Interacting quantum criticality with U(1) symmetry breaking in 1+1 dimensions
cond-mat.str-el, cond-mat.stat-mech, quant-ph
Submitted: 2026-10-05
Updated: 2026-10-05
Comments: 15 pages, 6 figures, 3 tables
License: http://creativecommons.org/licenses/by/4.0/
The gist: The Hohenberg-Mermin-Wagner theorem motivates the expectation that continuous symmetries remain unbroken in one-dimensional quantum ground states.
Terminology
Abstract
The Hohenberg-Mermin-Wagner theorem motivates the expectation that continuous symmetries remain unbroken in one-dimensional quantum ground states. Here, contrary to this expectation, we demonstrate the spontaneous breaking of U(1) spin-rotation symmetry and the emergence of an interacting quantum critical point in lattice spin- 1/2 and spin- 1 chains. Using subsystem Binder scaling, we locate the critical point and determine the correlation-length critical exponent as ν= 0.60 plus or minus 0.02, distinct from the Gaussian value 0.5 but consistent with the perturbative renormalization-group prediction. We further analyze the finite-size scaling of the lowest neutral excitation gap and obtain the dynamical critical exponent z=1.986 plus or minus 0.005. The result z < 2 is incompatible with microscopic realizations of this critical theory by frustration-free models, implying a mechanism for continuous symmetry breaking in one-dimensional quantum ground states distinct from frustration freeness.
Sources
- Temporal Berry Phase and the Emergence of Bose-Glass-Analog Phase in a Clean U(1) Superfluid
- Continuous symmetry breaking in 1D spin chains and 1+1D field theory
- Criticality enabled long-range order in a U(1)-symmetric spin-1 Heisenberg chain with biquadratic interactions
- Theory of criticality-enabled U(1) symmetry breaking in a class of 1+1D systems
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