Recently A. G. Ramm (1999) has shown that a subset of phase shifts
δ
l
\delta _l
,
l
=
0
,
1
,
…
l=0,1,\ldots
, determines the potential if the indices of the known shifts satisfy the Müntz condition
∑
l
≠
0
,
l
∈
L
1
l
=
∞
\sum _{l\neq 0,l\in L}\frac {1}{l}=\infty
. We prove the necessity of this condition in some classes of potentials. The problem is reduced to an inverse eigenvalue problem for the half-line Schrödinger operators.