44,210 research outputs found

    Identifying codes of corona product graphs

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    For a vertex xx of a graph GG, let NG[x]N_G[x] be the set of xx with all of its neighbors in GG. A set CC of vertices is an {\em identifying code} of GG if the sets NG[x]CN_G[x]\cap C are nonempty and distinct for all vertices xx. If GG admits an identifying code, we say that GG is identifiable and denote by γID(G)\gamma^{ID}(G) the minimum cardinality of an identifying code of GG. In this paper, we study the identifying code of the corona product HGH\odot G of graphs HH and GG. We first give a necessary and sufficient condition for the identifiable corona product HGH\odot G, and then express γID(HG)\gamma^{ID}(H\odot G) in terms of γID(G)\gamma^{ID}(G) and the (total) domination number of HH. Finally, we compute γID(HG)\gamma^{ID}(H\odot G) for some special graphs GG

    Nonequilibrium Kondo effect by equilibrium numerical renormalization group method: The hybrid Anderson model subject to a finite spin bias

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    We investigate Kondo correlations in a quantum dot with normal and superconducting electrodes, where a spin bias voltage is applied across the device and the local interaction UU is either attractive or repulsive. When the spin current is blockaded in the large-gap regime, this nonequilibrium strongly-correlated problem maps into an equilibrium model solvable by the numerical renormalization group method. The Kondo spectra with characteristic splitting due to the nonequilibrium spin accumulation are thus obtained at high precision. It is shown that while the bias-induced decoherence of the spin Kondo effect is partially compensated by the superconductivity, the charge Kondo effect is enhanced out of equilibrium and undergoes an additional splitting by the superconducting proximity effect, yielding four Kondo peaks in the local spectral density. In the charge Kondo regime, we find a universal scaling of charge conductance in this hybrid device under different spin biases. The universal conductance as a function of the coupling to the superconducting lead is peaked at and hence directly measures the Kondo temperature. Our results are of direct relevance to recent experiments realizing negative-UU charge Kondo effect in hybrid oxide quantum dots [Nat. Commun. \textbf{8}, 395 (2017)].Comment: 7 pages, 3 figures, the version accepted by Physical Review

    On the metric dimension and fractional metric dimension for hierarchical product of graphs

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    A set of vertices WW {\em resolves} a graph GG if every vertex of GG is uniquely determined by its vector of distances to the vertices in WW. The {\em metric dimension} for GG, denoted by dim(G)\dim(G), is the minimum cardinality of a resolving set of GG. In order to study the metric dimension for the hierarchical product G2u2G1u1G_2^{u_2}\sqcap G_1^{u_1} of two rooted graphs G2u2G_2^{u_2} and G1u1G_1^{u_1}, we first introduce a new parameter, the {\em rooted metric dimension} \rdim(G_1^{u_1}) for a rooted graph G1u1G_1^{u_1}. If G1G_1 is not a path with an end-vertex u1u_1, we show that \dim(G_2^{u_2}\sqcap G_1^{u_1})=|V(G_2)|\cdot\rdim(G_1^{u_1}), where V(G2)|V(G_2)| is the order of G2G_2. If G1G_1 is a path with an end-vertex u1u_1, we obtain some tight inequalities for dim(G2u2G1u1)\dim(G_2^{u_2}\sqcap G_1^{u_1}). Finally, we show that similar results hold for the fractional metric dimension.Comment: 11 page
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