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单词 Legendre Polynomial
释义

Legendre Polynomial

The Legendre Functions of the First Kind are solutions to theLegendre Differential Equation. If is an Integer, they are Polynomials. Theyare a special case of the Ultraspherical Functions with . The Legendrepolynomials are illustrated above for and , 2, ..., 5.


The Rodrigues Formula provides the Generating Function

(1)

which yields upon expansion
(2)

where is the Floor Function. The Generating Function is
(3)

Take ,
(4)

Multiply (4) by ,
(5)

and add (3) and (5),


(6)


(7)

This expansion is useful in some physical problems, including expanding the Heyney-Greenstein phase function and computing the charge distribution on a Sphere. They satisfy theRecurrence Relation
(8)


The Legendre polynomials are orthogonal over with Weighting Function 1 and satisfy

(9)

where is the Kronecker Delta.


A Complex Generating Function is

(10)

and the Schläfli integral is
(11)


Additional integrals (Byerly 1959, p. 172) include


(12)


(13)

An additional identity is
(14)

(Szegö 1975, p. 348).


The first few Legendre polynomials are




The first few Powers in terms of Legendre polynomials are




For Legendre polynomials and Powers up to exponent 12, see Abramowitz and Stegun (1972, p. 798).


The Legendre Polynomials can also be generated using Gram-Schmidt Orthonormalization in theOpen Interval with the Weighting Function 1.


(15)
 
 (16)
 
 (17)
 
  
  
 (18)

Normalizing so that gives the expected Legendre polynomials.


The ``shifted'' Legendre polynomials are a set of functions analogous to the Legendre polynomials, but defined on theinterval (0, 1). They obey the Orthogonality relationship

(19)

The first few are





The associated Legendre polynomials are solutions to the associated Legendre Differential Equation,where is a Positive Integer and , ..., . They can be given in terms of the unassociated polynomials by

 
 (20)

where are the unassociated Legendre Polynomials. Note that some authors (e.g.,Arfken 1985, p. 668) omit the Condon-Shortley Phase , while others include it (e.g., Abramowitz and Stegun1972, Press et al. 1992, and the LegendreP[l,m,z] command of Mathematica). Abramowitz and Stegun(1972, p. 332) use the notation
(21)

to distinguish these two cases.


Associated polynomials are sometimes called Ferrers' Functions(Sansone 1991, p. 246). If , they reduce to the unassociated Polynomials. The associatedLegendre functions are part of the Spherical Harmonics, which are the solution ofLaplace's Equation in Spherical Coordinates. They are Orthogonal over with the Weighting Function 1

(22)

Orthogonal over with respect to with the Weighting Function
(23)

They obey the Recurrence Relations
(24)


 
 (25)


(26)


(27)

An identity relating associated Polynomials with Negative to the corresponding functions with Positive is
(28)

Additional identities are
(29)


(30)

Written in terms of and using the convention without a leading factor of (Arfken 1985, p. 669), the first few associated Legendre polynomials are




Written in terms , the first few become




The derivative about the origin is
(31)

(Abramowitz and Stegun 1972, p. 334), and the logarithmic derivative is


(32)

(Binney and Tremaine 1987, p. 654).

See also Condon-Shortley Phase, Conical Function, Gegenbauer Polynomial, Kings Problem, Laplace's Integral,Laplace-Mehler Integral, Super Catalan Number, Toroidal Function, Turán'sInequalities
References

Abramowitz, M. and Stegun, C. A. (Eds.). ``Legendre Functions'' and ``Orthogonal Polynomials.'' Ch. 22 in Chs. 8 and 22 in Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, 9th printing. New York: Dover, pp. 331-339 and 771-802, 1972.

Arfken, G. ``Legendre Functions.'' Ch. 12 in Mathematical Methods for Physicists, 3rd ed. Orlando, FL: Academic Press, pp. 637-711, 1985.

Binney, J. and Tremaine, S. ``Associated Legendre Functions.'' Appendix 5 in Galactic Dynamics. Princeton, NJ: Princeton University Press, pp. 654-655, 1987.

Byerly, W. E. An Elementary Treatise on Fourier's Series, and Spherical, Cylindrical, and Ellipsoidal Harmonics, with Applications to Problems in Mathematical Physics. New York: Dover, 1959.

Iyanaga, S. and Kawada, Y. (Eds.). ``Legendre Function'' and ``Associated Legendre Function.'' Appendix A, Tables 18.II and 18.III in Encyclopedic Dictionary of Mathematics. Cambridge, MA: MIT Press, pp. 1462-1468, 1980.

Legendre, A. M. ``Sur l'attraction des Sphéroides.'' Mém. Math. et Phys. présentés à l'Ac. r. des. sc. par divers savants 10, 1785.

Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill, pp. 593-597, 1953.

Press, W. H.; Flannery, B. P.; Teukolsky, S. A.; and Vetterling, W. T. Numerical Recipes in FORTRAN: The Art of Scientific Computing, 2nd ed. Cambridge, England: Cambridge University Press, p. 252, 1992.

Sansone, G. ``Expansions in Series of Legendre Polynomials and Spherical Harmonics.'' Ch. 3 in Orthogonal Functions, rev. English ed. New York: Dover, pp. 169-294, 1991.

Snow, C. Hypergeometric and Legendre Functions with Applications to Integral Equations of Potential Theory. Washington, DC: U. S. Government Printing Office, 1952.

Spanier, J. and Oldham, K. B. ``The Legendre Polynomials '' and ``The Legendre Functions and .'' Chs. 21 and 59 in An Atlas of Functions. Washington, DC: Hemisphere, pp. 183-192 and 581-597, 1987.

Szegö, G. Orthogonal Polynomials, 4th ed. Providence, RI: Amer. Math. Soc., 1975.


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