pith. sign in

Computational Bottlenecks of Quantum Annealing

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
abstract

A promising approach to solving hard binary optimisation problems is quantum adiabatic annealing (QA) in a transverse magnetic field. An instantaneous ground state --- initially a symmetric superposition of all possible assignments of $N$ qubits --- is closely tracked as it becomes more and more localised near the global minimum of the classical energy. Regions where the energy gap to excited states is small (e.g. at the phase transition) are the algorithm's bottlenecks. Here I show how for large problems the complexity becomes dominated by $O(\log N)$ bottlenecks inside the spin glass phase, where the gap scales as a stretched exponential. For smaller $N$, only the gap at the critical point is relevant, where it scales polynomially, as long as the phase transition is second order. This phenomenon is demonstrated rigorously for the two-pattern Gaussian Hopfield Model. Qualitative comparison with the Sherrington-Kirkpatrick Model leads to similar conclusions.

years

2026 1

verdicts

UNVERDICTED 1

representative citing papers

Energy gap of quantum spin glasses: a projection quantum Monte Carlo study

cond-mat.dis-nn · 2026-02-23 · unverdicted · novelty 6.0

Simulations find that the inverse energy gap in 2D Edwards-Anderson spin glasses develops a fat-tailed distribution with infinite variance for large N, while the Sherrington-Kirkpatrick model shows a finite-variance gap scaling roughly as N to the power -1/3.

citing papers explorer

Showing 1 of 1 citing paper.

  • Energy gap of quantum spin glasses: a projection quantum Monte Carlo study cond-mat.dis-nn · 2026-02-23 · unverdicted · none · ref 38 · internal anchor

    Simulations find that the inverse energy gap in 2D Edwards-Anderson spin glasses develops a fat-tailed distribution with infinite variance for large N, while the Sherrington-Kirkpatrick model shows a finite-variance gap scaling roughly as N to the power -1/3.