We present a new approach (distinct from Gel'fand-Levitan) to the theorem o
f Borg-Marchenko that the m-function (equivalently, spectral measure) for a
finite interval or half-line Schrodinger operator determines the potential
. Our approach is an analog of the continued fraction approach for the mome
nt problem. We prove there is a representation for the m-function m(-kappa(
2)) = -kappa - integral(0)(b) A(alpha)e(-2 alpha kappa) d alpha + O(e(-(2b-
epsilon)kappa)). A on [0,a] is a function of q on [0, a] and vice-versa. A
key role is played by a differential equation that A Obeys after allowing x
-dependence:
delta A/delta x = delta A/delta alpha + integral(0)(alpha) A(beta, x)A(alph
a - beta, x) d beta.
Among our new results are necessary and sufficient conditions on the m-func
tions for potentials q(1) and q(2) for q(1) to equal q(2) on [0, a].