We suppose: (1) that the ground-state eigenvalue E = F(upsilon) of the Schr
odinger Hamiltonian H = -Delta + upsilon f(x) in one dimension is known for
all values of the coupling upsilon > 0; and (2) that the potential shape c
an be expressed in the form f(x) = g(x(2)), where g is monotone increasing
and convex. The inversion inequality f(x) less than or equal to f (1/4x(2))
is established, in which the "kinetic potential'' (f) over bar(s) is relat
ed to the energy function F(upsilon) by the transformation {(f) over bar(s)
= F' (upsilon), s = F(upsilon) - upsilon F'(upsilon)}. As an example, f is
approximately reconstructed from the energy function F for the potential f
(x) = ax(2) + b/(c + x(2)). (C) 1999 American Institute of Physics. [S0022-
2488(99)01705-3].