407 research outputs found

    Abelian gauge potentials on cubic lattices

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    The study of the properties of quantum particles in a periodic potential subject to a magnetic field is an active area of research both in physics and mathematics; it has been and it is still deeply investigated. In this review we discuss how to implement and describe tunable Abelian magnetic fields in a system of ultracold atoms in optical lattices. After discussing two of the main experimental schemes for the physical realization of synthetic gauge potentials in ultracold set-ups, we study cubic lattice tight-binding models with commensurate flux. We finally examine applications of gauge potentials in one-dimensional rings.Comment: To appear on: "Advances in Quantum Mechanics: Contemporary Trends and Open Problems", G. Dell'Antonio and A. Michelangeli eds., Springer-INdAM series 201

    Analysis of the modes of energy consumption of the complex of an incoherent scattering of the institute of ionosphere of national academy of sciences and the ministry of education and science of Ukraine

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    ĐŁ ĐŽĐ°ĐœŃ–Đč статті прДЎстаĐČĐ»Đ”ĐœŃ– Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž Đ°ĐœĐ°Đ»Ń–Đ·Ńƒ Ń€Đ”Đ¶ĐžĐŒŃ–ĐČ Đ”ĐœĐ”Ń€ĐłĐŸŃĐżĐŸĐ¶ĐžĐČĐ°ĐœĐœŃ ĐșĐŸĐŒĐżĐ»Đ”Đșсу ĐœĐ”ĐșĐŸĐłĐ”Ń€Đ”ĐœŃ‚ĐœĐŸĐłĐŸ Ń€ĐŸĐ·ŃŃ–ŃĐœĐœŃ Đ†ĐœŃŃ‚ĐžŃ‚ŃƒŃ‚Ńƒ Ń–ĐŸĐœĐŸŃŃ„Đ”Ń€Đž НАН і МОН ĐŁĐșŃ€Đ°Ń—ĐœĐž Đ· ĐŒĐ”Ń‚ĐŸŃŽ ĐČĐžŃ€Ń–ŃˆĐ”ĐœĐœŃ ĐżŃ€ĐŸĐ±Đ»Đ”ĐŒĐž піЮĐČĐžŃ‰Đ”ĐœĐœŃ Đ”ĐœĐ”Ń€ĐłĐŸĐ”Ń„Đ”ĐșтоĐČĐœĐŸŃŃ‚Ń– ĐœĐ°ŃƒĐșĐŸĐČĐŸ-ĐŽĐŸŃĐ»Ń–ĐŽĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșсу та стĐČĐŸŃ€Đ”ĐœĐœŃ Đ”ĐœĐ”Ń€ĐłĐŸĐ”Ń„Đ”ĐșтоĐČĐœĐŸŃ— ŃĐžŃŃ‚Đ”ĐŒĐž ДлДĐșŃ‚Ń€ĐŸĐżĐŸŃŃ‚Đ°Ń‡Đ°ĐœĐœŃ, яĐșĐ° Đ·Đ°Đ±Đ”Đ·ĐżĐ”Ń‡ĐžŃ‚ŃŒ стіĐčĐșу Ń€ĐŸĐ±ĐŸŃ‚Ńƒ ĐœĐ°ŃƒĐșĐŸĐČĐŸĐłĐŸ ĐŸĐ±Đ»Đ°ĐŽĐœĐ°ĐœĐœŃ ĐŽĐ»Ń ĐČĐžĐșĐŸĐœĐ°ĐœĐœŃ ĐŽĐŸŃĐ»Ń–ĐŽĐœĐžŃ†ŃŒĐșох ĐżŃ€ĐŸĐłŃ€Đ°ĐŒ НАН ĐŁĐșŃ€Đ°Ń—ĐœĐž. ĐžĐżĐžŃĐ°ĐœĐ° ŃĐžŃŃ‚Đ”ĐŒĐ° ДлДĐșŃ‚Ń€ĐŸĐ¶ĐžĐČĐ»Đ”ĐœĐœŃ ĐșĐŸĐŒĐżĐ»Đ”Đșсу та Ń€Đ”Đ¶ĐžĐŒĐž Đ”ĐœĐ”Ń€ĐłĐŸŃĐżĐŸĐ¶ĐžĐČĐ°ĐœĐœŃ ĐșĐŸĐŒĐżĐ»Đ”Đșсу. ĐžĐżĐžŃĐ°ĐœĐŸ ĐżŃ€ĐžŃŃ‚Ń€ĐŸŃ— Ń€Đ°ĐŽĐ°Ń€ĐœĐŸŃ— ŃĐžŃŃ‚Đ”ĐŒĐž, Đ° таĐșĐŸĐ¶ ĐœĐ°ĐčĐ±Ń–Đ»ŃŒŃˆ ĐżĐŸŃ‚ŃƒĐ¶ĐœŃ– ŃĐżĐŸĐ¶ĐžĐČачі ДлДĐșŃ‚Ń€ĐŸĐ”ĐœĐ”Ń€ĐłŃ–Ń—, яĐșі ŃĐżĐŸĐ¶ĐžĐČають ДлДĐșŃ‚Ń€ĐŸĐ”ĐœĐ”Ń€ĐłŃ–ŃŽ ĐœĐ° Đ”ĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœŃ– і ĐłĐŸŃĐżĐŸĐŽĐ°Ń€ŃŃŒĐșі ĐżĐŸŃ‚Ń€Đ”Đ±Đž. ĐŸŃ€ĐŸĐ°ĐœĐ°Đ»Ń–Đ·ĐŸĐČĐ°ĐœĐŸ Đ”ĐœĐ”Ń€ĐłĐŸŃĐżĐŸĐ¶ĐžĐČĐ°ĐœĐœŃ ĐșĐŸĐŒĐżĐ»Đ”Đșсу ĐœĐ”ĐșĐŸĐłĐ”Ń€Đ”ĐœŃ‚ĐœĐŸĐłĐŸ Ń€ĐŸĐ·ŃŃ–ŃĐœĐœŃ Đ·Đ° 2013 р. ĐžŃ‚Ń€ĐžĐŒĐ°ĐœĐŸ і прДЎстаĐČĐ»Đ”ĐœĐŸ графіĐșĐž ŃĐ”Ń€Đ”ĐŽĐœŃŒĐŸŃ— ŃĐżĐŸĐ¶ĐžĐČĐ°ĐœĐŸŃ— ĐżĐŸŃ‚ŃƒĐ¶ĐœĐŸŃŃ‚Ń– (ŃĐ”Ń€Đ”ĐŽĐœŃŒĐŸĐŽĐŸĐ±ĐŸĐČĐžĐč ĐżĐŸĐșĐ°Đ·ĐœĐžĐș) і ŃĐ”Ń€Đ”ĐŽĐœŃŒĐŸŃ— ŃĐżĐŸĐ¶ĐžĐČĐ°ĐœĐŸŃ— ĐżĐŸŃ‚ŃƒĐ¶ĐœĐŸŃŃ‚Ń– ĐČ Ń€Đ”Đ¶ĐžĐŒŃ– ĐČĐžĐŒŃ–Ń€ŃŽĐČĐ°ĐœŃŒ. ĐžĐżĐžŃĐ°ĐœĐ° ĐŽĐŸŃ†Ń–Đ»ŃŒĐœŃ–ŃŃ‚ŃŒ ĐżŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐœŃ Ń€ĐŸĐ±Ń–Ń‚ Đ· ĐŸĐżŃ‚ĐžĐŒŃ–Đ·Đ°Ń†Ń–Ń— Đ”ĐœĐ”Ń€ĐłĐŸĐżĐŸŃŃ‚Đ°Ń‡Đ°ĐœĐœŃ ĐœĐ°ŃƒĐșĐŸĐČĐŸ-ĐŽĐŸŃĐ»Ń–ĐŽĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșсу Đ†ĐœŃŃ‚ĐžŃ‚ŃƒŃ‚Ńƒ Ń–ĐŸĐœĐŸŃŃ„Đ”Ń€Đž. Đ—Đ°ĐżŃ€ĐŸĐżĐŸĐœĐŸĐČĐ°ĐœĐŸ ĐŒĐŸĐ¶Đ»ĐžĐČі Đ·Đ°Ń…ĐŸĐŽĐž ĐŽĐ»Ń Đ·ĐœĐžĐ¶Đ”ĐœĐœŃ Đ”ĐșĐŸĐœĐŸĐŒŃ–Ń‡ĐœĐŸŃ— ĐČĐ°Ń€Ń‚ĐŸŃŃ‚Ń– ĐżŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐœŃ Đ”ĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Ń–ĐČ Đ· ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐœŃ Ń–ĐŸĐœĐŸŃŃ„Đ”Ń€Đž ĐœĐ°ŃƒĐșĐŸĐČĐŸ-ĐŽĐŸŃĐ»Ń–ĐŽĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșсу ĐœĐ”ĐșĐŸĐłĐ”Ń€Đ”ĐœŃ‚ĐœĐŸĐłĐŸ Ń€ĐŸĐ·ŃŃ–ŃĐœĐœŃ. ĐŸŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐŸ Đ°ĐœĐ°Đ»Ń–Đ· Ń€ĐŸĐ±Ń–Ń‚ ŃŃƒŃ‡Đ°ŃĐœĐžŃ… Đ°ĐČŃ‚ĐŸŃ€Ń–ĐČ Đ· ĐŒĐ”Ń‚ĐŸŃŽ ĐżĐŸĐșĐ°Đ·Đ°Ń‚Đž, Ń‰ĐŸ піЮĐČĐžŃ‰Đ”ĐœĐœŃ ДфДĐșтоĐČĐœĐŸŃŃ‚Ń– Ń„ŃƒĐœĐșŃ†Ń–ĐŸĐœŃƒĐČĐ°ĐœĐœŃ ŃĐžŃŃ‚Đ”ĐŒ ДлДĐșŃ‚Ń€ĐŸĐżĐŸŃŃ‚Đ°Ń‡Đ°ĐœĐœŃ є Đ°ĐșŃ‚ŃƒĐ°Đ»ŃŒĐœĐŸŃŽ ĐżŃ€ĐŸĐ±Đ»Đ”ĐŒĐŸŃŽ ŃŃƒŃ‡Đ°ŃĐœĐžŃ… ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœŃŒ.This article presents the results of the analysis of the energy consumption modes of the incoherent scattering complex of the Institute of Ionosphere of the National Academy of Sciences and the Ministry of Education and Science of Ukraine to solve the problem of increasing the energy efficiency of a research complex and creating an energy efficient power supply system that will ensure the sustainability of scientific equipment for research programs of the National Academy of Sciences of Ukraine. The system of power supply of the complex and modes of power consumption of the complex are described. The devices of the radar system are described, as well as the most powerful consumers of electricity, which consume electricity for experimental and economic needs. The energy consumption of the incoherent scattering complex in 2013 is analyzed. Graphs of the average power consumption (daily average) and average power consumption in measurement modes were obtained and presented. The feasibility of work to optimize the energy supply of the research complex of the institute of the ionosphere is described. Possible measures are proposed to reduce the economic cost of conducting experiments on the study of the ionosphere of an incoherent scattering research complex. The analysis of the works of modern authors i s carried out in order to show that increasing the efficiency of the power supply systems is an actual problem of modern research

    Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in √s = 7 TeV pp collisions with the ATLAS detector

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    A search for the direct production of charginos and neutralinos in final states with three electrons or muons and missing transverse momentum is presented. The analysis is based on 4.7 fb−1 of proton–proton collision data delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in three signal regions that are either depleted or enriched in Z-boson decays. Upper limits at 95% confidence level are set in R-parity conserving phenomenological minimal supersymmetric models and in simplified models, significantly extending previous results

    Jet size dependence of single jet suppression in lead-lead collisions at sqrt(s(NN)) = 2.76 TeV with the ATLAS detector at the LHC

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    Measurements of inclusive jet suppression in heavy ion collisions at the LHC provide direct sensitivity to the physics of jet quenching. In a sample of lead-lead collisions at sqrt(s) = 2.76 TeV corresponding to an integrated luminosity of approximately 7 inverse microbarns, ATLAS has measured jets with a calorimeter over the pseudorapidity interval |eta| < 2.1 and over the transverse momentum range 38 < pT < 210 GeV. Jets were reconstructed using the anti-kt algorithm with values for the distance parameter that determines the nominal jet radius of R = 0.2, 0.3, 0.4 and 0.5. The centrality dependence of the jet yield is characterized by the jet "central-to-peripheral ratio," Rcp. Jet production is found to be suppressed by approximately a factor of two in the 10% most central collisions relative to peripheral collisions. Rcp varies smoothly with centrality as characterized by the number of participating nucleons. The observed suppression is only weakly dependent on jet radius and transverse momentum. These results provide the first direct measurement of inclusive jet suppression in heavy ion collisions and complement previous measurements of dijet transverse energy imbalance at the LHC.Comment: 15 pages plus author list (30 pages total), 8 figures, 2 tables, submitted to Physics Letters B. All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2011-02

    Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at sqrt(s) = 7 TeV with the ATLAS experiment

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    This paper describes an analysis of the angular distribution of W->enu and W->munu decays, using data from pp collisions at sqrt(s) = 7 TeV recorded with the ATLAS detector at the LHC in 2010, corresponding to an integrated luminosity of about 35 pb^-1. Using the decay lepton transverse momentum and the missing transverse energy, the W decay angular distribution projected onto the transverse plane is obtained and analysed in terms of helicity fractions f0, fL and fR over two ranges of W transverse momentum (ptw): 35 < ptw < 50 GeV and ptw > 50 GeV. Good agreement is found with theoretical predictions. For ptw > 50 GeV, the values of f0 and fL-fR, averaged over charge and lepton flavour, are measured to be : f0 = 0.127 +/- 0.030 +/- 0.108 and fL-fR = 0.252 +/- 0.017 +/- 0.030, where the first uncertainties are statistical, and the second include all systematic effects.Comment: 19 pages plus author list (34 pages total), 9 figures, 11 tables, revised author list, matches European Journal of Physics C versio

    Observation of a new chi_b state in radiative transitions to Upsilon(1S) and Upsilon(2S) at ATLAS

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    The chi_b(nP) quarkonium states are produced in proton-proton collisions at the Large Hadron Collider (LHC) at sqrt(s) = 7 TeV and recorded by the ATLAS detector. Using a data sample corresponding to an integrated luminosity of 4.4 fb^-1, these states are reconstructed through their radiative decays to Upsilon(1S,2S) with Upsilon->mu+mu-. In addition to the mass peaks corresponding to the decay modes chi_b(1P,2P)->Upsilon(1S)gamma, a new structure centered at a mass of 10.530+/-0.005 (stat.)+/-0.009 (syst.) GeV is also observed, in both the Upsilon(1S)gamma and Upsilon(2S)gamma decay modes. This is interpreted as the chi_b(3P) system.Comment: 5 pages plus author list (18 pages total), 2 figures, 1 table, corrected author list, matches final version in Physical Review Letter

    Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS

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    We present the results of a search for new, heavy particles that decay at a significant distance from their production point into a final state containing charged hadrons in association with a high-momentum muon. The search is conducted in a pp-collision data sample with a center-of-mass energy of 7 TeV and an integrated luminosity of 33 pb^-1 collected in 2010 by the ATLAS detector operating at the Large Hadron Collider. Production of such particles is expected in various scenarios of physics beyond the standard model. We observe no signal and place limits on the production cross-section of supersymmetric particles in an R-parity-violating scenario as a function of the neutralino lifetime. Limits are presented for different squark and neutralino masses, enabling extension of the limits to a variety of other models.Comment: 8 pages plus author list (20 pages total), 8 figures, 1 table, final version to appear in Physics Letters

    Measurement of the inclusive isolated prompt photon cross-section in pp collisions at sqrt(s)= 7 TeV using 35 pb-1 of ATLAS data

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    A measurement of the differential cross-section for the inclusive production of isolated prompt photons in pp collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. The measurement covers the pseudorapidity ranges |eta|<1.37 and 1.52<=|eta|<2.37 in the transverse energy range 45<=E_T<400GeV. The results are based on an integrated luminosity of 35 pb-1, collected with the ATLAS detector at the LHC. The yields of the signal photons are measured using a data-driven technique, based on the observed distribution of the hadronic energy in a narrow cone around the photon candidate and the photon selection criteria. The results are compared with next-to-leading order perturbative QCD calculations and found to be in good agreement over four orders of magnitude in cross-section.Comment: 7 pages plus author list (18 pages total), 2 figures, 4 tables, final version published in Physics Letters

    Measurement of D*+/- meson production in jets from pp collisions at sqrt(s) = 7 TeV with the ATLAS detector

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    This paper reports a measurement of D*+/- meson production in jets from proton-proton collisions at a center-of-mass energy of sqrt(s) = 7 TeV at the CERN Large Hadron Collider. The measurement is based on a data sample recorded with the ATLAS detector with an integrated luminosity of 0.30 pb^-1 for jets with transverse momentum between 25 and 70 GeV in the pseudorapidity range |eta| < 2.5. D*+/- mesons found in jets are fully reconstructed in the decay chain: D*+ -> D0pi+, D0 -> K-pi+, and its charge conjugate. The production rate is found to be N(D*+/-)/N(jet) = 0.025 +/- 0.001(stat.) +/- 0.004(syst.) for D*+/- mesons that carry a fraction z of the jet momentum in the range 0.3 < z < 1. Monte Carlo predictions fail to describe the data at small values of z, and this is most marked at low jet transverse momentum.Comment: 10 pages plus author list (22 pages total), 5 figures, 1 table, matches published version in Physical Review

    Search for scalar top quark pair production in natural gauge mediated supersymmetry models with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV

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    The results of a search for pair production of the lighter scalar partners of top quarks in 2.05 fb-1 of pp collisions at sqrt(s) =7 TeV using the ATLAS experiment at the LHC are reported. Scalar top quarks are searched for in events with two same flavour opposite-sign leptons (electrons or muons) with invariant mass consistent with the Z boson mass, large missing transverse momentum and jets in the final state. At least one of the jets is identified as originating from a b-quark. No excess over Standard Model expectations is found. The results are interpreted in the framework of R-parity conserving, gauge mediated Supersymmetry breaking `natural' scenarios, where the neutralino is the next-to-lightest supersymmetric particle. Scalar top quark masses up to 310 GeV are excluded for the lightest neutralino mass between 115 GeV and 230 GeV at 95% confidence level, reaching an exclusion of the scalar top quark mass of 330 GeV for the lightest neutralino mass of 190 GeV. Scalar top quark masses below 240 GeV are excluded for all values of the lightest neutralino mass above the Z boson mass.Comment: 7 pages plus author list (20 pages total), 4 figures, 1 table, matches published PLB versio
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