Dissipation splits the 1D Mott transition into two distinct critical points via an intermediate compressible gapless dissipative phase with zero superfluid stiffness.
On a more quantitative level, we consider the observableO(X) =|X(ω 1 = 2π/β)| 2 which we expect to decorrelate very slowly as it cap- tures the large-scale physics
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Dissipation splits the Mott transition in one dimension
Dissipation splits the 1D Mott transition into two distinct critical points via an intermediate compressible gapless dissipative phase with zero superfluid stiffness.