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Entanglement Theory Quantum Correlations
Quantum Simulation
Universal State Transfer on Graphs
arXiv
Authors: Stephen Cameron, Shannon Fehrenbach, Leah Granger, Oliver Hennigh, Sunrose Shrestha, Christino Tamon
Year
2013
Paper ID
32244
Status
Preprint
Abstract Read
~2 min
Abstract Words
259
Citations
N/A
Abstract
A continuous-time quantum walk on a graph G is given by the unitary matrix U(t) = exp(-itA), where A is the Hermitian adjacency matrix of G. We say G has pretty good state transfer between vertices a and b if for any ε> 0, there is a time t, where the (a,b)-entry of U(t) satisfies |U(t)a,b| ge 1-ε. This notion was introduced by Godsil (2011). The state transfer is perfect if the above holds for ε= 0. In this work, we study a natural extension of this notion called universal state transfer. Here, state transfer exists between every pair of vertices of the graph. We prove the following results about graphs with this stronger property: (1) Graphs with universal state transfer have distinct eigenvalues and flat eigenbasis (where each eigenvector has entries which are equal in magnitude). (2) The switching automorphism group of a graph with universal state transfer is abelian and its order divides the size of the graph. Moreover, if the state transfer is perfect, then the switching automorphism group is cyclic. (3) There is a family of prime-length cycles with complex weights which has universal pretty good state transfer. This provides a concrete example of an infinite family of graphs with the universal property. (4) There exists a class of graphs with real symmetric adjacency matrices which has universal pretty good state transfer. In contrast, Kay (2011) proved that no graph with real-valued adjacency matrix can have universal perfect state transfer. We also provide a spectral characterization of universal perfect state transfer graphs that are switching equivalent to circulants.
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- This paper contributes to the Quantum Simulation research area in the Quantum Articles archive.
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- A continuous-time quantum walk on a graph G is given by the unitary matrix U(t) = exp(-itA), where A is the Hermitian adjacency matrix of G.
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