where
are the unassociated Legendre polynomials. The associated Legendre polynomials for
negative
are then defined by
(3)
There are two sign conventions for associated Legendre polynomials. Some authors (e.g., Arfken 1985, pp. 668-669) omit the Condon-Shortley
phase, while others include it (e.g., Abramowitz and Stegun
1972, Press et al. 1992, and the LegendreP[l,
m, z] command in the Wolfram
Language). Care is therefore needed in comparing polynomials obtained from different
sources. One possible way to distinguish the two conventions is due to Abramowitz
and Stegun (1972, p. 332), who use the notation
(4)
to distinguish the two.
Associated polynomials are sometimes called Ferrers' functions (Sansone 1991, p. 246). If ,
they reduce to the unassociated polynomials. The associated
Legendre functions are part of the spherical harmonics,
which are the solution of Laplace's equation
in spherical coordinates. They are orthogonal
over
with the weighting function 1
(5)
and orthogonal over with respect to with the weighting function ,
(6)
The associated Legendre polynomials also obey the following recurrence
relations
(7)
Letting
(commonly denoted in this context),
(8)
(9)
Additional identities are
(10)
(11)
Including the factor of , the first few associated Legendre polynomials are
(12)
(13)
(14)
(15)
(16)
(17)
(18)
(19)
(20)
(21)
(22)
(23)
(24)
(25)
(26)
(27)
Written in terms (commonly written ), the first few become
(28)
(29)
(30)
(31)
(32)
(33)
(34)
(35)
(36)
(37)
The derivative about the origin is
(38)
(Abramowitz and Stegun 1972, p. 334), and the logarithmic derivative is