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11: 29.21 Tables
  • Arscott and Khabaza (1962) tabulates the coefficients of the polynomials P in Table 29.12.1 (normalized so that the numerically largest coefficient is unity, i.e. monic polynomials), and the corresponding eigenvalues h for k 2 = 0.1 ( .1 ) 0.9 , n = 1 ( 1 ) 30 . Equations from §29.6 can be used to transform to the normalization adopted in this chapter. Precision is 6S.

  • 12: 34.1 Special Notation
    An often used alternative to the 3 j symbol is the Clebsch–Gordan coefficient
    34.1.1 ( j 1 m 1 j 2 m 2 | j 1 j 2 j 3 m 3 ) = ( 1 ) j 1 j 2 + m 3 ( 2 j 3 + 1 ) 1 2 ( j 1 j 2 j 3 m 1 m 2 m 3 ) ;
    For other notations for 3 j , 6 j , 9 j symbols, see Edmonds (1974, pp. 52, 97, 104–105) and Varshalovich et al. (1988, §§8.11, 9.10, 10.10).
    13: 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.
    14: 26.16 Multiset Permutations
    The number of elements in 𝔖 S is the multinomial coefficient26.4) ( a 1 + a 2 + + a n a 1 , a 2 , , a n ) . … Thus inv ( 351322453154 ) = 4 + 8 + 0 + 3 + 1 + 1 + 2 + 3 + 1 + 0 + 1 = 24 , and maj ( 351322453154 ) = 2 + 4 + 8 + 9 + 11 = 34 . 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: 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 ) + ,
    16: 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 ,
    17: 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 ,
    18: 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 , . …
    19: 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. …
    20: 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). …