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11: 20.13 Physical Applications
Then the nonperiodic Gaussian …Thus the classical theta functions are “periodized”, or “anti-periodized”, Gaussians; see Bellman (1961, pp. 18, 19). …
12: 35.1 Special Notation
a , b complex variables.
The main functions treated in this chapter are the multivariate gamma and beta functions, respectively Γ m ( a ) and B m ( a , b ) , and the special functions of matrix argument: Bessel (of the first kind) A ν ( 𝐓 ) and (of the second kind) B ν ( 𝐓 ) ; confluent hypergeometric (of the first kind) F 1 1 ( a ; b ; 𝐓 ) or F 1 1 ( a b ; 𝐓 ) and (of the second kind) Ψ ( a ; b ; 𝐓 ) ; Gaussian hypergeometric F 1 2 ( a 1 , a 2 ; b ; 𝐓 ) or F 1 2 ( a 1 , a 2 b ; 𝐓 ) ; generalized hypergeometric F q p ( a 1 , , a p ; b 1 , , b q ; 𝐓 ) or F q p ( a 1 , , a p b 1 , , b q ; 𝐓 ) . … Related notations for the Bessel functions are 𝒥 ν + 1 2 ( m + 1 ) ( 𝐓 ) = A ν ( 𝐓 ) / A ν ( 𝟎 ) (Faraut and Korányi (1994, pp. 320–329)), K m ( 0 , , 0 , ν | 𝐒 , 𝐓 ) = | 𝐓 | ν B ν ( 𝐒 𝐓 ) (Terras (1988, pp. 49–64)), and 𝒦 ν ( 𝐓 ) = | 𝐓 | ν B ν ( 𝐒 𝐓 ) (Faraut and Korányi (1994, pp. 357–358)).
13: 7.21 Physical Applications
Voigt functions 𝖴 ( x , t ) , 𝖵 ( x , t ) , can be regarded as the convolution of a Gaussian and a Lorentzian, and appear when the analysis of light (or particulate) absorption (or emission) involves thermal motion effects. …
14: 26.16 Multiset Permutations
The q -multinomial coefficient is defined in terms of Gaussian polynomials (§26.9(ii)) by
26.16.1 [ a 1 + a 2 + + a n a 1 , a 2 , , a n ] q = k = 1 n 1 [ a k + a k + 1 + + a n a k ] q ,
15: 17.2 Calculus
17.2.27 [ n m ] q = ( q ; q ) n ( q ; q ) m ( q ; q ) n m = ( q n ; q ) m ( 1 ) m q n m ( m 2 ) ( q ; q ) m ,
17.2.30 [ n m ] q = [ m + n 1 m ] q ( 1 ) m q m n ( m 2 ) ,
17.2.31 [ n m ] q = [ n 1 m 1 ] q + q m [ n 1 m ] q ,
16: 9.17 Methods of Computation
For details, including the application of a generalized form of Gaussian quadrature, see Gordon (1969, Appendix A) and Schulten et al. (1979). …
17: Philip J. Davis
An interesting anecdote told by Davis reveals that he and mathematician Philip Rabinowitz were dubbed “Heroes of the SEAC” when their Gaussian integration code executed correctly on its first run. …
18: 17.3 q -Elementary and q -Special Functions
17.3.8 A m , s ( q ) = q ( s m 2 ) + ( s 2 ) j = 0 s ( 1 ) j q ( j 2 ) [ m + 1 j ] q ( 1 q s j ) m ( 1 q ) m .
17.3.9 a m , s ( q ) = q ( s 2 ) ( 1 q ) s ( q ; q ) s j = 0 s ( 1 ) j q ( j 2 ) [ s j ] q ( 1 q s j ) m ( 1 q ) m .
19: 26.1 Special Notation
( m n ) binomial coefficient.
[ m n ] q Gaussian polynomial.
20: Bibliography F
  • B. D. Fried and S. D. Conte (1961) The Plasma Dispersion Function: The Hilbert Transform of the Gaussian. Academic Press, London-New York.
  • Y. V. Fyodorov (2005) Introduction to the Random Matrix Theory: Gaussian Unitary Ensemble and Beyond. In Recent Perspectives in Random Matrix Theory and Number Theory, London Math. Soc. Lecture Note Ser., Vol. 322, pp. 31–78.