62,358 research outputs found

    The Value-of-Information in Matching with Queues

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    We consider the problem of \emph{optimal matching with queues} in dynamic systems and investigate the value-of-information. In such systems, the operators match tasks and resources stored in queues, with the objective of maximizing the system utility of the matching reward profile, minus the average matching cost. This problem appears in many practical systems and the main challenges are the no-underflow constraints, and the lack of matching-reward information and system dynamics statistics. We develop two online matching algorithms: Learning-aided Reward optimAl Matching (LRAM\mathtt{LRAM}) and Dual-LRAM\mathtt{LRAM} (DRAM\mathtt{DRAM}) to effectively resolve both challenges. Both algorithms are equipped with a learning module for estimating the matching-reward information, while DRAM\mathtt{DRAM} incorporates an additional module for learning the system dynamics. We show that both algorithms achieve an O(ϵ+δr)O(\epsilon+\delta_r) close-to-optimal utility performance for any ϵ>0\epsilon>0, while DRAM\mathtt{DRAM} achieves a faster convergence speed and a better delay compared to LRAM\mathtt{LRAM}, i.e., O(δz/ϵ+log(1/ϵ)2))O(\delta_{z}/\epsilon + \log(1/\epsilon)^2)) delay and O(δz/ϵ)O(\delta_z/\epsilon) convergence under DRAM\mathtt{DRAM} compared to O(1/ϵ)O(1/\epsilon) delay and convergence under LRAM\mathtt{LRAM} (δr\delta_r and δz\delta_z are maximum estimation errors for reward and system dynamics). Our results reveal that information of different system components can play very different roles in algorithm performance and provide a systematic way for designing joint learning-control algorithms for dynamic systems

    Tunable Fano-Kondo resonance in side-coupled double quantum dot system

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    We study the interference between the Fano and Kondo effects in a side-coupled double-quantum- dot system where one of the quantum dots couples to conduction electron bath while the other dot only side-couples to the first dot via antiferromagnetic (AF) spin exchange coupling. We apply both the perturbative renormalization group (RG) and numerical renormalization group (NRG) approaches to study the effect of AF coupling on the Fano lineshape in the conduction leads. With particle-hole symmetry, the AF exchange coupling competes with the Kondo effect and leads to a local spin-singlet ground state for arbitrary small coupling, so called "two-stage Kondo effect". As a result, via NRG we find the spectral properties of the Fano lineshape in the tunneling density of states (TDOS) of conduction electron leads shows double dip-peak features at the energy scale around the Kondo temperature and the one much below it, corresponding to the two-stage Kondo effect; it also shows an universal scaling behavior at very low energies. We find the qualitative agreement between the NRG and the perturbative RG approach. Relevance of our work to the experiments is discussed.Comment: 7 pages, 7 figure

    Alternative subtraction scheme using Nagy Soper dipoles

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    We present an alternative subtraction scheme for the treatment of infrared divergences in NLO QCD calculations. In this scheme, the number of transformations is greatly reduced with respect to the standard subtraction scheme by Catani and Seymour. We discuss the general setup of the scheme as well as first applications to NLO processes at hadron and lepton colliders.Comment: 6 pages, 1 figure, presented at RADCOR 0

    Energy spectra of donors in GaAs-Ga_(1-x)Al_(x)As quantum well structures in the effective mass approximation

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    We present the results of a study of the energy spectrum of the ground state and the low-lying excited states for shallow donors in quantum well structures consisting of a single slab of GaAs sandwiched between two semi-infinite layers of Ga_(1-x)Al_(x)As. The effect of the position of the impurity atom within central GaAs slab is investigated for different slab thicknesses and alloy compositions. Two limiting cases are presented: one in which the impurity atom is located at the center of the quantum well (on-center impurity), the other in which the impurity atom is located at the edge of the quantum well (on-edge impurity). Both the on-center and the on-edge donor ground state are bound for all values of GaAs slab thicknesses and alloy compositions. The alloy composition x is varied between 0.1 and 0.4. In this composition range, Ga_(1-x)Al_(x)As is direct, and the single-valley effective-mass theory is a valid technique for treating shallow donor states. Calculations are carried out in the case of finite potential barriers determined by realistic conduction-band offsets

    Quantum criticality out of equilibrium in the pseudogap Kondo model

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    We theoretically investigate the non-equilibrium quantum phase transition in a generic setup: the pseudogap Kondo model where a quantum dot couples to two-left (L) and right (R)-voltage-biased fermionic leads with power-law density of states (DOS) with respect to their Fermi levels {\mu}_L/R, {\rho}_c,L(R) ({\omega}) \propto |{\omega} - {\mu}_L(R) |r, and 0 < r < 1. In equilibrium (zero bias voltage) and for 0 < r < 1/2, with increasing Kondo correlations, in the presence of particle-hole symmetry this model exhibits a quantum phase transition from a unscreened local moment (LM) phase to the Kondo phase. Via a controlled frequency-dependent renormalization group (RG) approach, we compute analytically and numerically the non-equilibrium conductance, conduction electron T-matrix and local spin susceptibility at finite bias voltages near criticality. The current-induced decoherence shows distinct nonequilibrium scaling, leading to new universal non-equilibrium quantum critical behaviors in the above observables. Relevance of our results for the experiments is discussed.Comment: 4.1 pages, 2 figure

    Screening and antiscreening in anisotropic QED and QCD plasmas

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    We use a transport-theory approach to construct the static propagator of a gauge boson in a plasma with a general axially- and reflection-symmetric momentum distribution. Non-zero magnetic screening is found if the distribution is anisotropic, confirming the results of a closed-time-path-integral approach. We find that the electric and magnetic screening effects depend on both the orientation of the momentum carried by the boson and the orientation of its polarization. In some orientations there can be antiscreening, reflecting the instabilities of such a medium. We present some fairly general conditions on the dependence of these effects on the anisotropy.Comment: 14 pages late

    Extraction of nuclear matter properties from nuclear masses by a model of equation of state

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    The extraction of nuclear matter properties from measured nuclear masses is investigated in the energy density functional formalism of nuclei. It is shown that the volume energy a1a_1 and the nuclear incompressibility K0K_0 depend essentially on μnN+μˉpZ2EN\mu_n N+\bar{\mu}_p Z-2E_N, whereas the symmetry energy JJ and the density symmetry coefficient LL as well as symmetry incompressibility KsK_s depend essentially on μnμˉp\mu_n-\bar{\mu}_p, where μˉp=μpEC/Z\bar{\mu}_p=\mu_p-\partial E_C/\partial Z, μn\mu_n and μp\mu_p are the neutron and proton chemical potentials respectively, ENE_N the nuclear energy, and ECE_C the Coulomb energy. The obtained symmetry energy is J=28.5MeVJ=28.5MeV, while other coefficients are uncertain within ranges depending on the model of nuclear equation of state.Comment: 12 pages and 7 figure
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