Skip to content
aiqbench takeQuantum Computing

aiqbench analysis

This research presents a rigorous theoretical framework for continuous-time quantum walks featuring absorption at boundaries modeled as non-Hermitian systems. By deriving closed-form expressions for the propagator, it reveals how strong dissipation creates localized edge modes that fundamentally alter first-passage statistics and phase-space dynamics. These findings advance our understanding of open quantum system behavior, which is critical for designing robust quantum algorithms resilient to decoherence.
Source coveringarXiv
What this isA model's reading of the article and related coverage, written for aiqbench. Not the publisher's words.

Boundary-localized non-Hermitian modes in an absorbing quantum walk

arXiv1 min read

arXiv:2605.08056v3 Announce Type: replace Abstract: We introduce and solve from first principles a continuous-time quantum walk with absorption generated by a Lindblad boundary sink of arbitrary strength. Tracing out the sink maps the problem onto a non-Hermitian tight-binding Hamiltonian with a rank-one imaginary defect on the semi-infinite line. We obtain closed-form expressions for the exact propagator, from which the first-passage statistics follow. Weak coupling limits absorption through inefficient transfer into the sink, whereas for strong dissipation, occupation at the boundary is stunted by the emergence of a localized non-Hermitian mode. Despite the different physical origin of these suppression mechanisms, we show their respective absorption probabilities exhibit an asymptotic duality. The evolution is conveniently visualized in phase-space, where the non-Hermitian mode produces a Wigner droplet exponentially confined near the edge site.

Abstract:We introduce and solve from first principles a continuous-time quantum walk with absorption generated by a Lindblad boundary sink of arbitrary strength. Tracing out the sink maps the problem onto a non-Hermitian tight-binding Hamiltonian with a rank-one imaginary defect on the semi-infinite line. We obtain closed-form expressions for the exact propagator, from which the first-passage statistics follow. Weak coupling limits absorption through inefficient transfer into the sink, whereas for strong dissipation, occupation at the boundary is stunted by the emergence of a localized non-Hermitian mode. Despite the different physical origin of these suppression mechanisms, we show their respective absorption probabilities exhibit an asymptotic duality. The evolution is conveniently visualized in phase-space, where the non-Hermitian mode produces a Wigner droplet exponentially confined near the edge site.

arXiv:2605.08056 [quant-ph]

(or arXiv:2605.08056v3 [quant-ph] for this version)

From: Francisco Riberi Mr. [view email] [v1] Fri, 8 May 2026 17:43:56 UTC (674 KB) [v2] Sun, 17 May 2026 22:11:43 UTC (678 KB) [v3] Mon, 17 Aug 2026 21:12:41 UTC (680 KB)

Full text under the publisher's open licence · 166 words

Related coverage