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Gaussian elimination

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11: 26.9 Integer Partitions: Restricted Number and Part Size
26.9.4 [ m n ] q = j = 1 n 1 q m n + j 1 q j , n 0 ,
is the Gaussian polynomial (or q -binomial coefficient); see also §§17.2(i)17.2(ii). …
26.9.5 n = 0 p k ( n ) q n = j = 1 k 1 1 q j = 1 + m = 1 [ k + m 1 m ] q q m ,
12: 3.5 Quadrature
As in Simpson’s rule, by combining the rule for h with that for h / 2 , the first error term c 1 h 2 in (3.5.9) can be eliminated. With the Romberg scheme successive terms c 1 h 2 , c 2 h 4 , , in (3.5.9) are eliminated, according to the formula … For effective testing of Gaussian quadrature rules see Gautschi (1983). … Oscillatory integral transforms are treated in Wong (1982) by a method based on Gaussian quadrature. …
13: 8.24 Physical Applications
The function γ ( a , x ) appears in: discussions of power-law relaxation times in complex physical systems (Sornette (1998)); logarithmic oscillations in relaxation times for proteins (Metzler et al. (1999)); Gaussian orbitals and exponential (Slater) orbitals in quantum chemistry (Shavitt (1963), Shavitt and Karplus (1965)); population biology and ecological systems (Camacho et al. (2002)). …
14: 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). …
15: 1.13 Differential Equations
Elimination of First Derivative by Change of Dependent Variable
Elimination of First Derivative by Change of Independent Variable
16: 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)).
17: 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. …
18: 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 ,
19: 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 ,
20: 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). …