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A Conductive Heterometallic Coordination Polymer Hosting a Quasi-1D S = 1/2 Antiferromagnetic Chain.
PubMed
Authors: Jin Y, Wu S, Matsushita MM, Zhang Z, Xu W, Zhong YW, Awaga K
Year
2026
Paper ID
67687
Status
Peer-reviewed
Abstract Read
~2 min
Abstract Words
184
Citations
N/A
Abstract
Conductive coordination polymers (CPs) offer a chemically tunable platform for exploring correlated electronic states. However, integrating a well-defined quantum spin chain into such conductive systems remains a fundamental challenge, as the electronic delocalization needed for conductivity often disrupts low-dimensional spin topology. Here, we demonstrate that the heterometallic framework AgCuBHT BHT = benzenehexathiol concurrently hosts a nearly ideal = 1/2 antiferromagnetic spin chain and exhibits high electrical conductivity. Crystalline films of AgCuBHT exhibit a conductivity of 17 S cm at 300 K, with its intrinsic metallic nature confirmed by ultraviolet photoelectron spectroscopy and band-structure calculations. Magnetic susceptibility measurements on AgCuBHT reveal a broad maximum, characteristic of spin-1/2 antiferromagnetic chain behavior. Analysis using the Bonner-Fisher model yields a strong intrachain exchange coupling of / = 294 K. The absence of long-range magnetic order, along with weak interchain interactions, establishes AgCuBHT as a nearly ideal quasi-1D antiferromagnet. First-principles calculations uncover an orbital-selective mechanism enabling the coexistence of itinerant electrons and localized spins. This work identifies AgCuBHT as a pioneering conductive CP hosting a quasi-1D quantum spin-lattice, opening new avenues for the concurrent design of spin topology and electronic transport in molecular quantum materials.
Why This Paper Matters
- This paper contributes to the Quantum Chemistry research area in the Quantum Articles archive.
- It adds a 2026 reference point for readers tracking recent quantum research.
- Conductive coordination polymers (CPs) offer a chemically tunable platform for exploring correlated electronic states.
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