  In this article, we study a second-order expansion for the effect induced on
a large quantum particle which undergoes a single scattering with a low-mass
particle via a repulsive point interaction. We give an approximation with
third-order error in $\lambda$ to the map $G\to \Tr_{2}[(I\otimes
\rho)S_{\lambda}^{*}(G\otimes I)S_{\lambda}]$, where $G\in \Bi(L^{2}(\R^{n}))$
is a heavy-particle observable, $\rho\in \Bi_{1}(\R^{n})$ is the density matrix
corresponding to the state of the light particle, $\lambda=\frac{m}{M}$ is the
mass ratio of the light particle to the heavy particle, $S_{\lambda}\in
\Bi(L^{2}(\R^{n})\otimes L^{2}(\R^{n}))$ is the scattering matrix between the
two particles due to a repulsive point interaction, and the trace is over the
light-particle Hilbert space. The third-order error is bounded in operator norm
for dimensions one and three using a weighted operator norm on $G$.
