  A typical result of the paper is the following. Let $H_\gamma=H_0 +\gamma V$
where $H_0$ is multiplication by $|x|^{2l}$ and $V$ is an integral operator
with kernel $\cos< x,y\rang le$ in the space $L_2(R^d)$. If $l=d/2+ 2k$ for
some $k= 0,1,...$, then the operator $H_\gamma$ has infinite number of negative
eigenvalues for any coupling constant $\gamma\neq 0$. For other values of $l$,
the negative spectrum of $H_\gamma$ is infinite for $|\gamma|> \sigma_l$ where
$\sigma_l$ is some explicit positive constant. In the case $\pm \gamma\in
(0,\sigma_l]$, the number $N^{(\pm)}_l$ of negative eigenvalues of $H_\gamma$
is finite and does not depend on $\gamma$. We calculate $N^{(\pm)}_l$.
