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11: Nico M. Temme
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►In November 2015, Temme was named Senior Associate Editor of the DLMF and Associate Editor for Chapters 3, 6, 7, and 12.
12: 16.24 Physical Applications
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§16.24(iii) , , and Symbols
►The symbols, or Clebsch–Gordan coefficients, play an important role in the decomposition of reducible representations of the rotation group into irreducible representations. They can be expressed as functions with unit argument. The coefficients of transformations between different coupling schemes of three angular momenta are related to the Wigner symbols. These are balanced functions with unit argument. …13: 34.5 Basic Properties: Symbol
§34.5 Basic Properties: Symbol
… ►§34.5(ii) Symmetry
… ►§34.5(iv) Orthogonality
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… ►Equation (34.5.23) can be regarded as an alternative definition of the symbol. …14: 34.12 Physical Applications
§34.12 Physical Applications
►The angular momentum coupling coefficients (, , and symbols) are essential in the fields of nuclear, atomic, and molecular physics. …, and symbols are also found in multipole expansions of solutions of the Laplace and Helmholtz equations; see Carlson and Rushbrooke (1950) and Judd (1976).15: 26.10 Integer Partitions: Other Restrictions
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denotes the number of partitions of into parts with difference at least 3, except that multiples of 3 must differ by at least 6.
…The set is denoted by .
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►where the sum is over nonnegative integer values of for which .
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►Note that , with strict inequality for .
It is known that for , , with strict inequality for sufficiently large, provided that , or ; see Yee (2004).
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16: 24.2 Definitions and Generating Functions
17: 26.9 Integer Partitions: Restricted Number and Part Size
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►The conjugate to the example in Figure 26.9.1 is .
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►Equations (26.9.2)–(26.9.3) are examples of closed forms that can be computed explicitly for any positive integer .
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►equivalently, partitions into at most parts either have exactly parts, in which case we can subtract one from each part, or they have strictly fewer than parts.
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18: 28.6 Expansions for Small
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►Leading terms of the power series for and for are:
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►Higher coefficients in the foregoing series can be found by equating coefficients in the following continued-fraction equations:
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►Here for , for , and for and .
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►For ,
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►For the corresponding expansions of for change to everywhere in (28.6.26).
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19: 34.7 Basic Properties: Symbol
20: 23.20 Mathematical Applications
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►Points on the curve can be parametrized by , , where and : in this case we write .
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►The geometric nature of this construction is illustrated in McKean and Moll (1999, §2.14), Koblitz (1993, §§6, 7), and Silverman and Tate (1992, Chapter 1, §§3, 4): each of these references makes a connection with the addition theorem (23.10.1).
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must have one of the forms , or , or , .
…The order of a point (if finite and not already determined) can have only the values 3, 5, 6, 7, 9, 10, or 12, and so can be found from , , , , , , or .
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►See also Silverman and Tate (1992), Serre (1973, Part 2, Chapters 6, 7), Koblitz (1993), and Cornell et al. (1997).
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