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arXiv:2610.38741

Mixed-State Topological Transition and Emergent Fractionalized Supersymmetry in the Non-Abelian Kitaev Spin Liquid

Zhou-Quan Wan, Hong Yao, Shao-Kai Jian

cond-mat.str-elcond-mat.stat-mechquant-phSubmitted Oct 28, 2026• Announced Oct 30, 2026• 0 citations
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Abstract

We study a mixed-state topological transition in the non-Abelian Kitaev spin liquid driven by a bond-dephasing channel. In the vectorized picture, bond dephasing maps onto interactions between two time-reversed fractionalized Majorana systems coupled to gapped $\mathbb Z_2$ gauge fields, enabling sign-problem-free Monte Carlo simulations. We show that increasing dephasing condenses an inter-copy fermion pair, converting ${\rm Ising}\boxtimes\overline{\rm{Ising}}$ to toric-code order in the Choi state and yielding intrinsically mixed-state topological order upon unfolding. More interestingly, at a temporal interface between topological and trivial Kitaev states, a Chern-number mismatch enforces a gapless Majorana mode. Dephasing then drives a mixed-state topological transition at which the gapless mode develops emergent $\mathcal N=1$ supersymmetry. Our Monte Carlo simulations yield $ν=1.27(3)$ and $η_b\simeqη_f\simeq0.40$, consistent with the exact supersymmetric values $5/4$ and $2/5$. The supersymmetric partners are fractionalized and appear physically as distinct gauge-invariant spin strings, providing concrete observables for future experiments.

AI Summary

The paper asks how decoherence changes non-Abelian topological order and whether it can produce supersymmetric mixed-state criticality. It studies flux-preserving bond dephasing of the chiral Kitaev honeycomb ground state. Vectorization maps the channel to interactions between time-reversed Majorana copies; an exact auxiliary-field decomposition yields nonnegative Monte Carlo weights without Trotter error. In the normalized vectorized density matrix, increasing dephasing condenses the inter-copy boson $\psi\bar\psi$, changing doubled-Ising order to toric-code order. For $J_x=J_y=J_z=1$ and $\kappa=0.5$, Wilson-string finite-size scaling gives $p_c^{(2)}=0.16687(8)$, $\nu=1.011(16)$ and $\eta=0.246(11)$, consistent with two-dimensional Ising criticality. Unfolding the maximal-dephasing endpoint gives intrinsically mixed-state topological order with a transparent fermion. A distinct calculation uses strange correlators between topological and trivial reference states. Their Chern-number mismatch supplies gapless Majorana modes at a temporal interface. Dephasing drives this interface to a proposed tricritical-Ising endpoint with emergent $\mathcal N=1$ supersymmetry. Simulations up to $L=57$ give $p_c=0.24526(6)$, $\nu=1.27(3)$, $\eta_b=0.405(6)$ and $\eta_f=0.395(21)$, consistent with $5/4$ and $2/5$. Bosonic and fermionic partners are probed by distinct gauge-invariant spin strings; their estimated anisotropies also agree. The exponent $5/4$ applies to the symmetry-constrained dephasing trajectory, not generic tricritical-Ising tuning. The finite-dephasing mixed-state phase assignment assumes no intervening transition before maximal dephasing. Persistence beyond the integrable, flux-conserving setting is anticipated only while visons remain gapped and gauge fluctuations introduce no additional relevant perturbations.

Little sign of AI-generated textStrong assumptions

Error found: The abstract leaves implicit that extending the maximal-dephasing imTO identification to the finite-dephasing ordered branch assumes that no additional transition intervenes.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
4.3 pages + supplemental material, 3 figures

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We study a mixed-state topological transition in the non-Abelian Kitaev spin liquid driven by a bond-dephasing channel. In the vectorized picture, bond dephasing maps onto interactions between two time-reversed fractionalized Majorana systems coupled to gapped Z2\mathbb Z_2Z2​ gauge fields, enabling sign-problem-free Monte Carlo simulations. We show that increasing dephasing condenses an inter-copy fermion pair, converting Ising⊠Ising‾{\rm Ising}\boxtimes\overline{\rm{Ising}}Ising⊠Ising​ to toric-code order in the Choi state and yielding intrinsically mixed-state topological order upon unfolding. More interestingly, at a temporal interface between topological and trivial Kitaev states, a Chern-number mismatch enforces a gapless Majorana mode. Dephasing then drives a mixed-state topological transition at which the gapless mode develops emergent N=1\mathcal N=1N=1 supersymmetry. Our Monte Carlo simulations yield ν=1.27(3)ν=1.27(3)ν=1.27(3) and ηb≃ηf≃0.40η_b\simeqη_f\simeq0.40ηb​≃ηf​≃0.40, consistent with the exact supersymmetric values 5/45/45/4 and 2/52/52/5. The supersymmetric partners are fractionalized and appear physically as distinct gauge-invariant spin strings, providing concrete observables for future experiments.
The paper asks how decoherence changes non-Abelian topological order and whether it can produce supersymmetric mixed-state criticality. It studies flux-preserving bond dephasing of the chiral Kitaev honeycomb ground state. Vectorization maps the channel to interactions between time-reversed Majorana copies; an exact auxiliary-field decomposition yields nonnegative Monte Carlo weights without Trotter error.
In the normalized vectorized density matrix, increasing dephasing condenses the inter-copy boson ψψˉ\psi\bar\psiψψˉ​, changing doubled-Ising order to toric-code order. For Jx=Jy=Jz=1J_x=J_y=J_z=1Jx​=Jy​=Jz​=1 and κ=0.5\kappa=0.5κ=0.5, Wilson-string finite-size scaling gives pc(2)=0.16687(8)p_c^{(2)}=0.16687(8)pc(2)​=0.16687(8), ν=1.011(16)\nu=1.011(16)ν=1.011(16) and η=0.246(11)\eta=0.246(11)η=0.246(11), consistent with two-dimensional Ising criticality. Unfolding the maximal-dephasing endpoint gives intrinsically mixed-state topological order with a transparent fermion.
A distinct calculation uses strange correlators between topological and trivial reference states. Their Chern-number mismatch supplies gapless Majorana modes at a temporal interface. Dephasing drives this interface to a proposed tricritical-Ising endpoint with emergent N=1\mathcal N=1N=1 supersymmetry. Simulations up to L=57L=57L=57 give pc=0.24526(6)p_c=0.24526(6)pc​=0.24526(6), ν=1.27(3)\nu=1.27(3)ν=1.27(3), ηb=0.405(6)\eta_b=0.405(6)ηb​=0.405(6) and ηf=0.395(21)\eta_f=0.395(21)ηf​=0.395(21), consistent with 5/45/45/4 and 2/52/52/5. Bosonic and fermionic partners are probed by distinct gauge-invariant spin strings; their estimated anisotropies also agree. The exponent 5/45/45/4 applies to the symmetry-constrained dephasing trajectory, not generic tricritical-Ising tuning.
The finite-dephasing mixed-state phase assignment assumes no intervening transition before maximal dephasing. Persistence beyond the integrable, flux-conserving setting is anticipated only while visons remain gapped and gauge fluctuations introduce no additional relevant perturbations.
We investigate how the Kitaev spin liquid state described by Majorana fermions coupled with Z2{Z}_{2}Z2​ gauge fields is affected by non-Kitaev interactions which exist in real candidate materials of the Kitaev magnet. It is found that the off-diagonal exchange interaction referred to as the ${\mathrm{\ensuremath{\Gamma}}}^{\ensuremath{'}}$ term dramatically changes the Majorana band structure in the case of the antiferromagnetic Kitaev interaction and gives rise to a topological phase transition from a non-Abelian topological phase with the Chern number equal to $\ifmmode\pm\else\textpm\fi{}1$ to an Abelian phase with the Chern number equal to $\ifmmode\pm\else\textpm\fi{}2$, in which the Z2{Z}_{2}Z2​ vortices behave as Abelian anyons. On the other hand, other non-Kitaev interactions such as the Heisenberg interaction and the $\mathrm{\ensuremath{\Gamma}}$ term only affect the bandwidth of the Majorana band as long as the spin liquid state is not destabilized.
The competition between fractionalized spin-liquid states and magnetically ordered phases is an important paradigm in frustrated magnetism. Spin-orbit coupled Mott insulators with Ising-like magnetic anisotropies, such as Kitaev materials, are a particularly rich playground to explore this competition. In this work, we use effective field theory methods to show that a direct quantum phase transition can occur in two-dimensional (2D) Ising spin systems between a topologically ordered chiral spin liquid and a phase with magnetic long-range order. Such a transition can be protected by lattice symmetries and is described by a theory of massless Majorana fields coupled to non-Abelian SO(N)\text{SO}(N)SO(N) gauge fields with a Chern-Simons term. We further show that Euclidean Majorana zero modes bound to Z2{\mathbb{Z}}_{2}Z2​ monopole-instantons in the emergent non-Abelian gauge field are key to understanding spontaneous symmetry breaking in the ordered phase.
We study quantum phase transitions in the honeycomb Kitaev model under a magnetic field, focusing on the topological nature of Majorana fermion excitations. We find a gapless phase between the low-field gapless quantum spin liquid and the high-field gapped forced-ferromagnetic state for the antiferromagnetic Kitaev model in the [001] field by using the Majorana mean-field theory, in conjunction with the exact diagonalization and the spin-wave theory supporting the validity of this approach. The transition between the two gapless phases is driven by a topological change of the Majorana spectrum---line node formation interconnecting two Majorana cones. The peculiar change of the Majorana band topology is rationalized by a sign change of the effective Kitaev coupling by the magnetic field, which does not occur in the ferromagnetic Kitaev case. Upon tilting the magnetic field away from [001], the two gapless phases become gapped and topologically nontrivial, characterized by nonzero Chern numbers with different signs. The sign change of the Chern number leads to a reversal of the thermal edge current in the half-quantized thermal Hall effect.
In the field of frustrated magnetism, Kitaev models provide prototypical examples of exactly solvable quantum spin liquids, in which the spin degrees of freedom fractionalize into Majorana fermions coupled to an emergent Z2 gauge field. While the ground states of these models are already well understood as exhibiting different kinds of Majorana (semi)metals, it has still been an open task to achieve a detailed understanding of the thermodynamics, and, namely, the low-temperature ordering of the gauge field into different Z2 flux configurations. In this thesis, we investigate the thermodynamics of Kitaev systems in two and three spatial dimensions with sign-problem-free quantum Monte Carlo simulations. In a first study of elementary 3D Kitaev models, we verify that the ground state Z2 flux sectors of these systems are entirely determined by their elementary plaquette length – a result which shows the validity of Lieb’s theorem for lattice geometries which lack the geometric requirements for its proof. We closely investigate the low-temperature phase transition associated with gauge-ordering, which is a particular realization of an inverted Ising phase transition, as it occurs in general lattice Z2 gauge theories. Our results corroborate the understanding of this transition as separating different regimes in terms of vison-loop excitations, by showing a clear correlation between the critical temperature and the vison gap. We also introduce the concept of “gauge frustration”, which, for a particular 3D Kitaev model, leads to the suppression of the phase transition and a more complex physical behavior at low temperatures. A second quantum Monte Carlo study focuses on a generalized 2D Kitaev model on a five-coordinated lattice system. Here, the gauge ordering is accompanied by the spontaneous breaking of time-reversal symmetry, a scenario which not only allows for a variety of topological ground states, but also for the occurrence of a phase transition in two spatial dimensions. We show that this model exhibits such a transition at a particularly high temperature scale. Moreover, the system possesses a number of phases where the Z2 fluxes are only partially ordered.
The Kitaev model on a honeycomb lattice with bond-dependent Ising interactions offers an exactly solvable model of a quantum spin liquid (QSL) with fractionalized excitations: gapped Z2{Z}_{2}Z2​ fluxes and gapless linearly dispersing Majorana fermions in the isotropic limit (Kx=Ky=Kz{K}_{x}={K}_{y}={K}_{z}Kx​=Ky​=Kz​). We explore the phase diagram along two axes, an external magnetic field hhh, applied out of plane of the honeycomb, and anisotropic interactions Kz{K}_{z}Kz​ larger than the other two (${K}_{x}={K}_{y}\ensuremath{\equiv}K$). For ${K}_{z}/K\ensuremath{\gg}2$ and h=0h=0h=0, the matter Majorana fermions have the largest gap, and the system is described by a gapped Z2{Z}_{2}Z2​ toric code. One of the central questions we address is whether the fractionalized excitations in the different phases have sharp signatures that can be detected in experiments. We show that while the response to single-spin excitations is broad, the spectral function corresponding to two-spin excitations across a bond has sharp signatures that can be attributed to specific anyons. In the toric code regime, the $\ensuremath{\epsilon}=e\ifmmode\times\else\texttimes\fi{}m$ fermion, formed from the bosonic Ising electric (eee) and magnetic (mmm) charges, disperses along a specific one-dimensional direction that provides a fingerprint of fractionalization. At lower Kz{K}_{z}Kz​ in the center of the Abelian phase, in a regime we dub the primordial fractionalized regime, the field generates a hybridization between the $\ensuremath{\epsilon}$ fermion and the Majorana matter fermion, resulting in a $\ensuremath{\psi}$ fermion which too has a distinct quasi-one-dimensional dispersion. All the other phases in the field-anisotropy plane are naturally obtained from this primordial soup. These highly constrained fractonlike dispersions can be observable by inelastic light and neutron scattering, thereby providing ``smoking gun'' signatures of fractionalization in the QSL phase. Our analysis is based on calculations of susceptibilities, topological entanglement entropy, and excitation dynamics, obtained using exact diagonalization and density matrix renormalization group, and supported by perturbation theory.
We propose a scenario of realizing the toric code phase, which can be potentially utilized for fault-tolerant quantum computation, in candidate materials of Kitaev magnets.It is demonstrated that four-body interactions among Majorana fermions in the Kitaev spin liquid state, which are induced by applied magnetic fields as well as non-Kitaev-type exchange interactions, trigger a nematic phase transition of Majorana bonds without magnetic orders, accompanying the change of the Chern number from ±1 to zero.This gapful spin liquid state with zero Chern number is simply the toric code phase.Our result potentially explains the topological nematic transition recently observed in α-RuCl 3 via heat capacity measurements (O.Tanaka et al.,