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Verblunsky coefficients

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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: 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 ,
13: 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 ) + ,
14: 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 ,
15: 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 ,
16: 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 , . …
17: Errata
In regard to orthogonal polynomials on the unit circle, we now discuss monic polynomials, Verblunsky’s Theorem, and Szegő’s theorem. …
  • Section 16.11(i)

    A sentence indicating that explicit representations for the coefficients c k are given in Volkmer (2023) was inserted just below (16.11.5).

  • Additions

    Equations: (3.3.3_1), (3.3.3_2), (5.15.9) (suggested by Calvin Khor on 2021-09-04), (8.15.2), Pochhammer symbol representation in (10.17.1) for a k ( ν ) coefficient, Pochhammer symbol representation in (11.9.4) for a k ( μ , ν ) coefficient, and (12.14.4_5).

  • Section 34.1

    The reference for Clebsch-Gordan coefficients, Condon and Shortley (1935), was replaced by Edmonds (1974) and Rotenberg et al. (1959). The references for 3 j , 6 j , 9 j symbols were made more precise.

  • Equation (10.20.14)
    10.20.14 B 3 ( 0 ) = 959 71711 84603 25 47666 37125 00000 2 1 3

    Originally this coefficient was given incorrectly as B 3 ( 0 ) = 430 99056 39368 59253 5 68167 34399 42500 00000 2 1 3 . The other coefficients in this equation have not been changed.

    Reported 2012-05-11 by Antony Lee.

  • 18: 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. …
    19: 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). …
    20: 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 ,