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11: 34.2 Definition: 3 j Symbol
The quantities j 1 , j 2 , j 3 in the 3 j symbol are called angular momenta. …The corresponding projective quantum numbers m 1 , m 2 , m 3 are given by …
34.2.4 ( j 1 j 2 j 3 m 1 m 2 m 3 ) = ( 1 ) j 1 j 2 m 3 Δ ( j 1 j 2 j 3 ) ( ( j 1 + m 1 ) ! ( j 1 m 1 ) ! ( j 2 + m 2 ) ! ( j 2 m 2 ) ! ( j 3 + m 3 ) ! ( j 3 m 3 ) ! ) 1 2 s ( 1 ) s s ! ( j 1 + j 2 j 3 s ) ! ( j 1 m 1 s ) ! ( j 2 + m 2 s ) ! ( j 3 j 2 + m 1 + s ) ! ( j 3 j 1 m 2 + s ) ! ,
where F 2 3 is defined as in §16.2. For alternative expressions for the 3 j symbol, written either as a finite sum or as other terminating generalized hypergeometric series F 2 3 of unit argument, see Varshalovich et al. (1988, §§8.21, 8.24–8.26).
12: 1.3 Determinants, Linear Operators, and Spectral Expansions
The cofactor A j k of a j k is … For real-valued a j k , … where ω 1 , ω 2 , , ω n are the n th roots of unity (1.11.21). … If 𝐷 n [ a j , k ] tends to a limit L as n , then we say that the infinite determinant 𝐷 [ a j , k ] converges and 𝐷 [ a j , k ] = L . … The corresponding eigenvectors 𝐚 1 , , 𝐚 n can be chosen such that they form a complete orthonormal basis in 𝐄 n . …
13: 1.12 Continued Fractions
A n and B n are called the n th (canonical) numerator and denominator respectively. … b 0 + a 1 b 1 + a 2 b 2 + is equivalent to b 0 + a 1 b 1 + a 2 b 2 + if there is a sequence { d n } n = 0 , d 0 = 1 ,
d n 0 , such that … Define … The continued fraction a 1 b 1 + a 2 b 2 + converges when … Then the convergents C n satisfy …
14: 26.9 Integer Partitions: Restricted Number and Part Size
p k ( n ) denotes the number of partitions of n into at most k parts. See Table 26.9.1. … It follows that p k ( n ) also equals the number of partitions of n into parts that are less than or equal to k . p k ( m , n ) is the number of partitions of n into at most k parts, each less than or equal to m . …
15: 16.12 Products
16.12.3 ( F 1 2 ( a , b c ; z ) ) 2 = k = 0 ( 2 a ) k ( 2 b ) k ( c 1 2 ) k ( c ) k ( 2 c 1 ) k k ! F 3 4 ( 1 2 k , 1 2 ( 1 k ) , a + b c + 1 2 , 1 2 a + 1 2 , b + 1 2 , 3 2 k c ; 1 ) z k , | z | < 1 .
16: 35.8 Generalized Hypergeometric Functions of Matrix Argument
The generalized hypergeometric function F q p with matrix argument 𝐓 𝓢 , numerator parameters a 1 , , a p , and denominator parameters b 1 , , b q is …
§35.8(iii) F 2 3 Case
Let c = b 1 + b 2 a 1 a 2 a 3 . … Let a 1 + a 2 + a 3 + 1 2 ( m + 1 ) = b 1 + b 2 ; one of the a j be a negative integer; ( b 1 a 1 ) , ( b 1 a 2 ) , ( b 1 a 3 ) , ( b 1 a 1 a 2 a 3 ) > 1 2 ( m 1 ) . … Again, let c = b 1 + b 2 a 1 a 2 a 3 . …
17: 16.1 Special Notation
p , q nonnegative integers.
a 1 , a 2 , , a p b 1 , b 2 , , b q } real or complex parameters.
𝐚 vector ( a 1 , a 2 , , a p ) .
𝐛 vector ( b 1 , b 2 , , b q ) .
The main functions treated in this chapter are the generalized hypergeometric function F q p ( a 1 , , a p b 1 , , b q ; z ) , the Appell (two-variable hypergeometric) functions F 1 ( α ; β , β ; γ ; x , y ) , F 2 ( α ; β , β ; γ , γ ; x , y ) , F 3 ( α , α ; β , β ; γ ; x , y ) , F 4 ( α , β ; γ , γ ; x , y ) , and the Meijer G -function G p , q m , n ( z ; a 1 , , a p b 1 , , b q ) . Alternative notations are F q p ( 𝐚 𝐛 ; z ) , F q p ( a 1 , , a p ; b 1 , , b q ; z ) , and F q p ( 𝐚 ; 𝐛 ; z ) for the generalized hypergeometric function, F 1 ( α , β , β ; γ ; x , y ) , F 2 ( α , β , β ; γ , γ ; x , y ) , F 3 ( α , α , β , β ; γ ; x , y ) , F 4 ( α , β ; γ , γ ; x , y ) , for the Appell functions, and G p , q m , n ( z ; 𝐚 ; 𝐛 ) for the Meijer G -function.
18: 16.18 Special Cases
The F 1 1 and F 1 2 functions introduced in Chapters 13 and 15, as well as the more general F q p functions introduced in the present chapter, are all special cases of the Meijer G -function. …
16.18.1 F q p ( a 1 , , a p b 1 , , b q ; z ) = ( k = 1 q Γ ( b k ) / k = 1 p Γ ( a k ) ) G p , q + 1 1 , p ( z ; 1 a 1 , , 1 a p 0 , 1 b 1 , , 1 b q ) = ( k = 1 q Γ ( b k ) / k = 1 p Γ ( a k ) ) G q + 1 , p p , 1 ( 1 z ; 1 , b 1 , , b q a 1 , , a p ) .
As a corollary, special cases of the F 1 1 and F 1 2 functions, including Airy functions, Bessel functions, parabolic cylinder functions, Ferrers functions, associated Legendre functions, and many orthogonal polynomials, are all special cases of the Meijer G -function. …
19: 16.3 Derivatives and Contiguous Functions
Two generalized hypergeometric functions F q p ( 𝐚 ; 𝐛 ; z ) are (generalized) contiguous if they have the same pair of values of p and q , and corresponding parameters differ by integers. …
16.3.7 F 2 3 ( a 1 + 2 , a 2 , a 3 b 1 , b 2 ; z ) a 1 ( a 1 + 1 ) ( 1 z ) + F 2 3 ( a 1 + 1 , a 2 , a 3 b 1 , b 2 ; z ) a 1 ( b 1 + b 2 3 a 1 2 + z ( 2 a 1 a 2 a 3 + 1 ) ) + F 2 3 ( a 1 , a 2 , a 3 b 1 , b 2 ; z ) ( ( 2 a 1 b 1 ) ( 2 a 1 b 2 ) + a 1 a 1 2 z ( a 1 a 2 ) ( a 1 a 3 ) ) F 2 3 ( a 1 1 , a 2 , a 3 b 1 , b 2 ; z ) ( a 1 b 1 ) ( a 1 b 2 ) = 0 .
20: 3.6 Linear Difference Equations
Given numerical values of w 0 and w 1 , the solution w n of the equation …These errors have the effect of perturbing the solution by unwanted small multiples of w n and of an independent solution g n , say. … The unwanted multiples of g n now decay in comparison with w n , hence are of little consequence. … The latter method is usually superior when the true value of w 0 is zero or pathologically small. … beginning with e 0 = w 0 . …