458 research outputs found

    Parameters of Integral Circulant Graphs and Periodic Quantum Dynamics

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    The intention of the paper is to move a step towards a classification of network topologies that exhibit periodic quantum dynamics. We show that the evolution of a quantum system, whose hamiltonian is identical to the adjacency matrix of a circulant graph, is periodic if and only if all eigenvalues of the graph are integers (that is, the graph is integral). Motivated by this observation, we focus on relevant properties of integral circulant graphs. Specifically, we bound the number of vertices of integral circulant graphs in terms of their degree, characterize bipartiteness and give exact bounds for their diameter. Additionally, we prove that circulant graphs with odd order do not allow perfect state transfer.Comment: 12 page

    Maximal diameter of integral circulant graphs

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    Integral circulant graphs are proposed as models for quantum spin networks that permit a quantum phenomenon called perfect state transfer. Specifically, it is important to know how far information can potentially be transferred between nodes of the quantum networks modelled by integral circulant graphs and this task is related to calculating the maximal diameter of a graph. The integral circulant graph ICGn(D)ICG_n (D) has the vertex set Zn={0,1,2,,n1}Z_n = \{0, 1, 2, \ldots, n - 1\} and vertices aa and bb are adjacent if gcd(ab,n)D\gcd(a-b,n)\in D, where D{d:dn, 1d<n}D \subseteq \{d : d \mid n,\ 1\leq d<n\}. Motivated by the result on the upper bound of the diameter of ICGn(D)ICG_n(D) given in [N. Saxena, S. Severini, I. Shparlinski, \textit{Parameters of integral circulant graphs and periodic quantum dynamics}, International Journal of Quantum Information 5 (2007), 417--430], according to which 2D+12|D|+1 represents one such bound, in this paper we prove that the maximal value of the diameter of the integral circulant graph ICGn(D)ICG_n(D) of a given order nn with its prime factorization p1α1pkαkp_1^{\alpha_1}\cdots p_k^{\alpha_k}, is equal to r(n)r(n) or r(n)+1r(n)+1, where r(n)=k+{i αi>1, 1ik}r(n)=k + |\{ i \ | \alpha_i> 1,\ 1\leq i\leq k \}|, depending on whether n∉4N+2n\not\in 4N+2 or not, respectively. Furthermore, we show that, for a given order nn, a divisor set DD with Dk|D|\leq k can always be found such that this bound is attained. Finally, we calculate the maximal diameter in the class of integral circulant graphs of a given order nn and cardinality of the divisor set tkt\leq k and characterize all extremal graphs. We actually show that the maximal diameter can have the values 2t2t, 2t+12t+1, r(n)r(n) and r(n)+1r(n)+1 depending on the values of tt and nn. This way we further improve the upper bound of Saxena, Severini and Shparlinski and we also characterize all graphs whose diameters are equal to 2D+12|D|+1, thus generalizing a result in that paper.Comment: 29 pages, 1 figur

    Perfect state transfer, graph products and equitable partitions

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    We describe new constructions of graphs which exhibit perfect state transfer on continuous-time quantum walks. Our constructions are based on variants of the double cones [BCMS09,ANOPRT10,ANOPRT09] and the Cartesian graph products (which includes the n-cube) [CDDEKL05]. Some of our results include: (1) If GG is a graph with perfect state transfer at time tGt_{G}, where t_{G}\Spec(G) \subseteq \ZZ\pi, and HH is a circulant with odd eigenvalues, their weak product G×HG \times H has perfect state transfer. Also, if HH is a regular graph with perfect state transfer at time tHt_{H} and GG is a graph where t_{H}|V_{H}|\Spec(G) \subseteq 2\ZZ\pi, their lexicographic product G[H]G[H] has perfect state transfer. (2) The double cone K2+G\overline{K}_{2} + G on any connected graph GG, has perfect state transfer if the weights of the cone edges are proportional to the Perron eigenvector of GG. This generalizes results for double cone on regular graphs studied in [BCMS09,ANOPRT10,ANOPRT09]. (3) For an infinite family \GG of regular graphs, there is a circulant connection so the graph K_{1}+\GG\circ\GG+K_{1} has perfect state transfer. In contrast, no perfect state transfer exists if a complete bipartite connection is used (even in the presence of weights) [ANOPRT09]. We also describe a generalization of the path collapsing argument [CCDFGS03,CDDEKL05], which reduces questions about perfect state transfer to simpler (weighted) multigraphs, for graphs with equitable distance partitions.Comment: 18 pages, 6 figure
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