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21: 29.7 Asymptotic Expansions
§29.7(i) Eigenvalues
29.7.1 a ν m ( k 2 ) p κ τ 0 τ 1 κ 1 τ 2 κ 2 ,
The same Poincaré expansion holds for b ν m + 1 ( k 2 ) , since
29.7.5 b ν m + 1 ( k 2 ) a ν m ( k 2 ) = O ( ν m + 3 2 ( 1 k 1 + k ) ν ) , ν .
22: 30.3 Eigenvalues
§30.3 Eigenvalues
These solutions exist only for eigenvalues λ n m ( γ 2 ) , n = m , m + 1 , m + 2 , , of the parameter λ . …
§30.3(iii) Transcendental Equation
§30.3(iv) Power-Series Expansion
Further coefficients can be found with the Maple program SWF9; see §30.18(i).
23: 28.17 Stability as x ±
The boundary of each region comprises the characteristic curves a = a n ( q ) and a = b n ( q ) ; compare Figure 28.2.1.
See accompanying text
Figure 28.17.1: Stability chart for eigenvalues of Mathieu’s equation (28.2.1). Magnify
24: 28.35 Tables
§28.35 Tables
  • Blanch and Rhodes (1955) includes 𝐵𝑒 n ( t ) , 𝐵𝑜 n ( t ) , t = 1 2 q , n = 0 ( 1 ) 15 ; 8D. The range of t is 0 to 0.1, with step sizes ranging from 0.002 down to 0.00025. Notation: 𝐵𝑒 n ( t ) = a n ( q ) + 2 q ( 4 n + 2 ) q , 𝐵𝑜 n ( t ) = b n ( q ) + 2 q ( 4 n 2 ) q .

  • Ince (1932) includes eigenvalues a n , b n , and Fourier coefficients for n = 0 or 1 ( 1 ) 6 , q = 0 ( 1 ) 10 ( 2 ) 20 ( 4 ) 40 ; 7D. Also ce n ( x , q ) , se n ( x , q ) for q = 0 ( 1 ) 10 , x = 1 ( 1 ) 90 , corresponding to the eigenvalues in the tables; 5D. Notation: a n = 𝑏𝑒 n 2 q , b n = 𝑏𝑜 n 2 q .

  • National Bureau of Standards (1967) includes the eigenvalues a n ( q ) , b n ( q ) for n = 0 ( 1 ) 3 with q = 0 ( .2 ) 20 ( .5 ) 37 ( 1 ) 100 , and n = 4 ( 1 ) 15 with q = 0 ( 2 ) 100 ; Fourier coefficients for ce n ( x , q ) and se n ( x , q ) for n = 0 ( 1 ) 15 , n = 1 ( 1 ) 15 , respectively, and various values of q in the interval [ 0 , 100 ] ; joining factors g e , n ( q ) , f e , n ( q ) for n = 0 ( 1 ) 15 with q = 0 ( .5  to  10 ) 100 (but in a different notation). Also, eigenvalues for large values of q . Precision is generally 8D.

  • Blanch and Clemm (1969) includes eigenvalues a n ( q ) , b n ( q ) for q = ρ e i ϕ , ρ = 0 ( .5 ) 25 , ϕ = 5 ( 5 ) 90 , n = 0 ( 1 ) 15 ; 4D. Also a n ( q ) and b n ( q ) for q = i ρ , ρ = 0 ( .5 ) 100 , n = 0 ( 2 ) 14 and n = 2 ( 2 ) 16 , respectively; 8D. Double points for n = 0 ( 1 ) 15 ; 8D. Graphs are included.

  • 25: 30.16 Methods of Computation
    §30.16(i) Eigenvalues
    Approximations to eigenvalues can be improved by using the continued-fraction equations from §30.3(iii) and §30.8; see Bouwkamp (1947) and Meixner and Schäfke (1954, §3.93). … and real eigenvalues α 1 , d , α 2 , d , , α d , d , arranged in ascending order of magnitude. …The eigenvalues of 𝐀 can be computed by methods indicated in §§3.2(vi), 3.2(vii). … which yields λ 4 2 ( 10 ) = 13.97907 345 . …
    26: 12.16 Mathematical Applications
    Sleeman (1968b) considers certain orthogonality properties of the PCFs and corresponding eigenvalues. In Brazel et al. (1992) exponential asymptotics are considered in connection with an eigenvalue problem involving PCFs. …
    27: 30.18 Software
  • SWF1: λ n m ( γ 2 ) .

  • §30.18(ii) Eigenvalues λ n m ( γ 2 )
    28: 30.17 Tables
    §30.17 Tables
  • Stratton et al. (1956) tabulates quantities closely related to λ n m ( γ 2 ) and a n , k m ( γ 2 ) for 0 m 8 , m n 8 , 64 γ 2 64 . Precision is 7S.

  • Flammer (1957) includes 18 tables of eigenvalues, expansion coefficients, spheroidal wave functions, and other related quantities. Precision varies between 4S and 10S.

  • Van Buren et al. (1975) gives λ n 0 ( γ 2 ) , 𝖯𝗌 n 0 ( x , γ 2 ) for 0 n 49 , 1600 γ 2 1600 , 1 x 1 . Precision is 8S.

  • Zhang and Jin (1996) includes 24 tables of eigenvalues, spheroidal wave functions and their derivatives. Precision varies between 6S and 8S.

  • 29: Bibliography R
  • M. Reed and B. Simon (1978) Methods of Modern Mathematical Physics, Vol. 4, Analysis of Operators. Academic Press, New York.
  • S. Ritter (1998) On the computation of Lamé functions, of eigenvalues and eigenfunctions of some potential operators. Z. Angew. Math. Mech. 78 (1), pp. 66–72.
  • G. Rota, D. Kahaner, and A. Odlyzko (1973) On the foundations of combinatorial theory. VIII. Finite operator calculus. J. Math. Anal. Appl. 42, pp. 684–760.
  • J. Rushchitsky and S. Rushchitska (2000) On Simple Waves with Profiles in the form of some Special Functions—Chebyshev-Hermite, Mathieu, Whittaker—in Two-phase Media. In Differential Operators and Related Topics, Vol. I (Odessa, 1997), Operator Theory: Advances and Applications, Vol. 117, pp. 313–322.
  • 30: 3.2 Linear Algebra
    §3.2(iv) Eigenvalues and Eigenvectors
    §3.2(v) Condition of Eigenvalues
    has the same eigenvalues as 𝐀 . …
    §3.2(vii) Computation of Eigenvalues