Abstract
The search for new functional materials with tunable properties remains a central challenge in chemistry, particularly for applications in energy and electronics. In this work, we present a framework for predictive crystal design in alkali metal chalcogenides that enables controlled dimensional reduction of a parent covalent motif, yielding a broad range of electronic structures, which systematically evolve from one parent to the other. We present 11 new members of the AnCu4–nSnS4family (A = alkali metal; n = 0–4), which reduce the three-dimensional (3D) covalent network of Cu4SnS4into various 3D, 2D, 1D, and 0D [Cu4–nSnS4]n−motifs through the substitution of Cu with alkali metals of various radii. The end members of the family set the range in achievable band gaps at 0.99 eV for fully covalent Cu4SnS4(n = 0) and 3.38 eV for K4SnS4(n = 4) with 0D [SnS4]n−tetrahedra. As the dimensionality of [Cu4–nSnS4]n−systematically reduces within AnCu4–nSnS4(n = 1–3), a stepwise increase in band gap energy occurs through a gradual decrease in the energy of the valence band maximum and an increase in the conduction band minimum, with an increase in the effective masses of charge carriers. Furthermore, irrespective of the alkali metal, the thermal stability decreases with decreasing [Cu4–nSnS4]n−dimensionality within the quaternary members. Most importantly, we demonstrate that predictable crystal structure and property evolution for a given composition space is possible by deriving a general formula based on substituting the covalent metals of a parent structure with alkali metals.
| Original language | English |
|---|---|
| Pages (from-to) | 29994-30008 |
| Number of pages | 15 |
| Journal | Journal of the American Chemical Society |
| Volume | 147 |
| Issue number | 33 |
| DOIs | |
| State | Published - Aug 20 2025 |
Funding
This work was made possible through the financial support of the National Science Foundation (DMR-2305731). This work made use of the IMSERC X-ray and Crystallography Facility at Northwestern University and the EPIC facility of Northwestern University’s NUANCE Center, which has received support from the SHyNE Resource (NSF ECCS-1542205 and NSF ECCS-2025633), the INN, Northwestern’s MRSEC program (NSF DMR-2308691), and Northwestern University. Purchase of the Ag-microsource diffractometer used to obtain results included in this publication was supported by the Major Research Instrumentation Program from the National Science Foundation under the award CHE-1920248. DFT calculations in this work were supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences under grant DE-SC0024256. Z.L. and C.W. acknowledge the computational resources of the National Energy Research Scientific Computing Center (NERSC) under award BES-ERCAP0027615.
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