On training a classifier of hitting times for quantum walks

Quantum walks with infinite hitting times

Physical Review A ◽

10.1103/physreva.74.042334 ◽

2006 ◽

Vol 74 (4) ◽

Cited By ~ 43

Author(s):

Hari Krovi ◽

Todd A. Brun

Keyword(s):

Quantum Walks ◽

Hitting Times

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A simulator for discrete quantum walks on lattices

International Journal of Modern Physics C ◽

10.1142/s0129183117500553 ◽

2017 ◽

Vol 28 (04) ◽

pp. 1750055

Author(s):

J. Rodrigues ◽

N. Paunković ◽

P. Mateus

Keyword(s):

Average Distance ◽

Joint Probability ◽

Quantum Walks ◽

Hitting Times ◽

Joint Probability Distribution ◽

Two Dimensional ◽

Line Lattice ◽

Various Boundary Conditions ◽

Open Circular ◽

Particle Localization

In this paper, we present a simulator for two-particle quantum walks on the line and one-particle on a two-dimensional squared lattice. It can be used to investigate the equivalence between the two cases (one- and two-particle walks) for various boundary conditions (open, circular, reflecting, absorbing and their combinations). For the case of a single walker on a two-dimensional lattice, the simulator can also implement the Möbius strip. Furthermore, other topologies for the walker are also simulated by the proposed tool, like certain types of planar graphs with degree up to 4, by considering missing links over the lattice. The main purpose of the simulator is to study the genuinely quantum effects on the global properties of the two-particle joint probability distribution on the entanglement between the walkers/axis. For that purpose, the simulator is designed to compute various quantities such as: the entanglement and classical correlations, (classical and quantum) mutual information, the average distance between the two walkers, different hitting times and quantum discord. These quantities are of vital importance in designing possible algorithmic applications of quantum walks, namely in search, 3-SAT problems, etc. The simulator can also implement the static partial measurements of particle(s) positions and dynamic breaking of the links between certain nodes, both of which can be used to investigate the effects of decoherence on the walker(s). Finally, the simulator can be used to investigate the dynamic Anderson-like particle localization by varying the coin operators of certain nodes on the line/lattice. We also present some illustrative and relevant examples of one- and two-particle quantum walks in various scenarios. The tool was implemented in C and is available on-line at http://qwsim.weebly.com/ .

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Improved upper bounds for the hitting times of quantum walks

Physical Review A ◽

10.1103/physreva.104.032215 ◽

2021 ◽

Vol 104 (3) ◽

Author(s):

Yosi Atia ◽

Shantanav Chakraborty

Keyword(s):

Upper Bounds ◽

Quantum Walks ◽

Hitting Times

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Hitting statistics from quantum jumps

Quantum ◽

10.22331/q-2017-07-21-19 ◽

2017 ◽

Vol 1 ◽

pp. 19

Author(s):

A. Chia ◽

T. Paterek ◽

L. C. Kwek

Keyword(s):

Discrete Time ◽

Continuous Time ◽

Quantum Walks ◽

Hitting Time ◽

Hitting Times ◽

Unitary Evolution ◽

Quantum Jumps ◽

Quantum Jump ◽

Open Quantum ◽

Starting Point

We define the hitting time for a model of continuous-time open quantum walks in terms of quantum jumps. Our starting point is a master equation in Lindblad form, which can be taken as the quantum analogue of the rate equation for a classical continuous-time Markov chain. The quantum jump method is well known in the quantum optics community and has also been applied to simulate open quantum walks in discrete time. This method however, is well-suited to continuous-time problems. It is shown here that a continuous-time hitting problem is amenable to analysis via quantum jumps: The hitting time can be defined as the time of the first jump. Using this fact, we derive the distribution of hitting times and explicit exressions for its statistical moments. Simple examples are considered to illustrate the final results. We then show that the hitting statistics obtained via quantum jumps is consistent with a previous definition for a measured walk in discrete time [Phys. Rev. A 73, 032341 (2006)] (when generalised to allow for non-unitary evolution and in the limit of small time steps). A caveat of the quantum-jump approach is that it relies on the final state (the state which we want to hit) to share only incoherent edges with other vertices in the graph. We propose a simple remedy to restore the applicability of quantum jumps when this is not the case and show that the hitting-time statistics will again converge to that obtained from the measured discrete walk in appropriate limits.

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