2001
DOI: 10.1139/p01-034
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Asymptotic expansions of the oblate spheroidal eigenvalues and wave functions for large parameter c

Abstract: The asymptotic expansion of the oblate spheroidal eigenfunctions can be expanded in terms of the Laguerre functions of the first and second kinds, from which their asymptotic eigenvalue can be expressed in an inverse power series of c, where the parameter c is proportional to the operating frequency. Analytical expressions of the eigenvalue coefficients, as well as those of the expansion coefficients of the eigenfunctions, are derived and verified with numerical results. PACS Nos.: 02.30Gp, 03.65ge

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Cited by 7 publications
(9 citation statements)
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“…The asymptotic expansion typically applied to the oblate ASWF (OASWF) (case 3 of Equation (1)) and its characteristic eigenvalue for the case of purely imaginary c, or c ⇒ −ic, consists of a similar method to that described by Equations (8)- (12) for the PSWF [19,31]. Similar to the case above, we designate all asymptotic expansions typically applied to the OSWF for purely imaginary c as oblate-type although as will be seen in Section 3.3, this expansion can also be applied to the PSWF in the case of arbitrary complex c. The original differential equation for the OASWF is…”
Section: Oblate-type Asymptotic Expansionmentioning
confidence: 99%
See 1 more Smart Citation
“…The asymptotic expansion typically applied to the oblate ASWF (OASWF) (case 3 of Equation (1)) and its characteristic eigenvalue for the case of purely imaginary c, or c ⇒ −ic, consists of a similar method to that described by Equations (8)- (12) for the PSWF [19,31]. Similar to the case above, we designate all asymptotic expansions typically applied to the OSWF for purely imaginary c as oblate-type although as will be seen in Section 3.3, this expansion can also be applied to the PSWF in the case of arbitrary complex c. The original differential equation for the OASWF is…”
Section: Oblate-type Asymptotic Expansionmentioning
confidence: 99%
“…Miles [22,23] provided compact, Bessel and Airy function expansions (used in part in Section 5) for [24] (for the prolate case), and Cloizeaux and Mehta [25], also made strides in providing uniform asymptotic expansions for Equation (1), and Sink and Eu [26] provided a WKB approximation for the ASWF. More recently, asymptotic expansions of λ mn for large c or n, m = 0 have been proposed in [27], expansions of Equation (1) as they relate to the quantum shell model for both large n and large c have been proposed by [28,29], and the work of Do-Nhat [30,31] summarizes and provides more details of Flammer's expansions for Equation (1) cases 1 and 3. Evaluation of the SWFs for complex size parameter c = c r + c i i, where c r = {c} and c i = {c}, has received less attention for both the standard and asymptotic regimes.…”
Section: Introductionmentioning
confidence: 99%
“…Other asymptotic results based on WKB methods have been obtained by Sink, and Eu [13]. Recently, asymptotic expansions of λ m ℓ (c) for large l, and c have been proposed by Guimaräes [14], de Moraes and Guimaräes [15], and the work of Do-Nhat [16,17] summarizes and provides more details of Flammer's expansions for λ m ℓ (c). Nevertheless, because of the complexity of the angular spheroidal wave equation with arbitrary complex size parameter c = c r + c i i, where c r = Re{c}, and c i = Im{c}, evaluation of λ m ℓ (c) in this regime has been much less studied.…”
Section: Introductionmentioning
confidence: 99%
“…In the asymptotic regime in which the parameter c = kF (k, operating wavenumber; F, semifocal length of a spheroid) is much greater than one, research was pioneered by Flammer [1] and was subsequently developed by Do-Nhat [2,3] for prolate and oblate spheroidal eigenvalues. In this regime, the work of Barrowes et al [4] was extended to c being a complex variable to compute the branch points of the spheroidal eigenvalues.…”
Section: Introductionmentioning
confidence: 99%