\lambda }}{2^{\lambda }(t-z)^{\lambda +1}}}dt}$$ where the contour winds around the points 1 and z in the positive direction and does not wind around −1. For real x, we have $${\displaystyle P_{s}(x)={\frac {1}{2\pi }}\int _{-\pi }^{\pi }\left(x+{\sqrt {x^{2}-1}}\cos \theta \right)^{s}d\theta ={\frac {1}{\pi }}\int _{0}^{1}\left(x+{\sqrt {x^{2}-1}}(2t-1)\right)^{s}{\frac {dt}{\sqrt {t(1-t)}}},\qquad s\in \mathbb {C} }$$

The real integral representation of ${\displaystyle P_{s}}$ are very useful in the study of harmonic analysis on ${\displaystyle L^{1}(G//K)}$ where ${\displaystyle G//K}$ is the double coset space of ${\displaystyle SL(2,\mathbb {R} )}$ (see Zonal spherical function). Actually the Fourier transform on ${\displaystyle L^{1}(G//K)}$ is given by $${\displaystyle L^{1}(G//K)\ni f\mapsto {\hat {f}}}$$ where $${\displaystyle {\hat {f}}(s)=\int _{1}^{\infty }f(x)P_{s}(x)dx,\qquad -1\leq \Re (s)\leq 0}$$

Legendre functions P_λ of non-integer degree are unbounded at the interval [-1, 1] . In applications in physics, this often provides a selection criterion. Indeed, because Legendre functions Q_λ of the second kind are always unbounded, in order to have a bounded solution of Legendre's equation at all, the degree must be integer valued: only for integer degree, Legendre functions of the first kind reduce to Legendre polynomials, which are bounded on [-1, 1] . It can be shown^[2] that the singularity of the Legendre functions P_λ for non-integer degree is a consequence of the mirror symmetry of Legendre's equation. Thus there is a symmetry under the selection rule just mentioned.

• Ferrers function

• Abramowitz, Milton; Stegun, Irene Ann, eds. (1983) [June 1964]. "Chapter 8". Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. Applied Mathematics Series. Vol. 55 (Ninth reprint with additional corrections of tenth original printing with corrections (December 1972); first ed.). Washington D.C.; New York: United States Department of Commerce, National Bureau of Standards; Dover Publications. p. 332. ISBN 978-0-486-61272-0. LCCN 64-60036. MR 0167642. LCCN 65-12253.
• Courant, Richard; Hilbert, David (1953), Methods of Mathematical Physics, Volume 1, New York: Interscience Publisher, Inc.
• Dunster, T. M. (2010), "Legendre and Related Functions", in Olver, Frank W. J.; Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W. (eds.), NIST Handbook of Mathematical Functions, Cambridge University Press, ISBN 978-0-521-19225-5, MR 2723248.
• Ivanov, A.B. (2001) [1994], "Legendre function", Encyclopedia of Mathematics, EMS Press
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• Whittaker, E. T.; Watson, G. N. (1963), A Course in Modern Analysis, Cambridge University Press, ISBN 978-0-521-58807-2

• Legendre function P on the Wolfram functions site.
• Legendre function Q on the Wolfram functions site.
• Associated Legendre function P on the Wolfram functions site.
• Associated Legendre function Q on the Wolfram functions site.