  When a quantum-chaotic normal conductor is coupled to a superconductor,
random-matrix theory predicts that a gap opens up in the excitation spectrum
which is of universal size $E_g^{\rm RMT}\approx 0.3 \hbar/t_D$, where $t_D$ is
the mean scattering time between Andreev reflections. We show that a scarred
state of long lifetime $t_S\gg t_D$ suppresses the excitation gap over a window
$\Delta E\approx 2 E_g^{\rm RMT}$ which can be much larger than the narrow
resonance width $\Gamma_S=\hbar/t_S$ of the scar in the normal system. The
minimal value of the excitation gap within this window is given by
$\Gamma_S/2\ll E_g^{\rm RMT}$. Hence the scarred state can be detected over a
much larger energy range than it is the case when the superconducting terminal
is replaced by a normal one.
