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Jacobi function

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31: 20.10 Integrals
20.10.1 0 x s 1 θ 2 ( 0 | i x 2 ) d x = 2 s ( 1 2 s ) π s / 2 Γ ( 1 2 s ) ζ ( s ) , s > 1 ,
20.10.2 0 x s 1 ( θ 3 ( 0 | i x 2 ) 1 ) d x = π s / 2 Γ ( 1 2 s ) ζ ( s ) , s > 1 ,
20.10.3 0 x s 1 ( 1 θ 4 ( 0 | i x 2 ) ) d x = ( 1 2 1 s ) π s / 2 Γ ( 1 2 s ) ζ ( s ) , s > 0 .
20.10.4 0 e s t θ 1 ( β π 2 | i π t 2 ) d t = 0 e s t θ 2 ( ( 1 + β ) π 2 | i π t 2 ) d t = s sinh ( β s ) sech ( s ) ,
20.10.5 0 e s t θ 3 ( ( 1 + β ) π 2 | i π t 2 ) d t = 0 e s t θ 4 ( β π 2 | i π t 2 ) d t = s cosh ( β s ) csch ( s ) .
32: 29.15 Fourier Series and Chebyshev Series
33: 20.13 Physical Applications
The functions θ j ( z | τ ) , j = 1 , 2 , 3 , 4 , provide periodic solutions of the partial differential equation …
20.13.4 π 4 α t n = e ( n π + z ) 2 / ( 4 α t ) = θ 3 ( z | i 4 α t / π ) ,
20.13.5 π 4 α t n = ( 1 ) n e ( n π + z ) 2 / ( 4 α t ) = θ 4 ( z | i 4 α t / π ) .
In the singular limit τ 0 + , the functions θ j ( z | τ ) , j = 1 , 2 , 3 , 4 , become integral kernels of Feynman path integrals (distribution-valued Green’s functions); see Schulman (1981, pp. 194–195). …
34: 20.15 Tables
20.15.1 sin α = θ 2 2 ( 0 , q ) / θ 3 2 ( 0 , q ) = k .
Tables of Neville’s theta functions θ s ( x , q ) , θ c ( x , q ) , θ d ( x , q ) , θ n ( x , q ) (see §20.1) and their logarithmic x -derivatives are given in Abramowitz and Stegun (1964, pp. 582–585) to 9D for ε , α = 0 ( 5 ) 90 , where (in radian measure) ε = x / θ 3 2 ( 0 , q ) = π x / ( 2 K ( k ) ) , and α is defined by (20.15.1). …
35: 20.9 Relations to Other Functions
20.9.1 k = θ 2 2 ( 0 | τ ) / θ 3 2 ( 0 | τ )
20.9.3 R F ( θ 2 2 ( z , q ) θ 2 2 ( 0 , q ) , θ 3 2 ( z , q ) θ 3 2 ( 0 , q ) , θ 4 2 ( z , q ) θ 4 2 ( 0 , q ) ) = θ 1 ( 0 , q ) θ 1 ( z , q ) z ,
20.9.4 R F ( 0 , θ 3 4 ( 0 , q ) , θ 4 4 ( 0 , q ) ) = 1 2 π ,
The relations (20.9.1) and (20.9.2) between k and τ (or q ) are solutions of Jacobi’s inversion problem; see Baker (1995) and Whittaker and Watson (1927, pp. 480–485). …
36: 29.8 Integral Equations
29.8.1 x = k 2 sn ( z , k ) sn ( z 1 , k ) sn ( z 2 , k ) sn ( z 3 , k ) k 2 k 2 cn ( z , k ) cn ( z 1 , k ) cn ( z 2 , k ) cn ( z 3 , k ) + 1 k 2 dn ( z , k ) dn ( z 1 , k ) dn ( z 2 , k ) dn ( z 3 , k ) ,
where z , z 1 , z 2 , z 3 are real, and sn , cn , dn are the Jacobian elliptic functions22.2). …
29.8.6 y = 1 k dn ( z , k ) dn ( z 1 , k ) .
29.8.7 𝐸𝑐 ν 2 m + 1 ( z 1 , k 2 ) w 2 ( K ) + w 2 ( K ) w 2 ( 0 ) = k 2 sn ( z 1 , k ) K K sn ( z , k ) d 𝖯 ν ( y ) d y 𝐸𝑐 ν 2 m + 1 ( z , k 2 ) d z ,
29.8.9 𝐸𝑠 ν 2 m + 2 ( z 1 , k 2 ) d w 2 ( z ) / d z | z = K d w 2 ( z ) / d z | z = K w 2 ( 0 ) = k 4 k sn ( z 1 , k ) cn ( z 1 , k ) K K sn ( z , k ) cn ( z , k ) d 2 𝖯 ν ( y ) d y 2 𝐸𝑠 ν 2 m + 2 ( z , k 2 ) d z .
37: 18.12 Generating Functions
Jacobi
18.12.2 𝐅 1 0 ( α + 1 ; ( x 1 ) z 2 ) 𝐅 1 0 ( β + 1 ; ( x + 1 ) z 2 ) = ( 1 2 ( 1 x ) z ) 1 2 α J α ( 2 ( 1 x ) z ) ( 1 2 ( 1 + x ) z ) 1 2 β I β ( 2 ( 1 + x ) z ) = n = 0 P n ( α , β ) ( x ) Γ ( n + α + 1 ) Γ ( n + β + 1 ) z n ,
18.12.2_5 F 1 2 ( γ , α + β + 1 γ α + 1 ; 1 R z 2 ) F 1 2 ( γ , α + β + 1 γ β + 1 ; 1 R + z 2 ) = n = 0 ( γ ) n ( α + β + 1 γ ) n ( α + 1 ) n ( β + 1 ) n P n ( α , β ) ( x ) z n , R = 1 2 x z + z 2 , | z | < 1 ,
18.12.3 ( 1 + z ) α β 1 F 1 2 ( 1 2 ( α + β + 1 ) , 1 2 ( α + β + 2 ) β + 1 ; 2 ( x + 1 ) z ( 1 + z ) 2 ) = n = 0 ( α + β + 1 ) n ( β + 1 ) n P n ( α , β ) ( x ) z n , | z | < 1 ,
38: 18.38 Mathematical Applications
The Askey–Gasper inequality
18.38.3 m = 0 n P m ( α , 0 ) ( x ) = ( α + 2 ) n n ! F 2 3 ( n , n + α + 2 , 1 2 ( α + 1 ) α + 1 , 1 2 ( α + 3 ) ; 1 2 ( 1 x ) ) 0 , x 1 , α 2 , n = 0 , 1 , ,
also the case β = 0 of (18.14.26), was used in de Branges’ proof of the long-standing Bieberbach conjecture concerning univalent functions on the unit disk in the complex plane. …
39: 18.10 Integral Representations
18.10.1 P n ( α , α ) ( cos θ ) P n ( α , α ) ( 1 ) = C n ( α + 1 2 ) ( cos θ ) C n ( α + 1 2 ) ( 1 ) = 2 α + 1 2 Γ ( α + 1 ) π 1 2 Γ ( α + 1 2 ) ( sin θ ) 2 α 0 θ cos ( ( n + α + 1 2 ) ϕ ) ( cos ϕ cos θ ) α + 1 2 d ϕ , 0 < θ < π , α > 1 2 .
18.10.3 P n ( α , β ) ( cos θ ) P n ( α , β ) ( 1 ) = 2 Γ ( α + 1 ) π 1 2 Γ ( α β ) Γ ( β + 1 2 ) 0 1 0 π ( ( cos 1 2 θ ) 2 r 2 ( sin 1 2 θ ) 2 + i r sin θ cos ϕ ) n ( 1 r 2 ) α β 1 r 2 β + 1 ( sin ϕ ) 2 β d ϕ d r , α > β > 1 2 .
18.10.4 P n ( α , α ) ( cos θ ) P n ( α , α ) ( 1 ) = C n ( α + 1 2 ) ( cos θ ) C n ( α + 1 2 ) ( 1 ) = Γ ( α + 1 ) π 1 2 Γ ( α + 1 2 ) 0 π ( cos θ + i sin θ cos ϕ ) n ( sin ϕ ) 2 α d ϕ , α > 1 2 .
40: 20.5 Infinite Products and Related Results
20.5.1 θ 1 ( z , q ) = 2 q 1 / 4 sin z n = 1 ( 1 q 2 n ) ( 1 2 q 2 n cos ( 2 z ) + q 4 n ) ,
20.5.2 θ 2 ( z , q ) = 2 q 1 / 4 cos z n = 1 ( 1 q 2 n ) ( 1 + 2 q 2 n cos ( 2 z ) + q 4 n ) ,
20.5.3 θ 3 ( z , q ) = n = 1 ( 1 q 2 n ) ( 1 + 2 q 2 n 1 cos ( 2 z ) + q 4 n 2 ) ,
20.5.4 θ 4 ( z , q ) = n = 1 ( 1 q 2 n ) ( 1 2 q 2 n 1 cos ( 2 z ) + q 4 n 2 ) .
Jacobi’s Triple Product