Abstract

While several tools have been developed to study the ground state of many-body quantum spin systems, the limitations of existing techniques call for the exploration of new approaches. In this manuscript we develop an alternative analytical and numerical framework for many-body quantum spin ground states, based on the disentanglement formalism. In this approach, observables are exactly expressed as Gaussian-weighted functional integrals over scalar fields. We identify the leading contribution to these integrals, given by the saddle point of a suitable effective action. Analytically, we develop a field-theoretical expansion of the functional integrals, performed by means of appropriate Feynman rules. The expansion can be truncated to a desired order to obtain analytical approximations to observables. Numerically, we show that the disentanglement approach can be used to compute ground state expectation values from classical stochastic processes. While the associated fluctuations grow exponentially with imaginary time and the system size, this growth can be mitigated by means of an importance sampling scheme based on knowledge of the saddle point configuration. We illustrate the advantages and limitations of our methods by considering the quantum Ising model in 1, 2 and 3 spatial dimensions. Our analytical and numerical approaches are applicable to a broad class of systems, bridging concepts from quantum lattice models, continuum field theory, and classical stochastic processes.

Highlights

  • Lattice quantum spin systems constitute an important class of models in many-body physics

  • Going beyond previous applications of the disentanglement formalism, we identify the trajectory yielding the largest contribution to a given observable: this corresponds to the saddle point configuration extremizing a suitably defined effective action, as we illustrate for the quantum Ising model in D spatial dimensions

  • We showed that the disentanglement formalism [24, 55, 56, 58, 59] provides a broadly applicable framework to describe many-body quantum spin ground states, bridging concepts from lattice spin systems, field theory and classical stochastic processes

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Summary

INTRODUCTION

Lattice quantum spin systems constitute an important class of models in many-body physics. Away from exactly solvable integrable models [8, 9], which are mostly one dimensional, analytical treatments of quantum spin systems are typically based on the spin coherent state path integral [10,11,12,13,14,15]. The path integrals obtained from the disentanglement method can be evaluated by numerically solving a set of stochastic differential equations [24, 55]. While this approach has been recently investigated in non-equilibrium settings [58, 59], much less is known in the context of ground states.

Disentanglement Transformation
Extremal Trajectories
Ising Saddle Point Equation
FIELD THEORY
Leading Order
Higher Order Corrections and Quantum Phase Transitions
Feynman Rules
Relation to Perturbation Theory
Example
Numerical Results
Fluctuations
CONCLUSIONS
General Case
Details on the Disentanglement Transformation in Higher Dimensions
Ising SDEs
Exactly Solvable Limits
Moments of the Disentangling Variables
Joint Probability Distribution
Numerical Solution
Saddle Point for General Observables
Higher Dimensions
Multiple Saddle Points
Quantum Phase Transitions
Full Text
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