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11: 28.30 Expansions in Series of Eigenfunctions
§28.30(i) Real Variable
Let λ ^ m , m = 0 , 1 , 2 , , be the set of characteristic values (28.29.16) and (28.29.17), arranged in their natural order (see (28.29.18)), and let w m ( x ) , m = 0 , 1 , 2 , , be the eigenfunctions, that is, an orthonormal set of 2 π -periodic solutions; thus
28.30.1 w m ′′ + ( λ ^ m + Q ( x ) ) w m = 0 ,
Then every continuous 2 π -periodic function f ( x ) whose second derivative is square-integrable over the interval [ 0 , 2 π ] can be expanded in a uniformly and absolutely convergent series
28.30.3 f ( x ) = m = 0 f m w m ( x ) ,
12: 1.8 Fourier Series
Formally, if f ( x ) is a real- or complex-valued 2 π -periodic function, …
13: 23.2 Definitions and Periodic Properties
Hence ( z ) is an elliptic function, that is, ( z ) is meromorphic and periodic on a lattice; equivalently, ( z ) is meromorphic and has two periods whose ratio is not real. …
14: 28.29 Definitions and Basic Properties
π is the minimum period of Q . … where the function P ν ( z ) is π -periodic. … The solutions of period π or 2 π are exceptional in the following sense. If (28.29.1) has a periodic solution with minimum period n π , n = 3 , 4 , , then all solutions are periodic with period n π . …
15: 4.2 Definitions
The real and imaginary parts of ln z are given by …
§4.2(iii) The Exponential Function
The function exp is an entire function of z , with no real or complex zeros. It has period 2 π i : … When a is real
16: 25.16 Mathematical Applications
25.16.6 H ( s ) = ζ ( s ) + γ ζ ( s ) + 1 2 ζ ( s + 1 ) + r = 1 k ζ ( 1 2 r ) ζ ( s + 2 r ) + n = 1 1 n s n B ~ 2 k + 1 ( x ) x 2 k + 2 d x ,
25.16.7 H ( s ) = 1 2 ζ ( s + 1 ) + ζ ( s ) s 1 r = 1 k ( s + 2 r 2 2 r 1 ) ζ ( 1 2 r ) ζ ( s + 2 r ) ( s + 2 k 2 k + 1 ) n = 1 1 n n B ~ 2 k + 1 ( x ) x s + 2 k + 1 d x .
17: 22.3 Graphics
§22.3(i) Real Variables: Line Graphs
§22.3(ii) Real Variables: Surfaces
sn ( x , k ) , cn ( x , k ) , and dn ( x , k ) as functions of real arguments x and k . The period diverges logarithmically as k 1 ; see §19.12. …
§22.3(iii) Complex z ; Real k
18: 28.5 Second Solutions fe n , ge n
As a consequence of the factor z on the right-hand sides of (28.5.1), (28.5.2), all solutions of Mathieu’s equation that are linearly independent of the periodic solutions are unbounded as z ± on . …
19: 28.11 Expansions in Series of Mathieu Functions
Let f ( z ) be a 2 π -periodic function that is analytic in an open doubly-infinite strip S that contains the real axis, and q be a normal value (§28.7). …
20: 32.10 Special Function Solutions
32.10.34 w ( z ; 0 , 0 , 0 , 1 2 ) = Λ ( C 1 ϕ 1 + C 2 ϕ 2 , z ) ,