The PHENIX Collaboration has measured the ratio of the yields of $psi(2S)$ to $psi(1S)$ mesons produced in $p$$+$$p$, $p$$+$Al, $p$$+$Au, and $^{3}$He$+$Au collisions at $sqrt{s_{_{NN}}}=200$ GeV over the forward and backward rapidity intervals $1.2<|y|<2.2$. We find that the ratio in $p$$+$$p$ collisions is consistent with measurements at other collision energies. In collisions with nuclei, we find that in the forward ($p$-going or $^{3}$He-going) direction, the relative yield of $psi(2S)$ mesons to $psi(1S)$ mesons is consistent with the value measured in pp collisions. However, in the backward (nucleus-going) direction, the $psi(2S)$ is preferentially suppressed by a factor of $sim$2. This suppression is attributed in some models to breakup of the weakly-bound $psi(2S)$ through final state interactions with comoving particles, which have a higher density in the nucleus-going direction. These breakup effects may compete with color screening in a deconfined quark-gluon plasma to produce sequential suppression of excited quarkonia states.
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