Chasing the spin gap through the phase diagram of a frustrated Mott insulator

Abstract

The quest for entangled spin excitations has stimulated intense research on frustrated magnetic systems. For almost two decades, the triangular-lattice Mott insulator -(BEDT-TTF)2Cu2(CN)3 has been the hottest candidate for a gapless quantum spin liquid with itinerant spinons. Very recently, however, this scenario was overturned as electron-spin-resonance (ESR) studies unveiled a spin gap, calling for reevaluation of the magnetic ground state. Here we achieve a precise mapping of this spin-gapped phase through the Mott transition by ultrahigh-resolution strain tuning. Our transport experiments reveal a reentrance of charge localization below T=6 K associated with a gap size of 30-50 K. The negative slope of the insulator-metal boundary, dT/dp<0, evidences the low-entropy nature of the spin-singlet ground state. By tuning the enigmatic '6 K anomaly' through the phase diagram of -(BEDT-TTF)2Cu2(CN)3, we identify it as the transition to a valence-bond-solid phase, with typical magnetic and structural fingerprints, that persists at T→ 0 until unconventional superconductivity and metallic transport proliferate.

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