self-adjoint extensions of differential operators
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11: 1.15 Summability Methods
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βΊ
is Abel summable to , or
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βΊ
is (C,1) summable to , or
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βΊIf converges and equals , then the integral is Abel and Cesàro summable to .
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βΊ
1.15.47
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βΊFor extensions of (1.15.48) see Love (1972b).
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12: 2.3 Integrals of a Real Variable
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βΊIn both cases the th error term is bounded in absolute value by , where the variational
operator
is defined by
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βΊFor an extension with more general -powers see Bleistein and Handelsman (1975, §4.1).
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βΊAnother extension is to more general factors than the exponential function.
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βΊFor extensions to oscillatory integrals with more general -powers and logarithmic singularities see Wong and Lin (1978) and Sidi (2010).
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βΊAssume also that and are continuous in and , and for each the minimum value of in is at , at which point vanishes, but both and are nonzero.
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13: 2.7 Differential Equations
§2.7 Differential Equations
… βΊFor extensions to singularities of higher rank see Olver and Stenger (1965). For extensions to higher-order differential equations see Stenger (1966a, b), Olver (1997a, 1999), and Olde Daalhuis and Olver (1998). … βΊand denotes the variational operator (§2.3(i)). … βΊThe first of these references includes extensions to complex variables and reversions for zeros. …14: 1.4 Calculus of One Variable
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βΊFor extensive tables of integrals, see Apelblat (1983), Bierens de Haan (1867), Gradshteyn and Ryzhik (2000), Gröbner and Hofreiter (1949, 1950), and Prudnikov et al. (1986a, b, 1990, 1992a, 1992b).
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βΊDefinite integrals over the Stieltjes measure could represent a sum, an integral, or a combination of the two.
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βΊIf , then is of bounded
variation on .
In this case, and are nondecreasing bounded functions and .
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βΊLastly, whether or not the real numbers and satisfy , and whether or not they are finite, we define
by (1.4.34) whenever this integral exists.
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15: Bibliography K
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βΊ
Some extensions of W. Gautschi’s inequalities for the gamma function.
Math. Comp. 41 (164), pp. 607–611.
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βΊ
An extension of Saalschütz’s summation theorem for the series
.
Integral Transforms Spec. Funct. 24 (11), pp. 916–921.
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Lowering and Raising Operators for Some Special Orthogonal Polynomials.
In Jack, Hall-Littlewood and Macdonald Polynomials,
Contemp. Math., Vol. 417, pp. 227–238.
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Fractional integral and generalized Stieltjes transforms for hypergeometric functions as transmutation operators.
SIGMA Symmetry Integrability Geom. Methods Appl. 11, pp. Paper 074, 22.
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βΊ
Construction of differential operators having Bochner-Krall orthogonal polynomials as eigenfunctions.
J. Math. Anal. Appl. 324 (1), pp. 285–303.
16: 2.8 Differential Equations with a Parameter
§2.8 Differential Equations with a Parameter
… βΊThe transformed differential equation is … βΊFor error bounds, extensions to pure imaginary or complex , an extension to inhomogeneous differential equations, and examples, see Olver (1997b, Chapter 10). … βΊFor error bounds, more delicate error estimates, extensions to complex and , zeros, connection formulas, extensions to inhomogeneous equations, and examples, see Olver (1997b, Chapters 11, 13), Olver (1964b), Reid (1974a, b), Boyd (1987), and Baldwin (1991). … βΊFor error bounds, more delicate error estimates, extensions to complex , , and , zeros, and examples see Olver (1997b, Chapter 12), Boyd (1990a), and Dunster (1990a). …17: 18.2 General Orthogonal Polynomials
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βΊ
§18.2(ii) -Difference Operators
βΊIf the orthogonality discrete set is or , then the role of the differentiation operator in the case of classical OP’s (§18.3) is played by , the forward-difference operator, or by , the backward-difference operator; compare §18.1(i). … βΊand similar extensions for (18.2.4_5) and (18.2.2). … βΊThe operator is a delta operator, i. … …18: 17.16 Mathematical Applications
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βΊIn Lie algebras Lepowsky and Milne (1978) and Lepowsky and Wilson (1982) laid foundations for extensive interaction with -series.
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19: 13.27 Mathematical Applications
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βΊVilenkin (1968, Chapter 8) constructs irreducible representations of this group, in which the diagonal matrices correspond to operators of multiplication by an exponential function.
The other group elements correspond to integral operators whose kernels can be expressed in terms of Whittaker functions.
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βΊFor applications of Whittaker functions to the uniform asymptotic theory of differential equations with a coalescing turning point and simple pole see §§2.8(vi) and 18.15(i).
20: Bibliography S
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An Introduction to the Operations with Series.
2nd edition, Chelsea Publishing Co., New York.
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The Bound State of Weakly Coupled Schrödinger Operators in One and Two Dimensions.
Annals of Physics 97 (2), pp. 279–288.
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βΊ
Operators with Singular Continuous Spectrum: I. General Operators.
Annals of Mathematics 141 (1), pp. 131–145.
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βΊ
Prolate spheroidal wave functions, Fourier analysis and uncertainity. IV. Extensions to many dimensions; generalized prolate spheroidal functions.
Bell System Tech. J. 43, pp. 3009–3057.
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βΊ
An extension of Airy’s equation.
SIAM J. Appl. Math. 15 (6), pp. 1400–1412.
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