Identifying Hidden Graphs with Quantum Walks: From BQP-Completeness to an Exponential Separation

Paweł

Wocjan

IBM Quantum

September 15, 2026 02:30 AM

Abstract:

Time evolution under a huge, sparse Hamiltonian can, from a well-chosen initial state, behave exactly like a walk on a tiny graph: the evolution never leaves a low-dimensional invariant subspace, and on that subspace the Hamiltonian is the adjacency matrix of a small graph. If we know in advance that this small graph is one of two possibilities, the algorithm splits cleanly into two parts. Classically, and before the quantum computer is switched on, we compute the return amplitudes of the two candidate graphs and the time at which they differ most. Quantumly, we run the evolution for exactly that long and read off the amplitude by interferometry — a Hadamard test, with the evolution as its controlled operation.

I will describe two problems of this shape. In the first, the small graph is a cycle whose length encodes the outcome of an arbitrary quantum circuit; deciding whether the short or the long cycle is hidden inside the Hamiltonian is therefore BQP-complete, so this single question captures the full power of quantum computation. In the second, we get to choose the hidden graph ourselves. Any regular graph can be buried inside an exponentially larger "spired graph," presented only through a black box that returns the neighbors of a label and reveals nothing else. The quantum walk collapses that graph back down to a polynomial-size object determined by the graph we hid; classically the problem is conjectured to be intractable, by close analogy with the proved exponential lower bound for the welded-trees problem, which the construction specializes to. Taking the two candidates to be a prism and a Möbius ladder — the same ladder closed straight or closed with a single localized twist — gives an efficient quantum identification algorithm supported by spectral theory and numerics, together with a conjectured exponential separation relative to the oracle. Details of the second part: arXiv:2605.11228 (https://arxiv.org/abs/2605.11228); the BQP connection is not in the paper.

Date: Sep 15, 2026 02:30 PM CEST, Room D

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Remigiusz Augusiak, Wojciech Bruzda, Marcin Kotowski, Michał Oszmaniec