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31: 3.6 Linear Difference Equations
§3.6 Linear Difference Equations
§3.6(ii) Homogeneous Equations
§3.6(iv) Inhomogeneous Equations
The difference equation … …
32: 10.73 Physical Applications
This equation governs problems in acoustic and electromagnetic wave propagation. … …
§10.73(ii) Spherical Bessel Functions
33: 32.5 Integral Equations
§32.5 Integral Equations
34: 28.29 Definitions and Basic Properties
§28.29(i) Hill’s Equation
A generalization of Mathieu’s equation (28.2.1) is Hill’s equation
35: 28.30 Expansions in Series of Eigenfunctions
§28.30 Expansions in Series of Eigenfunctions
§28.30(i) Real Variable
28.30.1 w m ′′ + ( λ ^ m + Q ( x ) ) w m = 0 ,
28.30.3 f ( x ) = m = 0 f m w m ( x ) ,
28.30.4 f m = 1 2 π 0 2 π f ( x ) w m ( x ) d x .
36: 32.17 Methods of Computation
The Painlevé equations can be integrated by Runge–Kutta methods for ordinary differential equations; see §3.7(v), Hairer et al. (2000), and Butcher (2003). …
37: 9.15 Mathematical Applications
Airy functions play an indispensable role in the construction of uniform asymptotic expansions for contour integrals with coalescing saddle points, and for solutions of linear second-order ordinary differential equations with a simple turning point. …
38: 10.72 Mathematical Applications
§10.72(i) Differential Equations with Turning Points
The canonical form of differential equation for these problems is given by …
§10.72(ii) Differential Equations with Poles
§10.72(iii) Differential Equations with a Double Pole and a Movable Turning Point
39: 29.9 Stability
§29.9 Stability
The Lamé equation (29.2.1) with specified values of k , h , ν is called stable if all of its solutions are bounded on ; otherwise the equation is called unstable. …
40: 32.1 Special Notation
The functions treated in this chapter are the solutions of the Painlevé equations P I P VI .