Quantum walk: Difference between revisions
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[[Image:One_dimensional_quantum_random_walk.png|thumb|right|A one dimensional quantum random walk created using the Hadamard coin.]] |
[[Image:One_dimensional_quantum_random_walk.png|thumb|right|A one dimensional quantum random walk created using the Hadamard coin is plotted (red) vs a classical walk (blue).]] |
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A quantum walk in discrete time is specified a coin and shift operator. |
A quantum walk in discrete time is specified a coin and shift operator. |
Revision as of 11:46, 28 November 2008
Quantum random walks are quantum mechanical extension of classical random walks where the walker may be in a superposition of positions. Quantum walks exhibit very different features from classical random walks. In particular, they do not converge to limiting distributions and due to the power of quantum interference they may spread significantly faster or slower than their classical equivalents. They are largely of interest as source for quantum algorithms.
Continuous time
Label the vertexes of arbitrary graph as independent quantum states. Then a quantum walk in continuous time is specified by using the adjacency matrix for the graph as a Hamiltonian, so time evolution is specified by the unitary operator in non-dimensionalized units.
Discrete time
A quantum walk in discrete time is specified a coin and shift operator.
References
- Andris Ambainis (2003). "Quantum walks and their algorithmic applications". International Journal of Quantum Information. 1: 507–518.
- Julia Kempe (2003). "Quantum random walks &ndash an introductory overview". Contemporary Physics. 44: 307–327.