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29 Lamé FunctionsLamé Polynomials

§29.12 Definitions

Contents
  1. §29.12(i) Elliptic-Function Form
  2. §29.12(ii) Algebraic Form
  3. §29.12(iii) Zeros

§29.12(i) Elliptic-Function Form

Throughout §§29.1229.16 the order \nu in the differential equation (29.2.1) is assumed to be a nonnegative integer.

The Lamé functions \mathit{Ec}^{m}_{\nu}\left(z,k^{2}\right), m=0,1,\dots,\nu, and \mathit{Es}^{m}_{\nu}\left(z,k^{2}\right), m=1,2,\dots,\nu, are called the Lamé polynomials. There are eight types of Lamé polynomials, defined as follows:

29.12.1 \mathit{uE}^{m}_{2n}\left(z,k^{2}\right)=\mathit{Ec}^{2m}_{2n}\left(z,k^{2}%
\right),
29.12.2 \mathit{sE}^{m}_{2n+1}\left(z,k^{2}\right)=\mathit{Ec}^{2m+1}_{2n+1}\left(z,k^%
{2}\right),
29.12.3 \mathit{cE}^{m}_{2n+1}\left(z,k^{2}\right)=\mathit{Es}^{2m+1}_{2n+1}\left(z,k^%
{2}\right),
29.12.4 \mathit{dE}^{m}_{2n+1}\left(z,k^{2}\right)=\mathit{Ec}^{2m}_{2n+1}\left(z,k^{2%
}\right),
29.12.5 \mathit{scE}^{m}_{2n+2}\left(z,k^{2}\right)=\mathit{Es}^{2m+2}_{2n+2}\left(z,k%
^{2}\right),
29.12.6 \mathit{sdE}^{m}_{2n+2}\left(z,k^{2}\right)=\mathit{Ec}^{2m+1}_{2n+2}\left(z,k%
^{2}\right),
29.12.7 \mathit{cdE}^{m}_{2n+2}\left(z,k^{2}\right)=\mathit{Es}^{2m+1}_{2n+2}\left(z,k%
^{2}\right),
29.12.8 \mathit{scdE}^{m}_{2n+3}\left(z,k^{2}\right)=\mathit{Es}^{2m+2}_{2n+3}\left(z,%
k^{2}\right),

where n=0,1,2,\dots, m=0,1,2,\dots,n. These functions are polynomials in \operatorname{sn}\left(z,k\right), \operatorname{cn}\left(z,k\right), and \operatorname{dn}\left(z,k\right). In consequence they are doubly-periodic meromorphic functions of z.

The superscript m on the left-hand sides of (29.12.1)–(29.12.8) agrees with the number of z-zeros of each Lamé polynomial in the interval (0,K), while n-m is the number of z-zeros in the open line segment from K to K+\mathrm{i}{K^{\prime}}.

The prefixes \mathit{u}, \mathit{s}, \mathit{c}, \mathit{d}, \mathit{sc}, \mathit{sd}, \mathit{cd}, \mathit{scd} indicate the type of the polynomial form of the Lamé polynomial; compare the 3rd and 4th columns in Table 29.12.1. In the fourth column the variable z and modulus k of the Jacobian elliptic functions have been suppressed, and P({\operatorname{sn}}^{2}) denotes a polynomial of degree n in {\operatorname{sn}}^{2}\left(z,k\right) (different for each type). For the determination of the coefficients of the P’s see §29.15(ii).

§29.12(ii) Algebraic Form

With the substitution \xi={\operatorname{sn}}^{2}\left(z,k\right) every Lamé polynomial in Table 29.12.1 can be written in the form

where \rho, \sigma, \tau are either 0 or \frac{1}{2}. The polynomial P(\xi) is of degree n and has m zeros (all simple) in (0,1) and n-m zeros (all simple) in (1,k^{-2}). The functions (29.12.9) satisfy (29.2.2).

§29.12(iii) Zeros

Let \xi_{1},\xi_{2},\dots,\xi_{n} denote the zeros of the polynomial P in (29.12.9) arranged according to

29.12.10 0<\xi_{1}<\cdots<\xi_{m}<1<\xi_{m+1}<\cdots<\xi_{n}<k^{-2}.

Then the function

29.12.11 g(t_{1},t_{2},\dots,t_{n})=\left(\prod_{p=1}^{n}t_{p}^{\rho+\frac{1}{4}}|t_{p}%
-1|^{\sigma+\frac{1}{4}}(k^{-2}-t_{p})^{\tau+\frac{1}{4}}\right)\prod_{q<r}(t_%
{r}-t_{q}),

defined for (t_{1},t_{2},\dots,t_{n}) with

29.12.12 0\leq t_{1}\leq\cdots\leq t_{m}\leq 1\leq t_{m+1}\leq\cdots\leq t_{n}\leq k^{-%
2},

attains its absolute maximum iff t_{j}=\xi_{j}, j=1,2,\dots,n. Moreover,

This result admits the following electrostatic interpretation: Given three point masses fixed at t=0, t=1, and t=k^{-2} with positive charges \rho+\tfrac{1}{4}, \sigma+\tfrac{1}{4}, and \tau+\tfrac{1}{4}, respectively, and n movable point masses at t_{1},t_{2},\dots,t_{n} arranged according to (29.12.12) with unit positive charges, the equilibrium position is attained when t_{j}=\xi_{j} for j=1,2,\dots,n.