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Deconfined quantum critical point in a dissipative spin-1/2 chain

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abstract

Open quantum spin systems offer a previously unexplored route to realizing deconfined quantum criticality. We consider a spin-1/2 $J$-$Q_3$ chain, consisting of an antiferromagnetic (AFM) Heisenberg exchange and a competing multi-spin interaction favoring a valence-bond solid (VBS) state, with each spin component coupled to a bosonic bath. Using non-Abelian bosonization and renormalization-group (RG) analysis, combined with large-scale quantum Monte Carlo (QMC) simulations, we determine the phase diagram and the associated phase transitions of the model. We show that strong dissipation stabilizes an AFM phase for sub-Ohmic, Ohmic, and super-Ohmic baths. Continuous AFM-VBS transitions at finite dissipation are found upon increasing the multi-spin interaction in both the sub-Ohmic and Ohmic regimes. Critical properties are obtained through perturbative RG analysis and QMC simulations. In the Ohmic case, the critical point features spinon deconfinement and emergent O(4) symmetry. In the sub-Ohmic regime, the transition may also involve spinon deconfinement, provided that spinons remain deconfined in the dissipative VBS phase. In addition, in the super-Ohmic regime, we propose a transition from AFM phase to a quasi-long-range ordered phase.

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representative citing papers

Dissipation-induced bulk and boundary criticality in the Haldane chain

cond-mat.str-el · 2026-08-06 · conditional · novelty 8.0

Dissipation drives the Haldane chain to a nonconformal critical point where its protected edge states exhibit a boundary critical exponent distinct from the trivial chain and from the dissipative O(3) epsilon expansion.

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  • Dissipation-induced bulk and boundary criticality in the Haldane chain cond-mat.str-el · 2026-08-06 · conditional · none · ref 16 · internal anchor

    Dissipation drives the Haldane chain to a nonconformal critical point where its protected edge states exhibit a boundary critical exponent distinct from the trivial chain and from the dissipative O(3) epsilon expansion.