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11: 11.4 Basic Properties
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βΊwhere denotes either or .
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βΊ
βΊ
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βΊFor properties of zeros of see Steinig (1970).
βΊFor asymptotic expansions of zeros of see MacLeod (2002a).
12: 25.15 Dirichlet -functions
§25.15 Dirichlet -functions
βΊ§25.15(i) Definitions and Basic Properties
βΊThe notation was introduced by Dirichlet (1837) for the meromorphic continuation of the function defined by the series … … βΊ§25.15(ii) Zeros
…13: 23.1 Special Notation
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βΊ
βΊ
βΊThe main functions treated in this chapter are the Weierstrass -function ; the Weierstrass zeta function ; the Weierstrass sigma function ; the elliptic modular function ; Klein’s complete invariant ; Dedekind’s eta function .
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lattice in . | |
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Cartesian product of groups and , that is, the set of all pairs of elements with group operation . |
14: 18.39 Applications in the Physical Sciences
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βΊwhere is the (squared) angular momentum operator (14.30.12).
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βΊwith an infinite set of orthonormal eigenfunctions
… here being the order of the Laguerre polynomial, of Table 18.8.1, line 11, and the angular momentum quantum number, and where
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βΊThe bound state eigenfunctions of the radial Coulomb Schrödinger operator are discussed in §§18.39(i) and 18.39(ii), and the -function normalized (non-) in Chapter 33, where the solutions appear as Whittaker functions.
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βΊThe fact that non- continuum scattering eigenstates may be expressed in terms or (infinite) sums of functions allows a reformulation of scattering theory in atomic physics wherein no non- functions need appear.
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15: 18.14 Inequalities
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βΊ
18.14.8
, .
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βΊ
18.14.12
, .
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βΊLet the maxima , , of in be arranged so that
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βΊ
18.14.24
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βΊThe successive maxima of form a decreasing sequence for , and an increasing sequence for .
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16: 18.18 Sums
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βΊ
Expansion of functions
βΊIn all three cases of Jacobi, Laguerre and Hermite, if is on the corresponding interval with respect to the corresponding weight function and if are given by (18.18.1), (18.18.5), (18.18.7), respectively, then the respective series expansions (18.18.2), (18.18.4), (18.18.6) are valid with the sums converging in sense. … βΊ
18.18.12
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βΊ
18.18.37
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βΊ
18.18.40
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17: 18.6 Symmetry, Special Values, and Limits to Monomials
18: 18.17 Integrals
19: 18.1 Notation
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βΊ
βΊ
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βΊ
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βΊ
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Laguerre: and . ( with is also called Generalized Laguerre.)
Hermite: , .
-Laguerre: .
Continuous -Hermite: .