Using the density functional theory (DFT) method, the geometrical structures of In mXn\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{m}X_{n}$\end{document} (X= Se \documentclass[12pt]{minimal}
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\begin{document}$ X={\rm Se}$\end{document}, Te; m+n=5\documentclass[12pt]{minimal}
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\begin{document}$ m+n=5$\end{document} clusters are optimized, and their relative stability as well as electronic, magnetic and spectral properties are calculated. The ground state structures of In mXn\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{m}X_{n}$\end{document} clusters are found to be largely similar for X= Se \documentclass[12pt]{minimal}
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\begin{document}$ X={\rm Se}$\end{document} and Te, with the exception of In 2X3\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{2}X_{3}$\end{document} . The energy gap exhibits the maximum for In 2 Se 3\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{2}{\rm Se}_{3}$\end{document} or In 3 Te 2\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{3}{\rm Te}_{2}$\end{document} . The electronic properties of In mXn\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{m}X_{n}$\end{document} clusters depend on their geometrical structures and, hence, on the value of m ; and In 2 Se 3\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{2}{\rm Se}_{3}$\end{document} shows a low vertical electron affinity (VEA) of about 1.60eV and a high vertical ionization potential (VIP) of about 9.33eV. The total magnetic moment is 1 or 0μ_B for the clusters with m= odd \documentclass[12pt]{minimal}
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\begin{document}$ m={\rm odd}$\end{document} (1, 3) or even (2, 4) , respectively. The local magnetic moments of X atoms amount to about 99.9% of the total magnetic moment, while those of In atoms are merely 0.1%. The IR and Raman spectra of In mXn\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{m}X_{n}$\end{document} clusters exhibit similarity for X= Se \documentclass[12pt]{minimal}
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\begin{document}$ X={\rm Se}$\end{document} and Te with an exception of In 2X3\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{2}X_{3}$\end{document}. The energies of the strongest peaks of In m Te n\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{m}{\rm Te}_{n}$\end{document} are largely smaller than the corresponding In m Se n\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{m}{\rm Se}_{n}$\end{document} in both IR and Raman spectra. For UV-Vis spectra, the absorption peaks at 200-400nm for all clusters and 390–780 nm for m = 1 and 3 (except In 3 Te 2\documentclass[12pt]{minimal}
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\begin{document}$ {\rm In}_{3}{\rm Te}_{2}$\end{document} are likely to hint useful properties of UV and visible light absorption, respectively.
