Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Spin-liquid phase in a spin-1/2 quantum magnet on the kagome lattice

Sergei V. Isakov, Yong Baek Kim, Arun Paramekanti

Published Mar 5, 2007• 3 citations
OpenAlex

Abstract

We study a model of hard-core bosons with short-range repulsive interactions at half filling on the kagome lattice. Using quantum Monte Carlo numerics, we find that this model shows a continuous superfluid-insulator quantum phase transition, with exponents $z=1$ and $\ensuremath{\nu}\ensuremath{\approx}0.67(5)$. The insulator, ${\mathcal{I}}^{*}$, exhibits short-ranged density and bond correlations, topological order, and exponentially decaying spatial vison correlations, all of which point to a ${Z}_{2}$ fractionalized phase. We estimate the vison gap in ${\mathcal{I}}^{*}$ from the temperature dependence of the energy. Our results, together with the equivalence between hard-core bosons and $S=1/2$ spins, provide compelling evidence for a spin-liquid phase in an easy-axis spin-$1/2$ model with no special conservation laws.

Related papers

Spin-Liquid Phase in a Spin- 1/2 Quantum Magnet on the Kagome Lattice

Sergei V. Isakov, Yong Baek Kim, Arun Paramekanti

We study a model of hard-core bosons with short-range repulsive interactions at half filling on the kagome lattice. Using quantum Monte Carlo numerics, we find that this model shows a continuous superfluid-insulator quantum phase transition, with exponents z=1 and nu approximately 0.67(5). The insulator, I*, exhibits short-ranged density and bond correlations, topological order, and exponentially decaying spatial vison correlations, all of which point to a Z2 fractionalized phase. We estimate the vison gap in I* from the temperature dependence of the energy. Our results, together with the equivalence between hard-core bosons and S=1/2 spins, provide compelling evidence for a spin-liquid phase in an easy-axis spin-1/2 model with no special conservation laws.

arXiv:cond-mat/0607778•Physical Review Letters•Nov 15, 2006•62 citations

Exotic phase diagram of a cluster charging model of bosons on the kagome lattice

Sergei V. Isakov, Arun Paramekanti, Yong Baek Kim

We study a model of hard-core bosons on the kagome lattice with short-range hopping $(t)$ and repulsive interactions $(V)$. This model directly maps onto an easy-axis $S=1∕2$ XXZ model on the kagome lattice and is also related, at large $V∕t$, to a quantum dimer model on the triangular lattice. Using quantum Monte Carlo numerics, we map out the phase diagram of this model at half-filling. At $T=0$, we show that this model exhibits a superfluid phase at small $V∕t$ and an insulating phase at large $V∕t$, separated by a continuous quantum phase transition at ${V}_{c}∕t\ensuremath{\approx}19.8$. The insulating phase at $T=0$ appears to have no conventional broken symmetries, and is thus a uniform Mott insulator (a ``spin liquid'' in magnetic language). We characterize this insulating phase as a uniform ${Z}_{2}$ fractionalized insulator from the topological order in the ground state and estimate its vison gap. Consistent with this identification, there is no apparent thermal phase transition upon heating the insulator. The insulating phase instead smoothly crosses over into the high temperature paramagnet via an intermediate cooperative paramagnetic regime. We also study the superfluid-to-normal thermal transition for $V<{V}_{c}$. We find that this is a Kosterlitz-Thouless transition at small $V∕t$ but changes to a first order transition for $V$ closer to ${V}_{c}$. We argue that this first order thermal transition is consistent with the presence of a nearby ${Z}_{2}$ insulating ground state obtained from the superfluid ground state by condensing double vortices.

arXiv:0706.4310•Physical Review B•Dec 27, 2007•21 citations

Hard-Core Bosons on the Kagome Lattice: Valence-Bond Solids and Their Quantum Melting

Sergei V. Isakov, Stefan Weßel, Roger G. Melko +2 more

Using large scale quantum Monte Carlo simulations and dual vortex theory, we analyze the ground state phase diagram of hard-core bosons on the kagome lattice with nearest-neighbor repulsion. In contrast with the case of a triangular lattice, no supersolid emerges for strong interactions. While a uniform superfluid prevails at half filling, two novel solid phases emerge at densities rho=1/3 and rho=2/3. These solids exhibit an only partial ordering of the bosonic density, allowing for local resonances on a subset of hexagons of the kagome lattice. We provide evidence for a weakly first-order phase transition at the quantum melting point between these solid phases and the superfluid.

arXiv:cond-mat/0602430•Physical Review Letters•Oct 6, 2006•163 citations

Valence Bond Solids and Unconventional Quantum Criticality in Hard-Core Bosons on the Kagome Lattice

Sergei V. Isakov, Stefan Weßel, Roger G. Melko +2 more

Using large scale quantum Monte Carlo simulations and dual vortex theory we analyze the ground state phase diagram of hard-core bosons on the kagome lattice with nearest neighbor repulsion. In contrast to the case of a triangular lattice, no supersolid emerges for strong interactions. While a uniform superfluid prevails at half-filling, two novel solid phases emerge at densities $\rho=1/3$ and $\rho=2/3$. These solids exhibit an only partial ordering of the bosonic density, allowing for local resonances on a subset of hexagons of the kagome lattice. We provide evidence for a weakly first-order phase transition at the quantum melting point between these solid phases and the superfluid.

•Feb 17, 2006•0 citations

Z2 topological liquid of hard-core bosons on a kagome lattice at 1/3 filling

Krishanu Roychowdhury, Subhro Bhattacharjee, Frank Pollmann

We consider hard-core bosons on the kagome lattice in the presence of short-range repulsive interactions and focus particularly on the filling factor $1/3$. In the strongly interacting limit, the low-energy excitations can be described by the quantum fully packed loop coverings on the triangular lattice. Using a combination of tensor product state based methods and exact diagonalization techniques, we show that the system has an extended ${\mathbb{Z}}_{2}$ topological liquid phase as well as a latti ce nematic phase. The latter breaks lattice rotational symmetry. By tuning appropriate parameters in the model, we study the quantum phase transition between the topological and the symmetry broken phases. We construct the critical theory for this transition using a mapping to an Ising gauge theory that predicts the transition to belong to the $O(3)$ universality class.

arXiv:1505.05998•Physical Review B•Aug 26, 2015•30 citations

Continuous Easy-Plane Deconfined Phase Transition on the Kagome Lattice

Xue‐Feng Zhang, Yin-Chen He, Sebastian Eggert +2 more

We use large scale quantum Monte Carlo simulations to study an extended Hubbard model of hard core bosons on the kagome lattice. In the limit of strong nearest-neighbor interactions at 1/3 filling, the interplay between frustration and quantum fluctuations leads to a valence bond solid ground state. The system undergoes a quantum phase transition to a superfluid phase as the interaction strength is decreased. It is still under debate whether the transition is weakly first order or represents an unconventional continuous phase transition. We present a theory in terms of an easy plane noncompact CP^{1} gauge theory describing the phase transition at 1/3 filling. Utilizing large scale quantum Monte Carlo simulations with parallel tempering in the canonical ensemble up to 15552 spins, we provide evidence that the phase transition is continuous at exactly 1/3 filling. A careful finite size scaling analysis reveals an unconventional scaling behavior hinting at deconfined quantum criticality.

arXiv:1706.05414•Physical Review Letters•Mar 15, 2018•56 citations
We study a model of hard-core bosons with short-range repulsive interactions at half filling on the kagome lattice. Using quantum Monte Carlo numerics, we find that this model shows a continuous superfluid-insulator quantum phase transition, with exponents z=1z=1z=1 and \ensuremathν\ensuremath≈0.67(5)\ensuremath{\nu}\ensuremath{\approx}0.67(5)\ensuremathν\ensuremath≈0.67(5). The insulator, I∗{\mathcal{I}}^{*}I∗, exhibits short-ranged density and bond correlations, topological order, and exponentially decaying spatial vison correlations, all of which point to a Z2{Z}_{2}Z2​ fractionalized phase. We estimate the vison gap in I∗{\mathcal{I}}^{*}I∗ from the temperature dependence of the energy. Our results, together with the equivalence between hard-core bosons and S=1/2S=1/2S=1/2 spins, provide compelling evidence for a spin-liquid phase in an easy-axis spin-1/21/21/2 model with no special conservation laws.
We study a model of hard-core bosons with short-range repulsive interactions at half filling on the kagome lattice. Using quantum Monte Carlo numerics, we find that this model shows a continuous superfluid-insulator quantum phase transition, with exponents z=1 and nu approximately 0.67(5). The insulator, I*, exhibits short-ranged density and bond correlations, topological order, and exponentially decaying spatial vison correlations, all of which point to a Z2 fractionalized phase. We estimate the vison gap in I* from the temperature dependence of the energy. Our results, together with the equivalence between hard-core bosons and S=1/2 spins, provide compelling evidence for a spin-liquid phase in an easy-axis spin-1/2 model with no special conservation laws.
We study a model of hard-core bosons on the kagome lattice with short-range hopping (t)(t)(t) and repulsive interactions (V)(V)(V). This model directly maps onto an easy-axis S=1∕2S=1∕2S=1∕2 XXZ model on the kagome lattice and is also related, at large V∕tV∕tV∕t, to a quantum dimer model on the triangular lattice. Using quantum Monte Carlo numerics, we map out the phase diagram of this model at half-filling. At T=0T=0T=0, we show that this model exhibits a superfluid phase at small V∕tV∕tV∕t and an insulating phase at large V∕tV∕tV∕t, separated by a continuous quantum phase transition at ${V}_{c}∕t\ensuremath{\approx}19.8$. The insulating phase at T=0T=0T=0 appears to have no conventional broken symmetries, and is thus a uniform Mott insulator (a ``spin liquid'' in magnetic language). We characterize this insulating phase as a uniform Z2{Z}_{2}Z2​ fractionalized insulator from the topological order in the ground state and estimate its vison gap. Consistent with this identification, there is no apparent thermal phase transition upon heating the insulator. The insulating phase instead smoothly crosses over into the high temperature paramagnet via an intermediate cooperative paramagnetic regime. We also study the superfluid-to-normal thermal transition for V<VcV<{V}_{c}V<Vc​. We find that this is a Kosterlitz-Thouless transition at small V∕tV∕tV∕t but changes to a first order transition for VVV closer to Vc{V}_{c}Vc​. We argue that this first order thermal transition is consistent with the presence of a nearby Z2{Z}_{2}Z2​ insulating ground state obtained from the superfluid ground state by condensing double vortices.
Using large scale quantum Monte Carlo simulations and dual vortex theory, we analyze the ground state phase diagram of hard-core bosons on the kagome lattice with nearest-neighbor repulsion. In contrast with the case of a triangular lattice, no supersolid emerges for strong interactions. While a uniform superfluid prevails at half filling, two novel solid phases emerge at densities rho=1/3 and rho=2/3. These solids exhibit an only partial ordering of the bosonic density, allowing for local resonances on a subset of hexagons of the kagome lattice. We provide evidence for a weakly first-order phase transition at the quantum melting point between these solid phases and the superfluid.
Using large scale quantum Monte Carlo simulations and dual vortex theory we analyze the ground state phase diagram of hard-core bosons on the kagome lattice with nearest neighbor repulsion. In contrast to the case of a triangular lattice, no supersolid emerges for strong interactions. While a uniform superfluid prevails at half-filling, two novel solid phases emerge at densities ρ=1/3\rho=1/3ρ=1/3 and ρ=2/3\rho=2/3ρ=2/3. These solids exhibit an only partial ordering of the bosonic density, allowing for local resonances on a subset of hexagons of the kagome lattice. We provide evidence for a weakly first-order phase transition at the quantum melting point between these solid phases and the superfluid.
We consider hard-core bosons on the kagome lattice in the presence of short-range repulsive interactions and focus particularly on the filling factor 1/31/31/3. In the strongly interacting limit, the low-energy excitations can be described by the quantum fully packed loop coverings on the triangular lattice. Using a combination of tensor product state based methods and exact diagonalization techniques, we show that the system has an extended Z2{\mathbb{Z}}_{2}Z2​ topological liquid phase as well as a latti ce nematic phase. The latter breaks lattice rotational symmetry. By tuning appropriate parameters in the model, we study the quantum phase transition between the topological and the symmetry broken phases. We construct the critical theory for this transition using a mapping to an Ising gauge theory that predicts the transition to belong to the O(3)O(3)O(3) universality class.
We use large scale quantum Monte Carlo simulations to study an extended Hubbard model of hard core bosons on the kagome lattice. In the limit of strong nearest-neighbor interactions at 1/3 filling, the interplay between frustration and quantum fluctuations leads to a valence bond solid ground state. The system undergoes a quantum phase transition to a superfluid phase as the interaction strength is decreased. It is still under debate whether the transition is weakly first order or represents an unconventional continuous phase transition. We present a theory in terms of an easy plane noncompact CP^{1} gauge theory describing the phase transition at 1/3 filling. Utilizing large scale quantum Monte Carlo simulations with parallel tempering in the canonical ensemble up to 15552 spins, we provide evidence that the phase transition is continuous at exactly 1/3 filling. A careful finite size scaling analysis reveals an unconventional scaling behavior hinting at deconfined quantum criticality.