6,210 research outputs found

    Universal quantum computation with unlabeled qubits

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    We show that an n-th root of the Walsh-Hadamard transform (obtained from the Hadamard gate and a cyclic permutation of the qubits), together with two diagonal matrices, namely a local qubit-flip (for a fixed but arbitrary qubit) and a non-local phase-flip (for a fixed but arbitrary coefficient), can do universal quantum computation on n qubits. A quantum computation, making use of n qubits and based on these operations, is then a word of variable length, but whose letters are always taken from an alphabet of cardinality three. Therefore, in contrast with other universal sets, no choice of qubit lines is needed for the application of the operations described here. A quantum algorithm based on this set can be interpreted as a discrete diffusion of a quantum particle on a de Bruijn graph, corrected on-the-fly by auxiliary modifications of the phases associated to the arcs.Comment: 6 page

    Regular quantum graphs

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    We introduce the concept of regular quantum graphs and construct connected quantum graphs with discrete symmetries. The method is based on a decomposition of the quantum propagator in terms of permutation matrices which control the way incoming and outgoing channels at vertex scattering processes are connected. Symmetry properties of the quantum graph as well as its spectral statistics depend on the particular choice of permutation matrices, also called connectivity matrices, and can now be easily controlled. The method may find applications in the study of quantum random walks networks and may also prove to be useful in analysing universality in spectral statistics.Comment: 12 pages, 3 figure

    Matrix permanent and quantum entanglement of permutation invariant states

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    We point out that a geometric measure of quantum entanglement is related to the matrix permanent when restricted to permutation invariant states. This connection allows us to interpret the permanent as an angle between vectors. By employing a recently introduced permanent inequality by Carlen, Loss and Lieb, we can prove explicit formulas of the geometric measure for permutation invariant basis states in a simple way.Comment: 10 page

    A Comparison between the Zero Forcing Number and the Strong Metric Dimension of Graphs

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    The \emph{zero forcing number}, Z(G)Z(G), of a graph GG is the minimum cardinality of a set SS of black vertices (whereas vertices in V(G)SV(G)-S are colored white) such that V(G)V(G) is turned black after finitely many applications of "the color-change rule": a white vertex is converted black if it is the only white neighbor of a black vertex. The \emph{strong metric dimension}, sdim(G)sdim(G), of a graph GG is the minimum among cardinalities of all strong resolving sets: WV(G)W \subseteq V(G) is a \emph{strong resolving set} of GG if for any u,vV(G)u, v \in V(G), there exists an xWx \in W such that either uu lies on an xvx-v geodesic or vv lies on an xux-u geodesic. In this paper, we prove that Z(G)sdim(G)+3r(G)Z(G) \le sdim(G)+3r(G) for a connected graph GG, where r(G)r(G) is the cycle rank of GG. Further, we prove the sharp bound Z(G)sdim(G)Z(G) \leq sdim(G) when GG is a tree or a unicyclic graph, and we characterize trees TT attaining Z(T)=sdim(T)Z(T)=sdim(T). It is easy to see that sdim(T+e)sdim(T)sdim(T+e)-sdim(T) can be arbitrarily large for a tree TT; we prove that sdim(T+e)sdim(T)2sdim(T+e) \ge sdim(T)-2 and show that the bound is sharp.Comment: 8 pages, 5 figure

    Performance of an Operating High Energy Physics Data Grid: D0SAR-Grid

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    The D0 experiment at Fermilab's Tevatron will record several petabytes of data over the next five years in pursuing the goals of understanding nature and searching for the origin of mass. Computing resources required to analyze these data far exceed capabilities of any one institution. Moreover, the widely scattered geographical distribution of D0 collaborators poses further serious difficulties for optimal use of human and computing resources. These difficulties will exacerbate in future high energy physics experiments, like the LHC. The computing grid has long been recognized as a solution to these problems. This technology is being made a more immediate reality to end users in D0 by developing a grid in the D0 Southern Analysis Region (D0SAR), D0SAR-Grid, using all available resources within it and a home-grown local task manager, McFarm. We will present the architecture in which the D0SAR-Grid is implemented, the use of technology and the functionality of the grid, and the experience from operating the grid in simulation, reprocessing and data analyses for a currently running HEP experiment.Comment: 3 pages, no figures, conference proceedings of DPF04 tal

    A quantum Bose-Hubbard model with evolving graph as toy model for emergent spacetime

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    We present a toy model for interacting matter and geometry that explores quantum dynamics in a spin system as a precursor to a quantum theory of gravity. The model has no a priori geometric properties, instead, locality is inferred from the more fundamental notion of interaction between the matter degrees of freedom. The interaction terms are themselves quantum degrees of freedom so that the structure of interactions and hence the resulting local and causal structures are dynamical. The system is a Hubbard model where the graph of the interactions is a set of quantum evolving variables. We show entanglement between spatial and matter degrees of freedom. We study numerically the quantum system and analyze its entanglement dynamics. We analyze the asymptotic behavior of the classical model. Finally, we discuss analogues of trapped surfaces and gravitational attraction in this simple model.Comment: 23 pages, 6 figures; updated to published versio

    Multi-core job submission and grid resource scheduling for ATLAS AthenaMP

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    AthenaMP is the multi-core implementation of the ATLAS software framework and allows the efficient sharing of memory pages between multiple threads of execution. This has now been validated for production and delivers a significant reduction on the overall application memory footprint with negligible CPU overhead. Before AthenaMP can be routinely run on the LHC Computing Grid it must be determined how the computing resources available to ATLAS can best exploit the notable improvements delivered by switching to this multi-process model. A study into the effectiveness and scalability of AthenaMP in a production environment will be presented. Best practices for configuring the main LRMS implementations currently used by grid sites will be identified in the context of multi-core scheduling optimisation
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