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11: 23.15 Definitions
§23.15 Definitions
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. …
12: 28.12 Definitions and Basic Properties
§28.12(ii) Eigenfunctions me ν ( z , q )
However, these functions are not the limiting values of me ± ν ( z , q ) as ν n ( 0 ) . … Again, the limiting values of ce ν ( z , q ) and se ν ( z , q ) as ν n ( 0 ) are not the functions ce n ( z , q ) and se n ( z , q ) defined in §28.2(vi). …
13: 14.19 Toroidal (or Ring) Functions
§14.19 Toroidal (or Ring) Functions
§14.19(i) Introduction
This form of the differential equation arises when Laplace’s equation is transformed into toroidal coordinates ( η , θ , ϕ ) , which are related to Cartesian coordinates ( x , y , z ) by …
§14.19(iv) Sums
§14.19(v) Whipple’s Formula for Toroidal Functions
14: 26.9 Integer Partitions: Restricted Number and Part Size
p k ( n ) denotes the number of partitions of n into at most k parts. … … Equations (26.9.2)–(26.9.3) are examples of closed forms that can be computed explicitly for any positive integer k . …
§26.9(ii) Generating Functions
§26.9(iv) Limiting Form
15: 14.20 Conical (or Mehler) Functions
(14.2.2) takes the form … …
§14.20(v) Trigonometric Expansion
From (14.20.9) or (14.20.10) it is evident that 𝖯 1 2 + i τ ( cos θ ) is positive for real θ . … where the inverse trigonometric functions take their principal values. …
16: 6.16 Mathematical Applications
These limits are not approached uniformly, however. The first maximum of 1 2 Si ( x ) for positive x occurs at x = π and equals ( 1.1789 ) × 1 4 π ; compare Figure 6.3.2. Hence if x = π / ( 2 n ) and n , then the limiting value of S n ( x ) overshoots 1 4 π by approximately 18%. Similarly if x = π / n , then the limiting value of S n ( x ) undershoots 1 4 π by approximately 10%, and so on. …
17: 5.12 Beta Function
§5.12 Beta Function
Euler’s Beta Integral
5.12.2 0 π / 2 sin 2 a 1 θ cos 2 b 1 θ d θ = 1 2 B ( a , b ) .
5.12.5 0 π / 2 ( cos t ) a 1 cos ( b t ) d t = π 2 a 1 a B ( 1 2 ( a + b + 1 ) , 1 2 ( a b + 1 ) ) , a > 0 .
Pochhammer’s Integral
18: 20.2 Definitions and Periodic Properties
§20.2(i) Fourier Series
§20.2(ii) Periodicity and Quasi-Periodicity
For fixed z , each of θ 1 ( z | τ ) / sin z , θ 2 ( z | τ ) / cos z , θ 3 ( z | τ ) , and θ 4 ( z | τ ) is an analytic function of τ for τ > 0 , with a natural boundary τ = 0 , and correspondingly, an analytic function of q for | q | < 1 with a natural boundary | q | = 1 . … The theta functions are quasi-periodic on the lattice: …
§20.2(iv) z -Zeros
19: 5.15 Polygamma Functions
§5.15 Polygamma Functions
The functions ψ ( n ) ( z ) , n = 1 , 2 , , are called the polygamma functions. In particular, ψ ( z ) is the trigamma function; ψ ′′ , ψ ( 3 ) , ψ ( 4 ) are the tetra-, penta-, and hexagamma functions respectively. Most properties of these functions follow straightforwardly by differentiation of properties of the psi function. … For B 2 k see §24.2(i). …
20: 9.12 Scorer Functions
§9.12 Scorer Functions
where …
§9.12(ii) Graphs
Functions and Derivatives