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11: 28.19 Expansions in Series of me ν + 2 n Functions
28.19.2 f ( z ) = n = f n me ν + 2 n ( z , q ) ,
28.19.3 f n = 1 π 0 π f ( z ) me ν + 2 n ( z , q ) d z .
28.19.4 e i ν z = n = c 2 n ν + 2 n ( q ) me ν + 2 n ( z , q ) ,
where the coefficients are as in §28.14.
12: 33.8 Continued Fractions
33.8.2 H ± H ± = c ± i ρ a b 2 ( ρ η ± i ) + ( a + 1 ) ( b + 1 ) 2 ( ρ η ± 2 i ) + ,
13: 24.6 Explicit Formulas
24.6.1 B 2 n = k = 2 2 n + 1 ( 1 ) k 1 k ( 2 n + 1 k ) j = 1 k 1 j 2 n ,
24.6.2 B n = 1 n + 1 k = 1 n j = 1 k ( 1 ) j j n ( n + 1 k j ) / ( n k ) ,
24.6.3 B 2 n = k = 1 n ( k 1 ) ! k ! ( 2 k + 1 ) ! j = 1 k ( 1 ) j 1 ( 2 k k + j ) j 2 n .
24.6.4 E 2 n = k = 1 n 1 2 k 1 j = 1 k ( 1 ) j ( 2 k k j ) j 2 n ,
24.6.9 B n = k = 0 n 1 k + 1 j = 0 k ( 1 ) j ( k j ) j n ,
14: 20.6 Power Series
Here the coefficients are given by
20.6.6 δ 2 j ( τ ) = n = m = | m | + | n | 0 ( m + n τ ) 2 j ,
20.6.7 α 2 j ( τ ) = n = m = ( m 1 2 + n τ ) 2 j ,
20.6.8 β 2 j ( τ ) = n = m = ( m 1 2 + ( n 1 2 ) τ ) 2 j ,
20.6.9 γ 2 j ( τ ) = n = m = ( m + ( n 1 2 ) τ ) 2 j ,
15: 2.9 Difference Equations
Often f ( n ) and g ( n ) can be expanded in series …Formal solutions are … c 0 = 1 , and higher coefficients are determined by formal substitution. … with a 0 , j = 1 and higher coefficients given by (2.9.7) (in the present case the coefficients of a s , j and a s 1 , j are zero). … The coefficients b s and constant c are again determined by formal substitution, beginning with c = 1 when α 2 α 1 = 0 , or with b 0 = 1 when α 2 α 1 = 1 , 2 , 3 , . …
16: 16.24 Physical Applications
§16.24(iii) 3 j , 6 j , and 9 j Symbols
The 3 j symbols, or Clebsch–Gordan coefficients, play an important role in the decomposition of reducible representations of the rotation group into irreducible representations. …The coefficients of transformations between different coupling schemes of three angular momenta are related to the Wigner 6 j symbols. …
17: 33.20 Expansions for Small | ϵ |
where
33.20.4 𝖥 k ( ; r ) = p = 2 k 3 k ( 2 r ) ( p + 1 ) / 2 C k , p J 2 + 1 + p ( 8 r ) , r > 0 ,
The functions J and I are as in §§10.2(ii), 10.25(ii), and the coefficients C k , p are given by C 0 , 0 = 1 , C 1 , 0 = 0 , and … where A ( ϵ , ) is given by (33.14.11), (33.14.12), and …The functions Y and K are as in §§10.2(ii), 10.25(ii), and the coefficients C k , p are given by (33.20.6). …
18: 18.22 Hahn Class: Recurrence Relations and Differences
18.22.2 x p n ( x ) = A n p n + 1 ( x ) ( A n + C n ) p n ( x ) + C n p n 1 ( x ) ,
18.22.5 ( a + i x ) q n ( x ) = A ~ n q n + 1 ( x ) ( A ~ n + C ~ n ) q n ( x ) + C ~ n q n 1 ( x ) ,
18.22.10 A ( x ) p n ( x + 1 ) ( A ( x ) + C ( x ) ) p n ( x ) + C ( x ) p n ( x 1 ) n ( n + α + β + 1 ) p n ( x ) = 0 ,
18.22.12 A ( x ) p n ( x + 1 ) ( A ( x ) + C ( x ) ) p n ( x ) + C ( x ) p n ( x 1 ) + λ n p n ( x ) = 0 .
18.22.14 A ( x ) p n ( x + i ) ( A ( x ) + C ( x ) ) p n ( x ) + C ( x ) p n ( x i ) + n ( n + 2 ( a + b ) 1 ) p n ( x ) = 0 ,
19: 34.14 Tables
Biedenharn and Louck (1981) give tables of algebraic expressions for Clebsch–Gordan coefficients and 6 j symbols, together with a bibliography of tables produced prior to 1975. In Varshalovich et al. (1988) algebraic expressions for the Clebsch–Gordan coefficients with all parameters 5 and numerical values for all parameters 3 are given on pp. …
20: 5.8 Infinite Products
5.8.4 k = 1 m a k = k = 1 m b k ,
5.8.5 k = 0 ( a 1 + k ) ( a 2 + k ) ( a m + k ) ( b 1 + k ) ( b 2 + k ) ( b m + k ) = Γ ( b 1 ) Γ ( b 2 ) Γ ( b m ) Γ ( a 1 ) Γ ( a 2 ) Γ ( a m ) ,