Asymptotic evolution of quantum walks with random coin

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

Organisationseinheiten

Forschungs-netzwerk anzeigen

Details

Originalspracheundefiniert/unbekannt
Seiten (von - bis)042201
Seitenumfang1
FachzeitschriftJ. Math. Phys.
Jahrgang52
PublikationsstatusVeröffentlicht - 2011

Abstract

We study the asymptotic position distribution of general quantum walks on a lattice, including walks with a random coin, which is chosen from step to step by a general Markov chain. In the unitary (i.e., non-random) case, we allow any unitary operator, which commutes with translations, and couples only sites at a finite distance from each other. For example, a single step of the walk could be composed of any finite succession of different shift and coin operations in the usual sense, with any lattice dimension and coin dimension. We find ballistic scaling, and establish a direct method for computing the asymptotic distribution of position divided by time, namely as the distribution of the discrete time analog of the group velocity. In the random case, we let a Markov chain (control process) pick in each step one of finitely many unitary walks, in the sense described above. In ballistic order we find a non-random drift, which depends only on the mean of the control process and not on the initial state. In diffusive scaling the limiting distribution is asymptotically Gaussian, with a covariance matrix (diffusion matrix) depending on momentum. The diffusion matrix depends not only on the mean but also on the transition rates of the control process. In the non-random limit, i.e., when the coins chosen are all very close, or the transition rates of the control process are small, leading to long intervals of ballistic evolution, the diffusion matrix diverges. Our method is based on spatial Fourier transforms, and the first and second order perturbation theory of the eigenvalue 1 of the transition operator for each value of the momentum.

Zitieren

Asymptotic evolution of quantum walks with random coin. / Ahlbrecht, Andre; Vogts, Holger; Werner, Albert H et al.
in: J. Math. Phys., Jahrgang 52, 2011, S. 042201.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Ahlbrecht A, Vogts H, Werner AH, Werner RF. Asymptotic evolution of quantum walks with random coin. J. Math. Phys. 2011;52:042201. doi: 10.1063/1.3575568
Ahlbrecht, Andre ; Vogts, Holger ; Werner, Albert H et al. / Asymptotic evolution of quantum walks with random coin. in: J. Math. Phys. 2011 ; Jahrgang 52. S. 042201.
Download
@article{4c3d19bad1bd491d92553fe91db8e97a,
title = "Asymptotic evolution of quantum walks with random coin",
abstract = "We study the asymptotic position distribution of general quantum walks on a lattice, including walks with a random coin, which is chosen from step to step by a general Markov chain. In the unitary (i.e., non-random) case, we allow any unitary operator, which commutes with translations, and couples only sites at a finite distance from each other. For example, a single step of the walk could be composed of any finite succession of different shift and coin operations in the usual sense, with any lattice dimension and coin dimension. We find ballistic scaling, and establish a direct method for computing the asymptotic distribution of position divided by time, namely as the distribution of the discrete time analog of the group velocity. In the random case, we let a Markov chain (control process) pick in each step one of finitely many unitary walks, in the sense described above. In ballistic order we find a non-random drift, which depends only on the mean of the control process and not on the initial state. In diffusive scaling the limiting distribution is asymptotically Gaussian, with a covariance matrix (diffusion matrix) depending on momentum. The diffusion matrix depends not only on the mean but also on the transition rates of the control process. In the non-random limit, i.e., when the coins chosen are all very close, or the transition rates of the control process are small, leading to long intervals of ballistic evolution, the diffusion matrix diverges. Our method is based on spatial Fourier transforms, and the first and second order perturbation theory of the eigenvalue 1 of the transition operator for each value of the momentum.",
author = "Andre Ahlbrecht and Holger Vogts and Werner, {Albert H} and Werner, {Reinhard F}",
note = "Funding information: We gratefully acknowledge the support of the DFG (Forschergruppe 635) and the EU projects CORNER, QUICS and CoQuit.",
year = "2011",
doi = "10.1063/1.3575568",
language = "Undefined/Unknown",
volume = "52",
pages = "042201",
journal = "J. Math. Phys.",
issn = "1089-7658",
publisher = "American Institute of Physics",

}

Download

TY - JOUR

T1 - Asymptotic evolution of quantum walks with random coin

AU - Ahlbrecht, Andre

AU - Vogts, Holger

AU - Werner, Albert H

AU - Werner, Reinhard F

N1 - Funding information: We gratefully acknowledge the support of the DFG (Forschergruppe 635) and the EU projects CORNER, QUICS and CoQuit.

PY - 2011

Y1 - 2011

N2 - We study the asymptotic position distribution of general quantum walks on a lattice, including walks with a random coin, which is chosen from step to step by a general Markov chain. In the unitary (i.e., non-random) case, we allow any unitary operator, which commutes with translations, and couples only sites at a finite distance from each other. For example, a single step of the walk could be composed of any finite succession of different shift and coin operations in the usual sense, with any lattice dimension and coin dimension. We find ballistic scaling, and establish a direct method for computing the asymptotic distribution of position divided by time, namely as the distribution of the discrete time analog of the group velocity. In the random case, we let a Markov chain (control process) pick in each step one of finitely many unitary walks, in the sense described above. In ballistic order we find a non-random drift, which depends only on the mean of the control process and not on the initial state. In diffusive scaling the limiting distribution is asymptotically Gaussian, with a covariance matrix (diffusion matrix) depending on momentum. The diffusion matrix depends not only on the mean but also on the transition rates of the control process. In the non-random limit, i.e., when the coins chosen are all very close, or the transition rates of the control process are small, leading to long intervals of ballistic evolution, the diffusion matrix diverges. Our method is based on spatial Fourier transforms, and the first and second order perturbation theory of the eigenvalue 1 of the transition operator for each value of the momentum.

AB - We study the asymptotic position distribution of general quantum walks on a lattice, including walks with a random coin, which is chosen from step to step by a general Markov chain. In the unitary (i.e., non-random) case, we allow any unitary operator, which commutes with translations, and couples only sites at a finite distance from each other. For example, a single step of the walk could be composed of any finite succession of different shift and coin operations in the usual sense, with any lattice dimension and coin dimension. We find ballistic scaling, and establish a direct method for computing the asymptotic distribution of position divided by time, namely as the distribution of the discrete time analog of the group velocity. In the random case, we let a Markov chain (control process) pick in each step one of finitely many unitary walks, in the sense described above. In ballistic order we find a non-random drift, which depends only on the mean of the control process and not on the initial state. In diffusive scaling the limiting distribution is asymptotically Gaussian, with a covariance matrix (diffusion matrix) depending on momentum. The diffusion matrix depends not only on the mean but also on the transition rates of the control process. In the non-random limit, i.e., when the coins chosen are all very close, or the transition rates of the control process are small, leading to long intervals of ballistic evolution, the diffusion matrix diverges. Our method is based on spatial Fourier transforms, and the first and second order perturbation theory of the eigenvalue 1 of the transition operator for each value of the momentum.

U2 - 10.1063/1.3575568

DO - 10.1063/1.3575568

M3 - Article

VL - 52

SP - 042201

JO - J. Math. Phys.

JF - J. Math. Phys.

SN - 1089-7658

ER -

Von denselben Autoren