16 research outputs found

    The isoperimetric constant of the random graph process

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    The isoperimetric constant of a graph GG on nn vertices, i(G)i(G), is the minimum of SS\frac{|\partial S|}{|S|}, taken over all nonempty subsets SV(G)S\subset V(G) of size at most n/2n/2, where S\partial S denotes the set of edges with precisely one end in SS. A random graph process on nn vertices, G~(t)\widetilde{G}(t), is a sequence of (n2)\binom{n}{2} graphs, where G~(0)\widetilde{G}(0) is the edgeless graph on nn vertices, and G~(t)\widetilde{G}(t) is the result of adding an edge to G~(t1)\widetilde{G}(t-1), uniformly distributed over all the missing edges. We show that in almost every graph process i(G~(t))i(\widetilde{G}(t)) equals the minimal degree of G~(t)\widetilde{G}(t) as long as the minimal degree is o(logn)o(\log n). Furthermore, we show that this result is essentially best possible, by demonstrating that along the period in which the minimum degree is typically Θ(logn)\Theta(\log n), the ratio between the isoperimetric constant and the minimum degree falls from 1 to 1/2, its final value

    Entanglement bounds on the performance of quantum computing architectures

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    There are many possible architectures of qubit connectivity that designers of future quantum computers will need to choose between. However, the process of evaluating a particular connectivity graph's performance as a quantum architecture can be difficult. In this paper, we show that a quantity known as the isoperimetric number establishes a lower bound on the time required to create highly entangled states. This metric we propose counts resources based on the use of two-qubit unitary operations, while allowing for arbitrarily fast measurements and classical feedback. We use this metric to evaluate the hierarchical architecture proposed by A. Bapat et al. [Phys. Rev. A 98, 062328 (2018)], and find it to be a promising alternative to the conventional grid architecture. We also show that the lower bound that this metric places on the creation time of highly entangled states can be saturated with a constructive protocol, up to a factor logarithmic in the number of qubits.Comment: 9 pages, 5 figures, 1 table (journal version

    Improved Mixing for the Convex Polygon Triangulation Flip Walk

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    Theories and Inequalities on the Satellite System

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    Isoperimetric Inequalities and Supercritical Percolation on High-dimensional Graphs

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    It is known that many different types of finite random subgraph models undergo quantitatively similar phase transitions around their percolation thresholds, and the proofs of these results rely on isoperimetric properties of the underlying host graph. Recently, the authors showed that such a phase transition occurs in a large class of regular high-dimensional product graphs, generalising a classic result for the hypercube. In this paper we give new isoperimetric inequalities for such regular high-dimensional product graphs, which generalise the well-known isoperimetric inequality of Harper for the hypercube, and are asymptotically sharp for a wide range of set sizes. We then use these isoperimetric properties to investigate the structure of the giant component L1L_1 in supercritical percolation on these product graphs, that is, when p=1+ϵdp=\frac{1+\epsilon}{d}, where dd is the degree of the product graph and ϵ>0\epsilon>0 is a small enough constant. We show that typically L1L_1 has edge-expansion Ω(1dlnd)\Omega\left(\frac{1}{d\ln d}\right). Furthermore, we show that L1L_1 likely contains a linear-sized subgraph with vertex-expansion Ω(1dlnd)\Omega\left(\frac{1}{d\ln d}\right). These results are best possible up to the logarithmic factor in dd. Using these likely expansion properties, we determine, up to small polylogarithmic factors in dd, the likely diameter of L1L_1 as well as the typical mixing time of a lazy random walk on L1L_1. Furthermore, we show the likely existence of a path of length Ω(ndlnd)\Omega\left(\frac{n}{d\ln d}\right). These results not only generalise, but also improve substantially upon the known bounds in the case of the hypercube, where in particular the likely diameter and typical mixing time of L1L_1 were previously only known to be polynomial in dd
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