Abstract

Models whose ground states can be written as an exact matrix product state (MPS) provide valuable insights into phases of matter. While MPS-solvable models are typically studied as isolated points in a phase diagram, they can belong to a connected network of MPS-solvable models, which we call the MPS skeleton. As a case study where we can completely unearth this skeleton, we focus on the one-dimensional BDI class -- non-interacting spinless fermions with time-reversal symmetry. This class, labelled by a topological winding number, contains the Kitaev chain and is Jordan-Wigner-dual to various symmetry-breaking and symmetry-protected topological (SPT) spin chains. We show that one can read off from the Hamiltonian whether its ground state is an MPS: defining a polynomial whose coefficients are the Hamiltonian parameters, MPS-solvability corresponds to this polynomial being a perfect square. We provide an explicit construction of the ground state MPS, its bond dimension growing exponentially with the range of the Hamiltonian. This complete characterization of the MPS skeleton in parameter space has three significant consequences: (i) any two topologically distinct phases in this class admit a path of MPS-solvable models between them, including the phase transition which obeys an area law for its entanglement entropy; (ii) we illustrate that the subset of MPS-solvable models is dense in this class by constructing a sequence of MPS-solvable models which converge to the Kitaev chain (equivalently, the quantum Ising chain in a transverse field); (iii) a subset of these MPS states can be particularly efficiently processed on a noisy intermediate-scale quantum computer.

Highlights

  • The realization that the entanglement of gapped manybody ground states obeys an area law was a breakthrough for condensed matter physics [1]

  • Our analysis shows that the implication works the other way: this property is sufficient for MPSsolvability, and we give an explicit construction of the ground state

  • The formula for χ is for matrix-product state (MPS) which are symmetric under fermion parity; in the case of spontaneous symmetry breaking, this formula applies to the cat state, whereas the symmetrybroken state has log2 χ = range(H )/2

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Summary

INTRODUCTION

The realization that the entanglement of gapped manybody ground states obeys an area law was a breakthrough for condensed matter physics [1]. Despite free-fermion Hamiltonians and MPS-solvable systems both being pinnacles of solubility, they have a rich interplay: one cannot typically write the ground state of a free-fermion system as an exact MPS due to its entanglement spectrum having infinite rank, and there is no analytic handle on truncating this to a particular bond dimension. This truncation has been investigated numerically: an approach for the XY model is given in Ref.

SUMMARY OF MAIN RESULTS
The MPS skeleton
Construction of MPS
Consequences
EXAMPLES
Result
A path of MPS for the quantum Ising chain
ANALYSIS
The Hamiltonians are frustration-free
Analysis
MPS representation
Unitary version
Circuit construction
A formula for the order parameter
Multicritical points
OUTLOOK
The gapped case and correlations
Proof that the MPS path is optimal
Variational energy
Algebraic relations for Un
General bond dimension formula
Findings
The gapless case
Full Text
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