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Mathieu equation

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21: 28.14 Fourier Series
28.14.4 q c 2 m + 2 ( a ( ν + 2 m ) 2 ) c 2 m + q c 2 m 2 = 0 , a = λ ν ( q ) , c 2 m = c 2 m ν ( q ) ,
22: 28.29 Definitions and Basic Properties
A generalization of Mathieu’s equation (28.2.1) is Hill’s equation
28.29.1 w ′′ ( z ) + ( λ + Q ( z ) ) w = 0 ,
28.29.11 w ( z + π ) = ( 1 ) ν w ( z ) + c P ( z ) ,
28.29.13 w ( z + π ) + w ( z π ) = 2 cos ( π ν ) w ( z ) .
23: 28.32 Mathematical Applications
The separated solutions V ( ξ , η ) = v ( ξ ) w ( η ) can be obtained from the modified Mathieu’s equation (28.20.1) for v and from Mathieu’s equation (28.2.1) for w , where a is the separation constant and q = 1 4 c 2 k 2 . … This leads to integral equations and an integral relation between the solutions of Mathieu’s equation (setting ζ = i ξ , z = η in (28.32.3)). … Let u ( ζ ) be a solution of Mathieu’s equation (28.2.1) and K ( z , ζ ) be a solution of …defines a solution of Mathieu’s equation, provided that (in the case of an improper curve) the integral converges with respect to z uniformly on compact subsets of . …
24: 28.22 Connection Formulas
§28.22 Connection Formulas
The joining factors in the above formulas are given by …
28.22.13 M ν ( 1 ) ( z , h ) = M ν ( 1 ) ( 0 , h ) me ν ( 0 , h 2 ) Me ν ( z , h 2 ) .
Here me ν ( 0 , h 2 ) ( 0 ) is given by (28.14.1) with z = 0 , and M ν ( 1 ) ( 0 , h ) is given by (28.24.1) with j = 1 , z = 0 , and n chosen so that | c 2 n ν ( h 2 ) | = max ( | c 2 ν ( h 2 ) | ) , where the maximum is taken over all integers . …
25: 28.35 Tables
§28.35 Tables
  • Blanch and Clemm (1969) includes eigenvalues a n ( q ) , b n ( q ) for q = ρ e i ϕ , ρ = 0 ( .5 ) 25 , ϕ = 5 ( 5 ) 90 , n = 0 ( 1 ) 15 ; 4D. Also a n ( q ) and b n ( q ) for q = i ρ , ρ = 0 ( .5 ) 100 , n = 0 ( 2 ) 14 and n = 2 ( 2 ) 16 , respectively; 8D. Double points for n = 0 ( 1 ) 15 ; 8D. Graphs are included.

  • 26: Simon Ruijsenaars
    27: 28.31 Equations of Whittaker–Hill and Ince
    28.31.3 w ′′ + ξ sin ( 2 z ) w + ( η p ξ cos ( 2 z ) ) w = 0 .
    28.31.4 w e , s ( z ) = = 0 A 2 + s cos ( 2 + s ) z , s = 0 , 1 ,
    28.31.5 w o , s ( z ) = = 0 B 2 + s sin ( 2 + s ) z , s = 1 , 2 ,
    28.31.18 w ′′ + ( η 1 8 ξ 2 ( p + 1 ) ξ cos ( 2 z ) + 1 8 ξ 2 cos ( 4 z ) ) w = 0 ,
    28: 28.28 Integrals, Integral Representations, and Integral Equations
    §28.28(i) Equations with Elementary Kernels
    28.28.2 1 2 π 0 2 π e 2 i h w ce n ( t , h 2 ) d t = i n ce n ( α , h 2 ) Mc n ( 1 ) ( z , h ) ,
    28.28.16 0 sin ( 2 h cos y cosh t ) Ce 2 n ( t , h 2 ) d t = π A 0 2 n ( h 2 ) 2 ce 2 n ( 1 2 π , h 2 ) ( ce 2 n ( y , h 2 ) 2 π C 2 n ( h 2 ) fe 2 n ( y , h 2 ) ) ,
    29: Bibliography L
  • R. E. Langer (1934) The solutions of the Mathieu equation with a complex variable and at least one parameter large. Trans. Amer. Math. Soc. 36 (3), pp. 637–695.
  • W. R. Leeb (1979) Algorithm 537: Characteristic values of Mathieu’s differential equation. ACM Trans. Math. Software 5 (1), pp. 112–117.
  • 30: Gerhard Wolf