Restart and first detection in a lackadaisical quantum walk with flat-band localization
Abstract
We study stochastic and sharp restart in a one-dimensional lackadaisical discrete-time quantum walk with self-loop weight $\ell$. In the absence of restart, the dynamics has a flat band responsible for intrinsic localization and two dispersive bands supporting ballistic propagation. We compare two initially localized benchmark states: a flat-band-active state with finite flat-band overlap and a flat-band-dark state with zero flat-band overlap. For geometric stochastic restart with per-step resta...
Description / Details
We study stochastic and sharp restart in a one-dimensional lackadaisical discrete-time quantum walk with self-loop weight . In the absence of restart, the dynamics has a flat band responsible for intrinsic localization and two dispersive bands supporting ballistic propagation. We compare two initially localized benchmark states: a flat-band-active state with finite flat-band overlap and a flat-band-dark state with zero flat-band overlap. For geometric stochastic restart with per-step restart probability , the stationary mean-squared displacement scales as as . In the same limit, the restart-site occupation probability approaches the restart-free intrinsic localized value for the flat-band-active state, whereas for the flat-band-dark state it vanishes as . For power-law restart, where is the probability that the waiting time to the next restart is steps, a normalized stationary site-occupation distribution exists only for , while the stationary absolute spatial moment of order is finite only for . In the regime , at every fixed lattice site, the flat-band-active occupation converges to the intrinsic flat-band profile, while the flat-band-dark occupation tends to zero. We also consider monitored first detection with sharp restart, in which the walk is reinitialized after a fixed number of consecutive unsuccessful measurements. For fixed , the mean first-detected-passage time of the flat-band-active state exhibits a minimum at an intermediate self-loop weight, whereas the flat-band-dark state approaches a ballistic detection limit as .
Source: arXiv:2609.08973v1 - http://arxiv.org/abs/2609.08973v1 PDF: https://arxiv.org/pdf/2609.08973v1 Original Link: http://arxiv.org/abs/2609.08973v1
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Sep 9, 2026
Quantum Computing
Quantum Physics
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