Alana Spak dos Santos

arXiv2026

Discrete-time quantum walks with energy-dependent coins

In this work, we extend the scattering quantum walk (SQW) framework to a lattice of energy-dependent point interactions. This yields, within the coined quantum walk (CQW) formalism, a coin operator that is directly related to the scattering matrix of zero-range potentials. The model thus provides a discrete-time quantum-walk (DTQW) analog of a periodic array of point interactions of the Kronig-Penney type, where the walker's wavenumber serves as a continuous, physically transparent control parameter for the coin operation. We analyze the spectra and the dynamics of position probability and entanglement, yielding distinct results for specific energies and point interactions. We relate the spectral structure to the spatial probability distribution and explicitly characterize the long-time entanglement behavior for each point interaction. The transmission modulus determines the quasienergy gap, bandwidth, and maximum group velocity, while also controlling the long-time coin-position entanglement for the initial state considered. The four families of one-dimensional point interactions ($δ$, $δ'$, crossed and asymmetric) realize qualitatively distinct transmission profiles and span the full range of behavior, including enhanced or strongly suppressed spreading and oscillatory entanglement.

quant-ph↗

arXiv2026

Energy-space quantum walks: Thermalization without state convergence

We introduce energy-space quantum walks as a minimal framework to investigate equilibration, thermalization, and irreversibility from an effective-dynamics perspective. By mapping the configuration space of a walk onto a ladder of energy eigenlevels, we reinterpret thermalization as transport in energy space, independently of microscopic system--bath details. At the classical level, the resulting birth--death--lazy dynamics leads to equilibration of the energy distribution and, under suitable conditions, to a Gibbs stationary state. We then embed this dynamics into a unitary, collision-assisted model in which coherence is controlled by a single parameter. A central result is a structural decoupling between population dynamics and coherence generation: while the populations evolve according to the classical process and relax to the Gibbs distribution, the full quantum state exhibits a persistent coherence-induced deviation from the thermal manifold. This establishes a minimal scenario of thermalization without state convergence, where equilibration occurs at the level of populations but not at the level of the full density operator. We quantify this effect using the thermal distance to the Gibbs state and derive perturbative bounds that relate the long-time deviation to classical transport properties. Our results show that coherence acts as a controllable and quantitatively bounded source of nonthermal behavior, providing a clear separation between classical equilibration and genuinely quantum corrections.

quant-ph↗