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Rapid adiabatic preparation of injective PEPS and Gibbs states (1508.00570v2)

Published 3 Aug 2015 in quant-ph

Abstract: We propose a quantum algorithm for many-body state preparation. It is especially suited for injective PEPS and thermal states of local commuting Hamiltonians on a lattice. We show that for a uniform gap and sufficiently smooth paths, an adiabatic runtime and circuit depth of $O(\operatorname{polylog}N)$ can be achieved for $O(N)$ spins. This is an almost exponential improvement over previous bounds. The total number of elementary gates scales as $O(N\operatorname{polylog}N)$. This is also faster than the best known upper bound of $O(N2)$ on the mixing times of Monte Carlo Markov chain algorithms for sampling classical systems in thermal equilibrium.

Citations (6)

Summary

  • The paper presents a rapid adiabatic quantum algorithm achieving a near-exponential speedup for preparing injective PEPS and Gibbs states with O(polylog N) runtime.
  • This algorithm enables O(N polylog N) quantum circuits, offering a significant advantage over classical methods and overcoming computational challenges like the sign problem.
  • These advancements offer practical benefits for quantum state preparation and sampling, with potential for future application in quantum simulation, optimization, and machine learning.

Rapid Adiabatic Preparation of Injective PEPS and Gibbs States

The paper entitled "Rapid adiabatic preparation of injective PEPS and Gibbs states" presents a quantum algorithm designed for the preparation of many-body quantum states, particularly injective Projected Entangled Pair States (PEPS) and thermal states of local commuting Hamiltonians on a lattice. This work highlights a significant advancement in reducing the adiabatic runtime and circuit depth, achieving a near exponential improvement over previous methods.

Summary of the Algorithm

The research introduces an algorithmic approach that substantially enhances state preparation speed by leveraging adiabatic processes. Significantly, it addresses two classes of quantum states:

  1. Injective PEPS: Representations of ground states in local gapped Hamiltonians.
  2. Gibbs States: Systems in thermal equilibrium described by a Gibbs distribution.

The crux of the proposed method lies in its ability to attain an adiabatic runtime and circuit depth scaling as $O(\polylog N)$ for systems comprising O(N)O(N) spins. This offers an almost exponential speedup relative to earlier algorithms and is notably faster than conventional Monte Carlo Markov chain methods, the latter being limited by non-optimal O(N2)O(N^2) bounds on mixing times.

Numerical and Theoretical Insights

This algorithm achieves the deployment of quantum circuits with complexity scaling as $O(N\polylog N)$, presenting a real step forward from the best-known classical techniques. The key to such efficiency lies in the algorithm's ability to maintain an adiabatic path with uniformly bounded gaps and smooth transitions.

Moreover, the paper emphasizes the implications of these advancements:

  • Practical: The increased efficacy of sampling from quantum distributions at finite temperatures and facilitating state preparation for optimization problems using injective PEPS.
  • Theoretical Implications: Demonstrates that quantum algorithms can circumvent classical computational hurdles such as the sign problem, leveraging quantum mechanical properties to yield computational advantages.

Future Developments and Implications

While the paper solidifies a profound leap in the adiabatic preparation of many-body states, it opens several avenues for future exploration:

  • Extending these methods to cover non-commuting Hamiltonians effectively, thus broadening the scope of quantum simulations.
  • Investigating further applications in deep machine learning, where quantum speedups could drastically alter computational paradigms.
  • Assessing the practical application of this quantum algorithm in analog quantum simulators, particularly those involving trapped ions or optical lattices.

In conclusion, this work provides a robust framework for utilizing quantum algorithms to achieve substantial speed improvements in state preparation over existing classical and quantum methods. The advancements in circuit efficiency and depth highlight the potential for quantum computing to tackle complex simulation problems in physics and beyond. The broader implications could be realized across multiple fields, opening new grounds for both theoretical innovations and practical applications.

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