86,247 research outputs found

    Resolved-sideband laser cooling in a penning trap

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    We report the laser cooling of a single 40Ca+^{40}\text{Ca}^+ ion in a Penning trap to the motional ground state in one dimension. Cooling is performed in the strong binding limit on the 729-nm electric quadrupole S1/2↔D5/2S_{1/2}\leftrightarrow D_{5/2} transition, broadened by a quench laser coupling the D5/2D_{5/2} and P3/2P_{3/2} levels. We find the final ground state occupation to be 98±1%98\pm1\%. We measure the heating rate of the trap to be very low with nˉ˙≈0.3±0.2s−1\dot{\bar{n}}\approx 0.3\pm0.2\textrm{s}^{-1} for trap frequencies from 150−400kHz150-400\textrm{kHz}, consistent with the large ion-electrode distance.Comment: 4 pages, 6 figures. Accepted: Phys. Rev. Lett. (2016) http://journals.aps.org/prl/accepted/b6074YefH1115b5881f77975417a6ae0bc9f652a

    Simulation of subseismic joint and fault networks using a heuristic mechanical model

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    Flow simulations of fractured and faulted reservoirs require representation of subseismic structures about which subsurface data are limited. We describe a method for simulating fracture growth that is mechanically based but heuristic, allowing for realistic modelling of fracture networks with reasonable run times. The method takes a triangulated meshed surface as input, together with an initial stress field. Fractures initiate and grow based on the stress field, and the growing fractures relieve the stress in the mesh. We show that a wide range of bedding-plane joint networks can be modelled simply by varying the distribution and anisotropy of the initial stress field. The results are in good qualitative agreement with natural joint patterns. We then apply the method to a set of parallel veins and demonstrate how the variations in thickness of the veins can be represented. Lastly, we apply the method to the simulation of normal fault patterns on salt domes. We derive the stress field on the bedding surface using the horizon curvature. The modelled fault network shows both radial and concentric faults. The new method provides an effective means of modelling joint and fault networks that can be imported to the flow simulator

    Towards pp -> VVjj at NLO QCD: Bosonic contributions to triple vector boson production plus jet

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    In this work, some of the NLO QCD corrections for pp -> VVjj + X are presented. A program in Mathematica based on the structure of FeynCalc which automatically simplifies a set of amplitudes up to the hexagon level of rank 5 has been created for this purpose. We focus on two different topologies. The first involves all the virtual contributions needed for quadruple electroweak vector boson production, i.e. pp -> VVVV + X. In the second, the remaining "bosonic" corrections to electroweak triple vector boson production with an additional jet (pp -> VVV j + X) are computed. We show the factorization formula of the infrared divergences of the bosonic contributions for VVVV and VVVj production with V=(W,Z,gamma). Stability issues associated with the evaluation of the hexagons up to rank 5 are studied. The CPU time of the FORTRAN subroutines rounds the 2 milliseconds and seems to be competitive with other more sophisticated methods. Additionally, in Appendix A the master equations to obtain the tensor coefficients up to the hexagon level in the external momenta convention are presented including the ones needed for small Gram determinants.Comment: 48 pages,16 figure

    Why the Tsirelson bound?

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    Wheeler's question 'why the quantum' has two aspects: why is the world quantum and not classical, and why is it quantum rather than superquantum, i.e., why the Tsirelson bound for quantum correlations? I discuss a remarkable answer to this question proposed by Pawlowski et al (2009), who provide an information-theoretic derivation of the Tsirelson bound from a principle they call 'information causality.'Comment: 17 page

    Hamilton-Jacobi Theory and Information Geometry

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    Recently, a method to dynamically define a divergence function DD for a given statistical manifold (M ,g ,T)(\mathcal{M}\,,g\,,T) by means of the Hamilton-Jacobi theory associated with a suitable Lagrangian function L\mathfrak{L} on TMT\mathcal{M} has been proposed. Here we will review this construction and lay the basis for an inverse problem where we assume the divergence function DD to be known and we look for a Lagrangian function L\mathfrak{L} for which DD is a complete solution of the associated Hamilton-Jacobi theory. To apply these ideas to quantum systems, we have to replace probability distributions with probability amplitudes.Comment: 8 page

    A fluid model for closed queueing networks with PS stations

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    This technical report introduces a closed multi-class queueing network (QN) model with class-switching, where the service rates are de ned to represent multi-processor stations with a processor-sharing (PS) allocation policy. These transition rates are also able to consider traditional delay nodes, and therefore a QN model with these transition rates is well-suited for multi-threaded software applications. In this report, we de ne the QN model and use the results in [1] to show that the transient sample paths of the QN model converge to the solution of a system of ordinary di erential equations (ODEs). As the size of the ODE system grows linearly with the number of stations and job classes in the QN model, solving the ODE system becomes a scalable alternative to Markov chain representations
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