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31: 30.3 Eigenvalues
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►With , the spheroidal wave functions are solutions of Equation (30.2.1) which are bounded on , or equivalently, which are of the form where is an entire function of .
These solutions exist only for eigenvalues , , of the parameter .
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►The eigenvalues are analytic functions of the real variable and satisfy
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►has the solutions , .
If is an odd positive integer, then Equation (30.3.5) has the solutions , .
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32: 29.6 Fourier Series
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§29.6(i) Function
… ►In the special case , , there is a unique nontrivial solution with the property , . … ►§29.6(ii) Function
… ►§29.6(iii) Function
… ►§29.6(iv) Function
…33: 26.6 Other Lattice Path Numbers
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is the number of lattice paths from to that stay on or above the line and are composed of directed line segments of the form , , or .
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26.6.7
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26.6.8
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26.6.11
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26.6.14
34: 29.12 Definitions
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►The Lamé functions , , and , , are called the Lamé
polynomials.
…where , .
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►where , , are either or .
The polynomial is of degree and has zeros (all simple) in and zeros (all simple) in .
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►defined for with
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35: 34.3 Basic Properties: Symbol
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►When any one of is equal to , or , the symbol has a simple algebraic form.
…For these and other results, and also cases in which any one of is or , see Edmonds (1974, pp. 125–127).
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►Even permutations of columns of a symbol leave it unchanged; odd permutations of columns produce a phase factor , for example,
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34.3.13
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34.3.15
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36: 28.14 Fourier Series
37: 30.16 Methods of Computation
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►and real eigenvalues , , , , arranged in ascending order of magnitude.
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►For , , ,
…which yields .
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►If is known, then can be found by summing (30.8.1).
The coefficients are computed as the recessive solution of (30.8.4) (§3.6), and normalized via (30.8.5).
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