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16 Generalized Hypergeometric Functions & Meijer G-FunctionApplications

§16.24 Physical Applications

Contents
  1. §16.24(i) Random Walks
  2. §16.24(ii) Loop Integrals in Feynman Diagrams
  3. §16.24(iii) \mathit{3j}, \mathit{6j}, and \mathit{9j} Symbols

§16.24(i) Random Walks

Generalized hypergeometric functions and Appell functions appear in the evaluation of the so-called Watson integrals which characterize the simplest possible lattice walks. They are also potentially useful for the solution of more complicated restricted lattice walk problems, and the 3D Ising model; see Barber and Ninham (1970, pp. 147–148).

§16.24(ii) Loop Integrals in Feynman Diagrams

Appell functions are used for the evaluation of one-loop integrals in Feynman diagrams. See Cabral-Rosetti and Sanchis-Lozano (2000).

For an extension to two-loop integrals see Moch et al. (2002).

§16.24(iii) \mathit{3j}, \mathit{6j}, and \mathit{9j} Symbols

The \mathit{3j} 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 {{}_{3}F_{2}} functions with unit argument. The coefficients of transformations between different coupling schemes of three angular momenta are related to the Wigner \mathit{6j} symbols. These are balanced {{}_{4}F_{3}} functions with unit argument. Lastly, special cases of the \mathit{9j} symbols are {{}_{5}F_{4}} functions with unit argument. For further information see Chapter 34 and Varshalovich et al. (1988, §§8.2.5, 8.8, and 9.2.3).