42,446 research outputs found

    BB and BcB_c mesons with NRQCD and Clover actions

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    We present preliminary results from our study of the heavy-light spectrum and decay constants. For the heavy quark, we use NRQCD at various masses around and above the bb quark mass. For the first time, the heavy quark action and the heavy-light current consistently include corrections at second order in the non-relativistic expansion, as well as the leading finite aa corrections. The light quarks are simulated using a tadpole-improved Clover action at various masses in the strange and cc quark region.Comment: 6 Pages LaTex. Axis files of figures included. Joint writeup of two talks presented at LATTICE96(heavy quarks

    A Comparative Study of the Decays B→(K,K∗)ℓ+ℓ−B \to (K,K^*) \ell^+ \ell^- in Standard Model and Supersymmetric Theories

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    Using improved theoretical calculations of the decay form factors in the Light Cone-QCD sum rule approach, we investigate the decay rates, dilepton invariant mass spectra and the forward-backward (FB) asymmetry in the decays B→(K,K∗)ℓ+ℓ−B \to (K,K^*) \ell^+ \ell^- (ℓ±=e±,Ό±,τ±\ell^\pm =e^\pm,\mu^\pm,\tau^\pm) in the standard model (SM) and a number of popular variants of the supersymmetric (SUSY) models. Theoretical precision on the differential decay rates and FB-asymmetry is estimated in these theories taking into account various parametric uncertainties. We show that existing data on B→XsÎłB \to X_s \gamma and the experimental upper limit on the branching ratio B(B→K∗Ό+Ό−){\cal B}(B \to K^* \mu^+ \mu^-) provide interesting bounds on the coefficients of the underlying effective theory. We argue that the FB-asymmetry in B→K∗ℓ+ℓ−B \to K^* \ell^+ \ell^- constitutes a precision test of the SM and its measurement in forthcoming experiments may reveal new physics. In particular, the presently allowed large-tan⁥ÎČ\tan \beta solutions in SUGRA models, as well as more general flavor-violating SUSY models, yield FB-asymmetries which are characteristically different from the corresponding ones in the SM.Comment: 36 pages, 12 figures (require epsfig.sty), 8 Tables, LaTeX2e; subsection 6.4 corrected, minor changes in numerical results, Figures 3 and 9 to 12 modified; submitted to Physical Review

    O(αs)O(\alpha_s) Corrections to B→Xse+e−B \to X_s e^+ e^- Decay in the 2HDM

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    O(αs)O(\alpha_s) QCD corrections to the inclusive B→Xse+e−B \to X_s e^+ e^- decay are investigated within the two - Higgs doublet extension of the standard model (2HDM). The analysis is performed in the so - called off-resonance region; the dependence of the obtained results on the choice of the renormalization scale is examined in details. It is shown that O(αs)O(\alpha_s) corrections can suppress the B→Xse+e−B \to X_s e^+ e^- decay width up to 1.5Ă·31.5 \div 3 times (depending on the choice of the dilepton invariant mass ss and the low - energy scale ÎŒ\mu). As a result, in the experimentally allowed range of the parameters space, the relations between the B→Xse+e−B \to X_s e^+ e^- branching ratio and the new physics parameters are strongly affected. It is found also that though the renormalization scale dependence of the B→Xse+e−B \to X_s e^+ e^- branching is significantly reduced, higher order effects in the perturbation theory can still be nonnegligible.Comment: 16 pages, latex, including 6 figures and 3 table

    Coherent States on Hilbert Modules

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    We generalize the concept of coherent states, traditionally defined as special families of vectors on Hilbert spaces, to Hilbert modules. We show that Hilbert modules over C∗C^*-algebras are the natural settings for a generalization of coherent states defined on Hilbert spaces. We consider those Hilbert C∗C^*-modules which have a natural left action from another C∗C^*-algebra say, A\mathcal A. The coherent states are well defined in this case and they behave well with respect to the left action by A\mathcal A. Certain classical objects like the Cuntz algebra are related to specific examples of coherent states. Finally we show that coherent states on modules give rise to a completely positive kernel between two C∗C^*-algebras, in complete analogy to the Hilbert space situation. Related to this there is a dilation result for positive operator valued measures, in the sense of Naimark. A number of examples are worked out to illustrate the theory

    Joint Resource Optimization for Multicell Networks with Wireless Energy Harvesting Relays

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    This paper first considers a multicell network deployment where the base station (BS) of each cell communicates with its cell-edge user with the assistance of an amplify-and-forward (AF) relay node. Equipped with a power splitter and a wireless energy harvester, the self-sustaining relay scavenges radio frequency (RF) energy from the received signals to process and forward the information. Our aim is to develop a resource allocation scheme that jointly optimizes (i) BS transmit powers, (ii) received power splitting factors for energy harvesting and information processing at the relays, and (iii) relay transmit powers. In the face of strong intercell interference and limited radio resources, we formulate three highly-nonconvex problems with the objectives of sum-rate maximization, max-min throughput fairness and sum-power minimization. To solve such challenging problems, we propose to apply the successive convex approximation (SCA) approach and devise iterative algorithms based on geometric programming and difference-of-convex-functions programming. The proposed algorithms transform the nonconvex problems into a sequence of convex problems, each of which is solved very efficiently by the interior-point method. We prove that our algorithms converge to the locally optimal solutions that satisfy the Karush-Kuhn-Tucker conditions of the original nonconvex problems. We then extend our results to the case of decode-and-forward (DF) relaying with variable timeslot durations. We show that our resource allocation solutions in this case offer better throughput than that of the AF counterpart with equal timeslot durations, albeit at a higher computational complexity. Numerical results confirm that the proposed joint optimization solutions substantially improve the network performance, compared with cases where the radio resource parameters are individually optimized
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