difference operators
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21—30 of 40 matching pages
21: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
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►For to be actually self adjoint it is necessary to also show that , as it is often the case that and have different domains, see Friedman (1990, p 148) for a simple example of such differences involving the differential operator
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22: Bibliography G
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WKB and turning point theory for second-order difference equations.
In Spectral Methods for Operators of Mathematical Physics,
Oper. Theory Adv. Appl., Vol. 154, pp. 101–138.
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23: Bibliography K
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Algorithm 910: a portable C++ multiple-precision system for special-function calculations.
ACM Trans. Math. Software 37 (4), pp. Art. 45, 27.
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24: Bibliography R
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Methods of Modern Mathematical Physics, Vol. 4, Analysis of Operators.
Academic Press, New York.
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Research Institute for Symbolic Computation, Hagenberg im Mühlkreis, Austria.
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On the computation of Lamé functions, of eigenvalues and eigenfunctions of some potential operators.
Z. Angew. Math. Mech. 78 (1), pp. 66–72.
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On the foundations of combinatorial theory. VIII. Finite operator calculus.
J. Math. Anal. Appl. 42, pp. 684–760.
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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.
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25: 23.1 Special Notation
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lattice in . | |
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set of all elements of , modulo elements of . Thus two elements of are equivalent if they are both in and their difference is in . (For an example see §20.12(ii).) | |
Cartesian product of groups and , that is, the set of all pairs of elements with group operation . |
26: 21.7 Riemann Surfaces
27: 2.1 Definitions and Elementary Properties
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►means that for each , the difference between and the th partial sum on the right-hand side is as in .
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28: 1.15 Summability Methods
29: 1.16 Distributions
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1.16.30
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30: Guide to Searching the DLMF
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