Divide the second-order difference equation by and set . The first quotient is a central finite difference approximation to ; the quotient approximates . Their Taylor series errors are for a sufficiently smooth function. This is therefore a finite difference method for the second-order linear differential equation in part (a).
At a fixed , take with integral. Since , the exact bounded discrete solution satisfies
Likewise . The decay selected by boundedness in the linear recurrence relation becomes exactly the decay selected by boundedness in the ordinary differential equation.

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