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21: 30.2 Differential Equations
The Liouville normal form of equation (30.2.1) is …
22: 18.36 Miscellaneous Polynomials
They are related to Hermite–Padé approximation and can be used for proofs of irrationality or transcendence of interesting numbers. … Orthogonality of the the classical OP’s with respect to a positive weight function, as in Table 18.3.1 requires, via Favard’s theorem, A n A n 1 C n > 0 for n 1 as per (18.2.9_5). … These results are proven in Everitt et al. (2004), via construction of a self-adjoint Sturm–Liouville operator which generates the L n ( k ) ( x ) polynomials, self-adjointness implying both orthogonality and completeness. … The y ( x ) = L ^ n ( k ) ( x ) satisfy a second order Sturm–Liouville eigenvalue problem of the type illustrated in Table 18.8.1, as satisfied by classical OP’s, but now with rational, rather than polynomial coefficients: … In §18.39(i) it is seen that the functions, w ( x ) H ^ n + 3 ( x ) , are solutions of a Schrödinger equation with a rational potential energy; and, in spite of first appearances, the Sturm oscillation theorem, Simon (2005c, Theorem 3.3, p. 35), is satisfied. …
23: 2.8 Differential Equations with a Parameter
In Case III f ( z ) has a simple pole at z 0 and ( z z 0 ) 2 g ( z ) is analytic at z 0 . … First we apply the Liouville transformation1.13(iv)) to (2.8.1). … In Case III the approximating equation is … For connection formulas for LiouvilleGreen approximations across these transition points see Olver (1977b, a, 1978). … For examples of uniform asymptotic approximations in terms of Whittaker functions with fixed second parameter see §18.15(i) and §28.8(iv). …
24: 15.16 Products
25: 3.7 Ordinary Differential Equations
§3.7(iv) Sturm–Liouville Eigenvalue Problems
The Sturm–Liouville eigenvalue problem is the construction of a nontrivial solution of the system …
26: 1.9 Calculus of a Complex Variable
DeMoivre’s Theorem
Jordan Curve Theorem
Cauchy’s Theorem
Liouville’s Theorem
Dominated Convergence Theorem
27: 18.38 Mathematical Applications
§18.38(i) Classical OP’s: Numerical Analysis
Approximation Theory
For these results and applications in approximation theory see §3.11(ii) and Mason and Handscomb (2003, Chapter 3), Cheney (1982, p. 108), and Rivlin (1969, p. 31). … The basic ideas of Gaussian quadrature, and their extensions to non-classical weight functions, and the computation of the corresponding quadrature abscissas and weights, have led to discrete variable representations, or DVRs, of Sturm–Liouville and other differential operators. …
18.38.3 m = 0 n P m ( α , 0 ) ( x ) = ( α + 2 ) n n ! F 2 3 ( n , n + α + 2 , 1 2 ( α + 1 ) α + 1 , 1 2 ( α + 3 ) ; 1 2 ( 1 x ) ) 0 , x 1 , α 2 , n = 0 , 1 , ,
28: 1.15 Summability Methods
For α > 0 and x 0 , the Riemann-Liouville fractional integral of order α is defined by …
§1.15(viii) Tauberian Theorems
29: 2.6 Distributional Methods
§2.6 Distributional Methods
§2.6(ii) Stieltjes Transform
Corresponding results for the generalized Stieltjes transformThe Riemann–Liouville fractional integral of order μ is defined by … For rigorous derivations of these results and also order estimates for δ n ( x ) , see Wong (1979) and Wong (1989, Chapter 6).
30: 27.3 Multiplicative Properties
Examples are 1 / n and λ ( n ) , and the Dirichlet characters, defined in §27.8. …