12,358 research outputs found

    Making electromagnetic wavelets

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    Electromagnetic wavelets are constructed using scalar wavelets as superpotentials, together with an appropriate polarization. It is shown that oblate spheroidal antennas, which are ideal for their production and reception, can be made by deforming and merging two branch cuts. This determines a unique field on the interior of the spheroid which gives the boundary conditions for the surface charge-current density necessary to radiate the wavelets. These sources are computed, including the impulse response of the antenna.Comment: 29 pages, 4 figures; minor corrections and addition

    Chiral π\pi-exchange NN-potentials: Results for diagrams proportional to g_A^4 and g_A^6

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    We calculate in (two-loop) chiral perturbation theory the local NN-potentials generated by the three-pion exchange diagrams proportional to g_A^4 and g_A^6. Surprisingly, we find that the total isoscalar central 3π3\pi-exchange potential vanishes identically. The individually largest 3π3\pi-exchange potentials are of isoscalar spin-spin, isovector central and isoscalar tensor type. For these potentials simple analytical expressions can be given. The strength of these dominant 3π3\pi-exchange potentials at r=1.0 fm is 4.6 MeV, 2.9 MeV and 1.4 MeV, respectively. Furthermore, we observe that the spin-spin and tensor potentials due to the diagrams proportional to g_A^6 do not exist in the infinite nucleon mass limit.Comment: 8 pages, 5 figure

    Violation of the Leggett-Garg Inequality in Neutrino Oscillations

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    The Leggett-Garg inequality, an analogue of Bell's inequality involving correlations of measurements on a system at different times, stands as one of the hallmark tests of quantum mechanics against classical predictions. The phenomenon of neutrino oscillations should adhere to quantum-mechanical predictions and provide an observable violation of the Leggett-Garg inequality. We demonstrate how oscillation phenomena can be used to test for violations of the classical bound by performing measurements on an ensemble of neutrinos at distinct energies, as opposed to a single neutrino at distinct times. A study of the MINOS experiment's data shows a greater than 6σ6{\sigma} violation over a distance of 735 km, representing the longest distance over which either the Leggett-Garg inequality or Bell's inequality has been tested.Comment: Updated to match published version. 6 pages, 2 figure

    Exact calculation of three-body contact interaction to second order

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    For a system of fermions with a three-body contact interaction the second-order contributions to the energy per particle Eˉ(kf)\bar E(k_f) are calculated exactly. The three-particle scattering amplitude in the medium is derived in closed analytical form from the corresponding two-loop rescattering diagram. We compare the (genuine) second-order three-body contribution to Eˉ(kf)kf10\bar E(k_f)\sim k_f^{10} with the second-order term due to the density-dependent effective two-body interaction, and find that the latter term dominates. The results of the present study are of interest for nuclear many-body calculations where chiral three-nucleon forces are treated beyond leading order via a density-dependent effective two-body interaction.Comment: 9 pages, 6 figures, to be published in European Journal

    Nuclear energy density functional from chiral pion-nucleon dynamics: Isovector terms

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    We extend a recent calculation of the nuclear energy density functional in the framework of chiral perturbation theory by computing the isovector surface and spin-orbit terms: (\vec \nabla \rho_p- \vec \nabla \rho_n)^2 G_d(\rho)+ (\vec \nabla \rho_p- \vec \nabla \rho_n)\cdot(\vec J_p-\vec J_n) G_{so(\rho)+(\vec J_p-\vec J_n)^2 G_J(\rho) pertaining to different proton and neutron densities. Our calculation treats systematically the effects from 1π1\pi-exchange, iterated 1π1\pi-exchange, and irreducible 2π2\pi-exchange with intermediate Δ\Delta-isobar excitations, including Pauli-blocking corrections up to three-loop order. Using an improved density-matrix expansion, we obtain results for the strength functions Gd(ρ)G_d(\rho), Gso(ρ)G_{so}(\rho) and GJ(ρ)G_J(\rho) which are considerably larger than those of phenomenological Skyrme forces. These (parameter-free) predictions for the strength of the isovector surface and spin-orbit terms as provided by the long-range pion-exchange dynamics in the nuclear medium should be examined in nuclear structure calculations at large neutron excess.Comment: 12 pages, 5 figure

    Chiral 3π\pi-exchange NN-potentials: Results for dominant next-to-leading order contributions

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    We calculate in (two-loop) chiral perturbation theory the local NN-potentials generated by the three-pion exchange diagrams with one insertion from the second order chiral effective pion-nucleon Lagrangian proportional to the low-energy constants c1,2,3,4c_{1,2,3,4}. The resulting isoscalar central potential vanishes identically. In most cases these 3π3\pi-exchange potentials are larger than the ones generated by the diagrams involving only leading order vertices due to the large values of c3,4c_{3,4} (which mainly represent virtual Δ\Delta-excitation). A similar feature has been observed for the chiral 2π2\pi-exchange. We also give suitable (double-integral) representations for the spin-spin and tensor potentials generated by the leading-order diagrams proportional to gA6g_A^6 involving four nucleon propagators. In these cases the Cutkosky rule cannot be used to calculate the spectral-functions in the infinite nucleon mass limit since the corresponding mass-spectra start with a non-vanishing value at the 3π3\pi-threshold. Altogether, one finds that chiral 3π3\pi-exchange leads to small corrections in the region r1.4r\geq 1.4 fm where 1π1\pi- and chiral 2π2\pi-exchange alone provide a very good strong NN-force as shown in a recent analysis of the low-energy pp-scattering data-base.Comment: 11 pages, 7 figures, to be published in The Physical Review

    Incremental Process Support for Code Reengineering

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    Reengineering a large code base can be a monumental task, and the situation becomes even worse if the code is concomitantly being modified. For the past two years, we have been using the Marvel process centered environment (PCE) for all of our software development and are currently using it to develop the Oz PCE (Marvel's successor). Towards this effort, we are reengineering Oz's code base to isolate the process engine, transaction manager, and object management system as separate components that can be mixed and matched in arbitrary systems. In this paper, we show how a PCE can guide and assist teams of users in carrying out code reengineering while allowing them to continue their normal code development. The key features to this approach are its incremental nature and the ability of the PCE to automate most of the tasks necessary to maintain the consistency of the code base

    An Architecture for Integrating Concurrency Control into Environment Frameworks

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    Research in layered and componentized systems shows the benefit of dividing the responsibility of services into separate components. It is still an unresolved issue, however, how a system can be created from a set of existing (independently developed) components. This issue of integration is of immense concern to software architects since a proper solution would reduce duplicate implementation efforts and promote component reuse. In this paper we take a step towards this goal within the domain of software development environments (SDEs) by showing how to integrate an external concurrency control component, called Pern, with environment frameworks. We discuss two experiments where we integrated Pern with Oz, a multi-site, decentralized process centered environment, and Process WEAVER, a commercial process server. We introduce an architecture for retrofitting an external concurrency control component into an environment
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