29.6 Fourier Series29.8 Integral Equations

§29.7 Asymptotic Expansions

Contents

§29.7(i) Eigenvalues

29.7.6\tau _{2}=\frac{1}{2^{{10}}}(1+k^{2})(1-k^{2})^{2}(5p^{4}+34p^{2}+9),
29.7.7\tau _{3}=\frac{p}{2^{{14}}}((1+k^{2})^{4}(33p^{4}+410p^{2}+405)-24k^{2}(1+k^{2})^{2}(7p^{4}+90p^{2}+95)+16k^{4}(9p^{4}+130p^{2}+173)),
29.7.8\tau _{4}=\frac{1}{2^{{16}}}((1+k^{2})^{5}(63p^{6}+1260p^{4}+2943p^{2}+486)-8k^{2}(1+k^{2})^{3}(49p^{6}+1010p^{4}+2493p^{2}+432)+16k^{4}(1+k^{2})(35p^{6}+760p^{4}+2043p^{2}+378)).

Formulas for additional terms can be computed with the author’s Maple program LA5; see §29.22.

§29.7(ii) Lamé Functions

Müller (1966a, b) found three formal asymptotic expansions for a fundamental system of solutions of (29.2.1) (and (29.11.1)) as \nu\to\infty, one in terms of Jacobian elliptic functions and two in terms of Hermite polynomials. In Müller (1966c) it is shown how these expansions lead to asymptotic expansions for the Lamé functions \mathop{\mathit{Ec}^{{m}}_{{\nu}}\/}\nolimits\!\left(z,k^{2}\right) and \mathop{\mathit{Es}^{{m}}_{{\nu}}\/}\nolimits\!\left(z,k^{2}\right). Weinstein and Keller (1985) give asymptotics for solutions of Hill’s equation (§28.29(i)) that are applicable to the Lamé equation.