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21: 34.8 Approximations for Large Parameters
34.8.1 { j 1 j 2 j 3 j 2 j 1 l 3 } = ( 1 ) j 1 + j 2 + j 3 + l 3 ( 4 π ( 2 j 1 + 1 ) ( 2 j 2 + 1 ) ( 2 l 3 + 1 ) sin θ ) 1 2 ( cos ( ( l 3 + 1 2 ) θ 1 4 π ) + o ( 1 ) ) , j 1 , j 2 , j 3 l 3 1 ,
34.8.2 cos θ = j 1 ( j 1 + 1 ) + j 2 ( j 2 + 1 ) j 3 ( j 3 + 1 ) 2 j 1 ( j 1 + 1 ) j 2 ( j 2 + 1 ) ,
22: 17.4 Basic Hypergeometric Functions
§17.4(i) ϕ s r Functions
Here and elsewhere it is assumed that the b j do not take any of the values q n . …
§17.4(ii) ψ s r Functions
Here and elsewhere the b j must not take any of the values q n , and the a j must not take any of the values q n + 1 . … For the function H r r see §16.4(v). …
23: 16.11 Asymptotic Expansions
For subsequent use we define two formal infinite series, E p , q ( z ) and H p , q ( z ) , as follows: …and b q + 1 = 1 . Explicit representations for the coefficients c k are given in Volkmer (2023). … In this subsection we assume that none of a 1 , a 2 , , a p is a nonpositive integer. … Explicit representations for the coefficients c k are given in Volkmer and Wood (2014). …
24: 5.10 Continued Fractions
where
a 0 = 1 12 ,
a 1 = 1 30 ,
a 2 = 53 210 ,
For exact values of a 7 to a 11 and 40S values of a 0 to a 40 , see Char (1980). …
25: 16.19 Identities
16.19.1 G p , q m , n ( 1 z ; a 1 , , a p b 1 , , b q ) = G q , p n , m ( z ; 1 b 1 , , 1 b q 1 a 1 , , 1 a p ) ,
16.19.2 z μ G p , q m , n ( z ; a 1 , , a p b 1 , , b q ) = G p , q m , n ( z ; a 1 + μ , , a p + μ b 1 + μ , , b q + μ ) ,
16.19.3 G p + 1 , q + 1 m , n + 1 ( z ; a 0 , , a p b 1 , , b q , a 0 ) = G p , q m , n ( z ; a 1 , , a p b 1 , , b q ) ,
16.19.5 ϑ G p , q m , n ( z ; a 1 , , a p b 1 , , b q ) = G p , q m , n ( z ; a 1 1 , a 2 , , a p b 1 , , b q ) + ( a 1 1 ) G p , q m , n ( z ; a 1 , , a p b 1 , , b q ) ,
16.19.6 0 1 t a 0 ( 1 t ) a 0 b q + 1 1 G p , q m , n ( z t ; a 1 , , a p b 1 , , b q ) d t = Γ ( a 0 b q + 1 ) G p + 1 , q + 1 m , n + 1 ( z ; a 0 , , a p b 1 , , b q + 1 ) ,
26: 17.5 ϕ 0 0 , ϕ 0 1 , ϕ 1 1 Functions
§17.5 ϕ 0 0 , ϕ 0 1 , ϕ 1 1 Functions
17.5.1 ϕ 0 0 ( ; ; q , z ) = n = 0 ( 1 ) n q ( n 2 ) z n ( q ; q ) n = ( z ; q ) ;
27: 10.75 Tables
  • Achenbach (1986) tabulates J 0 ( x ) , J 1 ( x ) , Y 0 ( x ) , Y 1 ( x ) , x = 0 ( .1 ) 8 , 20D or 18–20S.

  • Abramowitz and Stegun (1964, Chapter 11) tabulates 0 x J 0 ( t ) d t , 0 x Y 0 ( t ) d t , x = 0 ( .1 ) 10 , 10D; 0 x t 1 ( 1 J 0 ( t ) ) d t , x t 1 Y 0 ( t ) d t , x = 0 ( .1 ) 5 , 8D.

  • Achenbach (1986) tabulates I 0 ( x ) , I 1 ( x ) , K 0 ( x ) , K 1 ( x ) , x = 0 ( .1 ) 8 , 19D or 19–21S.

  • Leung and Ghaderpanah (1979), tabulates all zeros of the principal value of K n ( z ) , for n = 2 ( 1 ) 10 , 29S.

  • Abramowitz and Stegun (1964, Chapter 11) tabulates e x 0 x I 0 ( t ) d t , e x x K 0 ( t ) d t , x = 0 ( .1 ) 10 , 7D; e x 0 x t 1 ( I 0 ( t ) 1 ) d t , x e x x t 1 K 0 ( t ) d t , x = 0 ( .1 ) 5 , 6D.

  • 28: 16.8 Differential Equations
    is a value z 0 of z at which all the coefficients f j ( z ) , j = 0 , 1 , , n 1 , are analytic. If z 0 is not an ordinary point but ( z z 0 ) n j f j ( z ) , j = 0 , 1 , , n 1 , are analytic at z = z 0 , then z 0 is a regular singularity. … where α j and β j are constants. … where indicates that the entry 1 + b j b j is omitted. … where indicates that the entry 1 a j + a j is omitted. …
    29: 3.7 Ordinary Differential Equations
    The path is partitioned at P + 1 points labeled successively z 0 , z 1 , , z P , with z 0 = a , z P = b . … Write τ j = z j + 1 z j , j = 0 , 1 , , P , expand w ( z ) and w ( z ) in Taylor series (§1.10(i)) centered at z = z j , and apply (3.7.2). … If, for example, β 0 = β 1 = 0 , then on moving the contributions of w ( z 0 ) and w ( z P ) to the right-hand side of (3.7.13) the resulting system of equations is not tridiagonal, but can readily be made tridiagonal by annihilating the elements of 𝐀 P that lie below the main diagonal and its two adjacent diagonals. … The values λ k are the eigenvalues and the corresponding solutions w k of the differential equation are the eigenfunctions. … where h = z n + 1 z n and …
    30: 16.2 Definition and Analytic Properties
    Throughout this chapter it is assumed that none of the bottom parameters b 1 , b 2 , , b q is a nonpositive integer, unless stated otherwise. Then formally …Equivalently, the function is denoted by F q p ( 𝐚 𝐛 ; z ) or F q p ( 𝐚 ; 𝐛 ; z ) , and sometimes, for brevity, by F q p ( z ) . … Suppose first one or more of the top parameters a j is a nonpositive integer. … See §16.5 for the definition of F q p ( 𝐚 ; 𝐛 ; z ) as a contour integral when p > q + 1 and none of the a k is a nonpositive integer. … When p q + 1 and z is fixed and not a branch point, any branch of 𝐅 q p ( 𝐚 ; 𝐛 ; z ) is an entire function of each of the parameters a 1 , , a p , b 1 , , b q .