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Spontaneous breaking of multipole symmetries
Statistical Mechanics · Submitted 15 Nov 2021
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We derive generalized Mermin-Wagner arguments for the total or partial breaking of multipolar symmetry groups and generalized Imry-Ma arguments for the robustness of such multipolar symmetry breaking to disorder.
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The abstract, sentence by sentence
Multipole symmetries are of interest both as a window on fracton physics and as a crucial ingredient in realizing new universality classes for quantum dynamics. Here we address the question of whether and when multipole symmetries can be spontaneously broken, both in thermal equilibrium and at zero temperature. We derive generalized Mermin-Wagner arguments for the total or partial breaking of multipolar symmetry groups and generalized Imry-Ma arguments for the robustness of such multipolar symmetry breaking to disorder. We present both general results and explicit examples. Our results should be directly applicable to quantum dynamics with multipolar symmetries and also provide a useful stepping stone to understanding the robustness of fracton phases to thermal fluctuations, quantum fluctuations, and disorder.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Multipole symmetries are of interest both as a window on fracton physics and as a crucial ingredient in realizing new universality classes for quantum dynamics. | background 1.00 | 0.04 | 0.03 | asserted 1.00 |
| s1 | Here we address the question of whether and when multipole symmetries can be spontaneously broken, both in thermal equilibrium and at zero temperature. | contribution 0.45 | 0.29 | 0.05 | unclear 0.88 |
| s2 | We derive generalized Mermin-Wagner arguments for the total or partial breaking of multipolar symmetry groups and generalized Imry-Ma arguments for the robustness of such multipolar symmetry breaking to disorder. | contribution 0.71 | 0.96 | 0.25 | asserted 1.00 |
| s3 | We present both general results and explicit examples. | contribution 0.96 | 0.87 | 0.05 | asserted 0.95 |
| s4 | Our results should be directly applicable to quantum dynamics with multipolar symmetries and also provide a useful stepping stone to understanding the robustness of fracton phases to thermal fluctuations, quantum fluctuations, and disorder. | interpretation 0.94 | 0.35 | 0.21 | hedged possibility 0.63 |
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Original abstract
Multipole symmetries are of interest both as a window on fracton physics and as a crucial ingredient in realizing new universality classes for quantum dynamics. Here we address the question of whether and when multipole symmetries can be spontaneously broken, both in thermal equilibrium and at zero temperature. We derive generalized Mermin-Wagner arguments for the total or partial breaking of multipolar symmetry groups and generalized Imry-Ma arguments for the robustness of such multipolar symmetry breaking to disorder. We present both general results and explicit examples. Our results should be directly applicable to quantum dynamics with multipolar symmetries and also provide a useful stepping stone to understanding the robustness of fracton phases to thermal fluctuations, quantum fluctuations, and disorder.
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References
How the literature uses it
24 arXiv papers cite this in 34 sentences
Papers citing it · 19 sentences without a confident label
Cites it as support 1 paper
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Despite being a continuous symmetry, and despite being in one dimension, dipole symmetry is actually spontaneously broken in the BEI at $T=0$ [ref] : indeed, correlations of the dipole order parameter $e^i_xϕ$ go as C_e^i_x ϕ(0,x) ∼e^-∫_q,øq^2 1-cos(qx)/ø^2 K_τ+q^4 K_D x ∞ 1,as the integral in the exponential is IR-finite (c.f. the power law behavior in the DC phase [ref]), implying a nonzero expectation value $|d_i | ≠0$.
Dipole condensates in tilted Bose-Hubbard chains · Finite size effects and the Bose Einstein Insulator · 0.98
Cites it as background 12 papers
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This global symmetry and the current conservation have been studied in [ref] .
Global Dipole Symmetry, Compact Lifshitz Theory, Tensor Gauge Theory, and Fractons · Introduction · 0.80
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So the mobile subspace is the $t-x$ plane, and the defect with respect to the $t-x$ plane is of codimension one.] [ref] .[There are also earlier works on subsystem symmetry from algebraic duality approach [ref] .] Here and in Tab. [ref] we only present a highly incomplete list of references.[Another line of development of unconventional symmetry, motivated by commutant algebra in the study of quantum many body scar, was explored in [ref] .
Subsystem Non-Invertible Symmetry Operators and Defects · Subsystem non-invertible symmetry · 0.80
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They encompass the higher-form or higher-group symmetries [ref] , non-invertible symmetries [ref] , subsystem symmetries [ref] , etc.
Web of 4D Dualities, Supersymmetric Partition functions and SymTFT · Introduction and Conclusion · 0.99
What it cites · 3 sentences without a confident label
Cites as background 3 papers
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A detailed discussion of the phase diagram and phenomenology of this model is given in [ref] ; in the following we will simply discuss the symmetry breaking patterns realized in various different limits.
The dipolar Bose-Hubbard model · Explicit lattice example · 0.93
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They are known to arise in `fracton' phases of quantum matter [ref] , the key dynamical properties of which are known to descend from conservation laws on multipole moments of charge [ref] .
Generalized $U(1)$ Gauge Field Theories and Fractal Dynamics · Introduction · 0.85
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Another setting for generalized Mermin-Wagner-type arguments is higher form global symmetries [ref] .
Higher-form symmetries and spontaneous symmetry breaking · Discussion · 0.89
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