Let E = F(v) be the ground-state eigenvalue of the Schrodinger Hamiltonian
H = - Delta + vf(x), where the potential shape f(x) is symmetric and monoto
ne increasing for x > 0, and the coupling parameter v is positive. if the k
inetic potential (f) over bar(s) associated with f(x) is defined by the tra
nsformation (f) over bar(s)= F(v), s = F(v)- vF'(v), then f can be reconstr
ucted from F by the sequence f([n+1]) = (f) over bar . (f) over bar([n]-1)
. f([n]) Convergence is proved for special classes of potential shape; for
other test cases it is demonstrated numerically. The seed potential shape f
([0]) need not be 'close' to the limit f. (C) 2000 Published by Elsevier Sc
ience B.V. All rights reserved.