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11: 29.12 Definitions
With the substitution ξ = sn 2 ( z , k ) every Lamé polynomial in Table 29.12.1 can be written in the form
12: 20.14 Methods of Computation
The Fourier series of §20.2(i) usually converge rapidly because of the factors q ( n + 1 2 ) 2 or q n 2 , and provide a convenient way of calculating values of θ j ( z | τ ) . Similarly, their z -differentiated forms provide a convenient way of calculating the corresponding derivatives. For instance, the first three terms of (20.2.1) give the value of θ 1 ( 2 i | i ) ( = θ 1 ( 2 i , e π ) ) to 12 decimal places. … For instance, to find θ 3 ( z , 0.9 ) we use (20.7.32) with q = 0.9 = e i π τ , τ = i ln ( 0.9 ) / π . …Hence the first term of the series (20.2.3) for θ 3 ( z τ | τ ) suffices for most purposes. …
13: 3.10 Continued Fractions
A continued fraction of the form
Jacobi Fractions
A continued fraction of the form …is called a Jacobi fraction ( J -fraction). … can be written in the form
14: 29.15 Fourier Series and Chebyshev Series
Since (29.2.5) implies that cos ϕ = sn ( z , k ) , (29.15.1) can be rewritten in the form
15: 20.13 Physical Applications
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). …
16: 29.2 Differential Equations
§29.2(i) Lamé’s Equation
For sn ( z , k ) see §22.2. …
§29.2(ii) Other Forms
we have …
17: 22.8 Addition Theorems
§22.8(ii) Alternative Forms for Sum of Two Arguments
22.8.14 sn ( u + v ) = sn u cn u dn v + sn v cn v dn u cn u cn v + sn u dn u sn v dn v ,
22.8.15 cn ( u + v ) = sn u cn u dn v sn v cn v dn u sn u cn v dn v sn v cn u dn u ,
22.8.17 dn ( u + v ) = sn u cn v dn u sn v cn u dn v sn u cn v dn v sn v cn u dn u ,
22.8.23 | sn z 1 cn z 1 cn z 1 dn z 1 cn z 1 dn z 1 sn z 2 cn z 2 cn z 2 dn z 2 cn z 2 dn z 2 sn z 3 cn z 3 cn z 3 dn z 3 cn z 3 dn z 3 sn z 4 cn z 4 cn z 4 dn z 4 cn z 4 dn z 4 | = 0 .
18: 18.18 Sums
Jacobi
Jacobi
See (18.17.45) and (18.17.49) for integrated forms of (18.18.22) and (18.18.23), respectively. …
Jacobi
See also (18.38.3) for a finite sum of Jacobi polynomials. …
19: 18.15 Asymptotic Approximations
§18.15(i) Jacobi
For large β , fixed α , and 0 n / β c , Dunster (1999) gives asymptotic expansions of P n ( α , β ) ( z ) that are uniform in unbounded complex z -domains containing z = ± 1 . …This reference also supplies asymptotic expansions of P n ( α , β ) ( z ) for large n , fixed α , and 0 β / n c . … The first term of this expansion also appears in Szegő (1975, Theorem 8.21.7). … For asymptotic approximations of Jacobi, ultraspherical, and Laguerre polynomials in terms of Hermite polynomials, see López and Temme (1999a). …
20: 23.15 Definitions
In §§23.1523.19, k and k ( ) denote the Jacobi modulus and complementary modulus, respectively, and q = e i π τ ( τ > 0 ) denotes the nome; compare §§20.1 and 22.1. … The set of all bilinear transformations of this form is denoted by SL ( 2 , ) (Serre (1973, p. 77)). … If, as a function of q , f ( τ ) is analytic at q = 0 , then f ( τ ) is called a modular form. If, in addition, f ( τ ) 0 as q 0 , then f ( τ ) is called a cusp form. …