Search results for "ACS"

showing 10 items of 259 documents

Light scattering in inhomogeneous Tomonaga-Luttinger liquids

2012

We derive the dynamical structure factor for an inhomogeneous Tomonaga-Luttinger liquid as can be formed in a confined strongly interacting one-dimensional gas. In view of current experimental progress in the field, we provide a simple analytic expression for the light-scattering cross section, requiring only the knowledge of the density dependence of the ground-state energy, as they can be extracted e.g. from exact or Quantum Monte Carlo techniques, and a Thomas-Fermi description. We apply the result to the case of one-dimensional quantum bosonic gases with dipolar interaction in a harmonic trap, using an energy functional deduced from Quantum Monte Carlo computations. We find an universal…

PhysicsCondensed Matter::Quantum GasesField (physics)[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Quantum Monte CarloBragg spectroscopyFOS: Physical sciencestrapping potentialPACS: 67.85.-d 71.10.Pm 67.10.Hk01 natural sciencesAtomic and Molecular Physics and OpticsLight scattering010305 fluids & plasmasTomonaga-Lutttinger liquidCross section (physics)Quantum Gases (cond-mat.quant-gas)Quantum mechanics0103 physical sciences010306 general physicsStructure factorCondensed Matter - Quantum GasesScalingQuantumEnergy functional
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Influence ofsp−dhybridization on the electronic structure of Al-Mn alloys

2008

The influence of $sp\text{\ensuremath{-}}d$ hybridization on the electronic structure of different Al-Mn alloys has been studied by photoelectron spectroscopy. Experimental evidence of a pseudogap in a crystalline binary Hume-Rothery alloy is provided. The pseudogap varies systematically with Mn concentration. The $sp\text{\ensuremath{-}}d$ hybridization alone, even in the absence of Hume-Rothery mechanism, can produce the pseudogap. Existence of the pseudogap, suppression of the $\mathrm{Mn}\phantom{\rule{0.2em}{0ex}}2p$ satellite, and decrease in the Doniach-\ifmmode \check{S}\else \v{S}\fi{}unji\ifmmode \acute{c}\else \'{c}\fi{} asymmetry parameter are the consequences of the $sp\text{\e…

PhysicsCondensed matter physicsAnnealing (metallurgy)Alloy02 engineering and technologyElectronic structureengineering.material021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesElectron spectroscopyPACS 71.20.Be 79.60.i 81.05.BxElectronic Optical and Magnetic MaterialsX-ray photoelectron spectroscopy0103 physical sciencesengineering010306 general physics0210 nano-technologyPseudogapSpectroscopyPhysical Review B
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Sudden change in the nuclear charge distribution of very light gold isotopes

1987

4 pages, 3 tables, 2 figures.-- PACS nrs.: 21.10.Ft, 21.10.Ky, 27.70.+q.

PhysicsGeneral Physics and AstronomyCharge densityRadiusPhotoionizationEffective nuclear chargeTime of flight[PACS] Electromagnetic momentsIonization[PACS] Charge distribution150 ≤ A ≤ 189 [[PACS] Properties of specific nuclei listed by mass ranges]Nuclear Physics - ExperimentPhysics::Atomic PhysicsIsotopes of gold[PACS] Properties of specific nuclei listed by mass ranges:150 ≤ A ≤ 189Atomic physicsHyperfine structure
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Dielectric Collimators for Beam Delivery Systems*

2012

Abstract Wakefield generation by the collimation system is known to be a critical linear collider design issue. Optimization of the collimators represents a tradeoff between beam quality (halo reduction) and luminosity reduction. The primary objective is to reduce both short range (resonant) and long range (resistive) deflecting wakefields from collimators that reduce the luminosity of the machine. We consider the CLIC BDS (beam delivery system) and examine the potential for using dielectric rather than highly conducting materials for collimation. We present some examples of the flexibility gained by having control over the permittivity and conductivity of the collimator. We discuss simulation …

PhysicsLuminosity (scattering theory)collimationbusiness.industry29.27.BdLinear colliderCollimatorDielectricwakefields PACS: 29.27.EgPhysics and Astronomy(all)Accelerators and Storage RingsCollimated lightlaw.invention29.20.EjBunchesOpticslawLaser beam qualityDetectors and Experimental TechniquesbusinessColliderBeam (structure)Physics Procedia
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Black hole state counting in loop quantum gravity: a number-theoretical approach

2008

4 pages, 1 figure.-- PACS nrs.: 04.70.Dy, 04.60.Pp.-- ArXiv pre-print available at: http://arxiv.org/abs/0802.4077

PhysicsMatemáticasAstrophysics::High Energy Astrophysical PhenomenaImmirzi parameterGeneral Physics and AstronomyFOS: Physical sciencesFísicaLoop quantum gravityGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)General Relativity and Quantum CosmologyBlack holeTheoretical physicsMicro black holeGeneral Relativity and Quantum CosmologyClassical mechanicsExtremal black hole[PACS] Quantum aspects of black holes evaporation thermodynamicsVirtual black holeBlack hole thermodynamics[PACS] Loop quantum gravity quantum geometry spin foamsMathematical PhysicsBlack hole complementarity
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New information on β-delayed neutron emission from Be-12, Be-14

1999

17 pages, 3 tables, 5 figures, 1 appendix.-- PACS nrs.: 23.40.Hc; 27.20.+n.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderRadioactivity: Be-12 Be-14 (from 1 GeV p on UC target selective mass separation)Astrophysics::High Energy Astrophysical PhenomenaConfidence intervalNuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Neutron long countersBe-12 Be-14 deduced P(n) values Be-14 deduced P(xn) valuesHigh Energy Physics::ExperimentNeutronMeasured βn nn time correlations[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentDelayed neutronRadioactive beam[PACS] Relation with nuclear matrix elements and nuclear structureBe-12 Be-14 (from 1 GeV p on UC target selective mass separation) [Radioactivity]
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Precision measurement of the conversion electron spectrum of 83mKr with a solenoid retarding spectrometer

1992

This paper reports on precision measurements of conversion lines in the decay of 83mKr with nuclear transition energies of 32.1 keV and 9.4 keV, respectively. The spectra were taken from a submonolayer surface of 83mKr frozen onto a cold backing, using the new Mainz solenoid retarding spectrometer. The high luminosity and resolution of this instrument enables the observation of all allowed conversion lines up to the N-shell and to fully separate the elastic component from inelastic satellites. The combined analysis of the data yields the transition energies Ey=32151.5±1.1 eV and 9405.9±0.8 eV, respectively. The experiment served also to pilot the application of this spectrometer to the ques…

PhysicsNuclear and High Energy PhysicsLuminosity (scattering theory)SpectrometerSolenoidElectronpacs:29.30.Dnpacs:27.50.+eElectron spectroscopySpectral lineNuclear physicsNuclear fusionddc:530NeutrinoAtomic physics
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He-8 - He-6: a comparative study of electromagnetic fragmentation reactions

2002

14 pages, 1 table, 2 figures.-- PACS nrs.:27.20.+n; 24.70.+.-- Available online Oct 8, 2001.

PhysicsNuclear and High Energy PhysicsNuclear Reactions: Pb(He-8xn He-6) E=227 MeV/nucleonNuclear TheoryHalo nucleusElectromagnetic fragmentationB(E1)Dissociation (chemistry)Nuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Measured σ σ(Θ) σ(E)He-8 deduced resonance energyPb(He-6xnα) E=240 MeV/nucleonNeutronAtomic physics[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentPb(He-8xn He-6) E=227 MeV/nucleon [Nuclear Reactions]
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Three-body correlations in electromagnetic dissociation of Borromean nuclei: The 6He case

2005

20 pages, 2 tables, 9 figures, 1 appendix.-- PACS nrs.: 25.60.-t; 27.20.+n; 25.70.De; 25.75.Gz.-- Printed version published Sep 5, 2005.

PhysicsNuclear and High Energy PhysicsParticle correlationsCoulomb excitationCoulomb excitationDissociation (chemistry)Coincidence[PACS] Reactions induced by unstable nucleiAmplitude6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)[PACS] Particle correlations and fluctuationsNeutronHe-6[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsSeries expansionGround stateUnstable nucleiNuclear Physics A
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Baryon decuplet in the chiral dynamics of Λ hyperons in nuclear matter

2007

6 pages, 5 figures.-- PACS nrs.: 21.80.+a; 21.65.+f; 13.75.Ev; 24.10.Cn.-- ISI Article Identifier: 000245332200063.-- ArXiv pre-print available at: http://arxiv.org/abs/nucl-th/0611082

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeMany-body theoryHigh Energy Physics::PhenomenologyNuclear TheoryHyperon[PACS] Hyperon–nucleon interactions (energy ≤ 10 GeV)FísicaSpin-orbit InteractionSpin–orbit interactionNuclear matter[PACS] Many-body theory of nucleiNuclear physicsBaryonMany-body problemFinite NucleiPionΣ-hypernucleiHigh Energy Physics::ExperimentNuclear Experiment[PACS] Nuclear matterSpin-½
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