Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:quant-ph/9906107 · Journal of Physics A Mathematical and General

Unravelling quantum carpets: a travelling-wave approach

Michael J. W. Hall, Martina S. Reineker, Wolfgang P. Schleich

Published Nov 11, 1999• 33 citations
arXivHTMLPDF

Abstract

Generic channel and ridge structures are known to appear in the time-dependent position probability distribution of a one-dimensional quantum particle confined to a box. These structures are shown to have a detailed quantitative explanation in terms of a travelling-wave decomposition of the probability density, wherein each contributing term corresponds simultaneously to (i) a real wave propagating at a quantized velocity and (ii) to the time-averaged structure of the position distribution along a quantized direction in spacetime. The approach leads to new predictions of channel locations, widths and depths, and is able to provide more structural details than earlier approaches based on partial interference and Wigner functions. Results are also applicable to light diffracted by a periodic grating, and to the quantum rigid rotator.

DOI
10.1088/0305-4470/32/47/307

Related papers

The Particle in the box: Intermode traces in the propagator

Irene Marzoli, Iwo Białynicki‐Birula, O. M. Friesch +2 more

Characteristic structures such as canals and ridges --intermode traces-- emerge in the spacetime representation of the probability distribution of a particle in a one-dimensional box. We show that the corresponding propagator already contains these structures. We relate their visibility to the factorization property of the initial wave packet.

arXiv:quant-ph/9804015•Apr 6, 1998•6 citations

Das Teilchen im Kasten: Strukturen in der Wahrscheinlichkeitsdichte / The Particle in a Box : Structures in the Probability

P. Stifter, C. Leichtie, Wolfgang P. Schleich +1 more

Abstract Recently W. Kinzel found characteristic structures, e. g. canals and ridges, in the contour plot of the quantum probability density of a particle moving in a box with infinitely high walls. Using the Wigner function we provide an analytical explanation of this numerical observation. Moreover we demonstrate that similar space-time structures also appear in other potentials, such as the one governing the vibrational motion of a diatomic molecule.

Zeitschrift für Naturforschung A•May 1, 1997•31 citations

Quantum carpets and Wigner functions

Irene Marzoli, O. M. Friesch, W. P. Schleich

A particle confined to an infinitely deep potential well is the ideal toy model for studying the origin of the regular patterns appearing for many physical systems in the spacetime representation of the probability density. The Wigner function is a useful tool to bring out the role of interference in the formation of these so-called "quantum carpets".

•Jan 1, 1998•1 citation

Quantum carpets: a tool to observe decoherence

P Kazemi, S. Chaturvedi, Irene Marzoli +2 more

Quantum carpets—the spatio-temporal de Broglie density profiles—woven by an atom or an electron in the near-field region of a diffraction grating bring to light, in real time, the decoherence of each individual component of the interference term of the Wigner function characteristic of superposition states. The proposed experiments are feasible with present-day technology.

New Journal of Physics•Jan 21, 2013•24 citations

Fermionic quantum carpets: From canals and ridges to solitonlike structures

Piotr T. Grochowski, Tomasz Karpiuk, Mirosław Brewczyk +1 more

Quantum carpets are spatiotemporal representations of the probability density of a quantum particle in a box. They stand out due to the characteristic structures, called canals and ridges. The authors show that these structures become much more pronounced in fermionic systems

arXiv:1811.05867•Physical Review Research•Feb 4, 2020•8 citations

Spacetime structures of continuous-time quantum walks

Oliver Mülken, A. Blumen

The propagation by continuous-time quantum walks (CTQWs) on one-dimensional lattices shows structures in the transition probabilities between different sites reminiscent of quantum carpets. For a system with periodic boundary conditions, we calculate the transition probabilities for a CTQW by diagonalizing the transfer matrix and by a Bloch function ansatz. Remarkably, the results obtained for the Bloch function ansatz can be related to results from (discrete) generalized coined quantum walks. Furthermore, we show that here the first revival time turns out to be larger than for quantum carpets.

arXiv:quant-ph/0502004•Physical Review E•Mar 22, 2005•68 citations
Generic channel and ridge structures are known to appear in the time-dependent position probability distribution of a one-dimensional quantum particle confined to a box. These structures are shown to have a detailed quantitative explanation in terms of a travelling-wave decomposition of the probability density, wherein each contributing term corresponds simultaneously to (i) a real wave propagating at a quantized velocity and (ii) to the time-averaged structure of the position distribution along a quantized direction in spacetime. The approach leads to new predictions of channel locations, widths and depths, and is able to provide more structural details than earlier approaches based on partial interference and Wigner functions. Results are also applicable to light diffracted by a periodic grating, and to the quantum rigid rotator.
The propagation by continuous-time quantum walks (CTQWs) on one-dimensional lattices shows structures in the transition probabilities between different sites reminiscent of quantum carpets. For a system with periodic boundary conditions, we calculate the transition probabilities for a CTQW by diagonalizing the transfer matrix and by a Bloch function ansatz. Remarkably, the results obtained for the Bloch function ansatz can be related to results from (discrete) generalized coined quantum walks. Furthermore, we show that here the first revival time turns out to be larger than for quantum carpets.