2015
DOI: 10.1007/s11128-015-1150-6
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Fast clique minor generation in Chimera qubit connectivity graphs

Abstract: The current generation of D-Wave quantum annealing processor is designed to minimize the energy of an Ising spin configuration whose pairwise interactions lie on the edges of a Chimera graph C M,N,L . In order to solve an Ising spin problem with arbitrary pairwise interaction structure, the corresponding graph must be minor-embedded into a Chimera graph. We define a combinatorial class of native clique minors in Chimera graphs with vertex images of uniform, near minimal size, and provide a polynomial-time algo… Show more

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Cited by 141 publications
(149 citation statements)
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“…One aspect which could be explored in statics and dynamics is the extension to two or higher dimensional systems which we have excluded due to the limitation of MPS algorithms to one spatial dimension for studies of this kind. Two-dimensional setups allow more options for quantum computation to apply gates [48]. In the case of the antiferromagnetic case triangular lattices can lead to the similar concurrence of the staggered order than for long-range interactions in the onedimensional case.…”
Section: Conclusion and Open Questionsmentioning
confidence: 99%
“…One aspect which could be explored in statics and dynamics is the extension to two or higher dimensional systems which we have excluded due to the limitation of MPS algorithms to one spatial dimension for studies of this kind. Two-dimensional setups allow more options for quantum computation to apply gates [48]. In the case of the antiferromagnetic case triangular lattices can lead to the similar concurrence of the staggered order than for long-range interactions in the onedimensional case.…”
Section: Conclusion and Open Questionsmentioning
confidence: 99%
“…In practice, we add an element x n+1 to the Q matrix that is strongly coupled to any node i with the following elements modified based on the value of penalty term M. Figure 4 provides an example of the changes made when adding node 6 that is strongly coupled to node 1. 1 2 3 4 5 1 2 3 4 5 6 1 5 2 2 2 2 1 -45 2 2 100 2 8 2 2 2 8 2 2 3 3 3 Future work will investigate the application of Rules 1-5 in conjunction with strong coupling in order to transform a given graph to one that meets a target graph's node and edge specifications [5].…”
Section: Graph Expansion Via Strongly Coupled Nodesmentioning
confidence: 99%
“…Considering this order statistic, and the fact that QuAMax considers only the best solution found by all the anneals in a run, the expected BER of instance I after N a anneals can be expressed as (9) where N is qubit count, L (≤ N a ) is the number of distinct solutions, r (1 ≤ r ≤ L) is the rank index of each solution, p(r ) is the probability of obtaining the r th solution, and F I (k) is the number of bit errors of the k th solution against ground truth. 7 To calculate TTB(p), we replace the left hand side of Eq. 9 with p, solve for N a , and compute TTB(p) = N a T a /P f .…”
Section: Ourmentioning
confidence: 99%