\begin{document}$K^*(892)^+$\end{document} mesons in \begin{document}${\pi^-}A$\end{document} reactions at near-threshold laboratory incident pion momenta of 1.4–2.0 GeV/c via a nuclear spectral function approach. The approach accounts for incoherent primary \begin{document}$\pi^-$\end{document} meson–proton \begin{document}${\pi^-}p \to {K^*(892)^+}\Sigma^-$\end{document} production processes as well as the influence of the scalar \begin{document}$K^*(892)^+$\end{document}–nucleus potential (or the \begin{document}$K^*(892)^+$\end{document} in-medium mass shift) on these processes. We calculate the absolute differential and total cross sections for the production of \begin{document}$K^*(892)^+$\end{document} mesons from carbon and tungsten nuclei at laboratory angles of 0\begin{document}$^{\circ}$\end{document}–45\begin{document}$^{\circ}$\end{document} and at the aforementioned momenta in five scenarios for the aforenoted shift. We show that the \begin{document}$K^*(892)^+$\end{document} momentum distributions and their excitation functions (absolute and relative) possess a high sensitivity to changes in the in-medium \begin{document}$K^*(892)^+$\end{document}mass shift in the low-momentum region of 0.1–0.6 GeV/c. Therefore, the measurement of such observables in a dedicated experiment at the GSI pion beam facility in the near-threshold momentum domain will allow us to get valuable information on the \begin{document}$K^*(892)^+$\end{document} in-medium properties."> Near-threshold <i>K</i><sup>*</sup>(892)<sup>+</sup> meson production in the interaction of π<sup>−</sup> mesons with nuclei -
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