Search results for "energie"

showing 10 items of 215 documents

Stable and metastable hard-sphere crystals in fundamental measure theory

2013

Using fully minimized fundamental measure functionals, we investigate free energies, vacancy concentrations and density distributions for bcc, fcc and hcp hard-sphere crystals. Results are complemented by an approach due to Stillinger which is based on expanding the crystal partition function in terms of the number n of free particles while the remaining particles are frozen at their ideal lattice positions. The free energies of fcc/hcp and one branch of bcc agree well with Stillinger's approach truncated at n=2. A second branch of bcc solutions features rather spread-out density distributions around lattice sites and large equilibrium vacancy concentrations and is presumably linked to the …

PhysicsCondensed matter physicsCondensed Matter::OtherShear instabilityFOS: Physical sciencesCondensed Matter - Soft Condensed MatterMeasure (mathematics)CrystalCondensed Matter::Materials ScienceClassical mechanicsMetastabilityLattice (order)Vacancy defectPhysics::Atomic and Molecular ClustersSoft Condensed Matter (cond-mat.soft)Free energiesPhysical Review E
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Positive Tolman Length in a Lattice Gas with Three-Body Interactions

2011

We present a new method to determine the curvature dependence of the interface tension between coexisting phases in a finite volume from free energies obtained by Monte Carlo simulations. For the example of a lattice gas on a 3D fcc lattice with nearest neighbor three-body interactions, we demonstrate how to calculate the equimolar radius ${R}_{e}$ as well as the radius ${R}_{s}$ of the surface of tension and thus the Tolman length $\ensuremath{\delta}({R}_{s})={R}_{e}\ensuremath{-}{R}_{s}$. Within the physically relevant range of radii, $\ensuremath{\delta}({R}_{s})$ shows a pronounced ${R}_{s}$ dependence, such that the simple Tolman parametrization for the interface tension is refutable.…

PhysicsCondensed matter physicsLattice (order)ExtrapolationGeneral Physics and AstronomyTolman lengthFree energiesLimitingRadiusCurvaturek-nearest neighbors algorithmPhysical Review Letters
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Observation of an excess in the search for the Standard Model Higgs boson at ALEPH

2000

A search has been performed for the Standard Model Higgs boson in the data sample collected with the ALEPH detector at LEP, at centre-of-mass energies up to 209GeV. An excess of 3sigma beyond the background expectation is found, consistent with the production of the Higgs boson with a mass near 114GeV/c2. Much of this excess is seen in the four-jet analyses, where three high purity events are selected.

PhysicsNuclear and High Energy PhysicsParticle physicsAlephResearch Groups and Centres\Physics\Low Temperature Physics010308 nuclear & particles physicsENERGIESFaculty of Science\PhysicsElectron–positron annihilationDetectorHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesHiggs boson[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsParticle Physics - Experiment
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Cross section ratio and angular distributions of the reaction p + d -> 3He + eta at 48.8 MeV and 59.8 MeV excess energy

2014

We present new data for angular distributions and on the cross section ratio of the p + d -> 3He + eta reaction at excess energies of Q = 48.8 MeV and Q = 59.8 MeV. The data have been obtained at the WASA-at-COSY experiment (Forschungszentrum J\"ulich) using a proton beam and a deuterium pellet target. While the shape of obtained angular distributions show only a slow variation with the energy, the new results indicate a distinct and unexpected total cross section fluctuation between Q = 20 MeV and Q = 60 MeV, which might indicate the variation of the production mechanism within this energy interval.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryIntermediate EnergiesEta01 natural sciences7. Clean energyNuclear physicsCross section (physics)Tensor Analyzing PowerDeuteriumNear-Threshold0103 physical sciencesEnergy intervalPhysics::Accelerator Physicsddc:530010306 general physicsNuclear ExperimentExcess energyNuclear ExperimentBeam (structure)
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Fission fragment angular distribution of 232Th(n,f) at the CERN n TOF facility

2014

The angular distribution of fragments emitted in neutron-induced fission of 232Th was measured in the white spectrum neutron beam at the n_TOF facility at CERN. A reaction chamber based on Parallel Plate Avalanche Counters (PPAC) was used, where the detectors and the targets have been tilted 45 degrees with respect to the neutron beam direction in order to cover the full angular range of the fission fragments. A GEANT4 simulation has been developed to study the setup efficiency. The data analysis and the preliminary results obtained for the 232Th(n,f) between fission threshold and 100 MeV are presented here.

PhysicsNuclear reaction:Energies::Energia nuclear [Àrees temàtiques de la UPC]NeutronsNuclear and High Energy PhysicsLarge Hadron Collidercross sectionFragment (computer graphics)FissionPhysics::Instrumentation and DetectorsNuclear TheoryTOFNuclear data232Th; n_TOF; fission fragments; angular distributionNuclear physicsCross section (physics)Angular distributionneutronPhysics::Accelerator PhysicsfissionNeutronNuclear Experimentnuclear reactions
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High-precision ab initio calculations of the spectrum of Lr$^+$

2019

The planned measurement of optical resonances in singly-ionised lawrencium (Z = 103) requires accurate theoretical predictions to narrow the search window. We present high-precision, ab initio calculations of the electronic spectra of Lr$^+$ and its lighter homologue lutetium (Z = 71). We have employed the state-of-the-art relativistic Fock space coupled cluster approach and the AMBiT CI+MBPT code to calculate atomic energy levels, g-factors, and transition amplitudes and branching-ratios. Our calculations are in close agreement with experimentally measured energy levels and transition strengths for the homologue Lu$^+$ , and are well-converged for Lr$^+$ , where we expect a similar level o…

PhysicsSPECTROSCOPYSETSAtomic Physics (physics.atom-ph)ENERGIESFOS: Physical scienceschemistry.chemical_elementConfiguration interaction01 natural sciencesSpectral lineLutetiumPhysics - Atomic Physics010305 fluids & plasmasFock spaceATOMSCoupled clusterchemistryAb initio quantum chemistry methodsIonization0103 physical sciencesPROGRAMddc:530Atomic physics010306 general physicsLawrencium
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Logarithmic finite-size effects on interfacial free energies: Phenomenological theory and Monte Carlo studies

2014

The computation of interfacial free energies between coexisting phases (e.g.~saturated vapor and liquid) by computer simulation methods is still a challenging problem due to the difficulty of an atomistic identification of an interface, and due to interfacial fluctuations on all length scales. The approach to estimate the interfacial tension from the free energy excess of a system with interfaces relative to corresponding single-phase systems does not suffer from the first problem but still suffers from the latter. Considering $d$-dimensional systems with interfacial area $L^{d-1}$ and linear dimension $L_z$ in the direction perpendicular to the interface, it is argued that the interfacial …

PhysicsStatistical Mechanics (cond-mat.stat-mech)LogarithmSurface PropertiesEntropyComputationTemperatureFOS: Physical sciencesTracingSurface tensionComputer SimulationFree energiesMonte carlo studiesStatistical physicsMonte Carlo MethodCondensed Matter - Statistical MechanicsPhysical Review E
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Computing absolute free energies of disordered structures by molecular simulation

2009

We present a Monte Carlo simulation technique by which the free energy of disordered systems can be computed directly. It is based on thermodynamic integration. The central idea is to construct an analytically solvable reference system from a configuration which is representative for the state of interest. The method can be applied to lattice models (e.g., the Ising model) as well as off-lattice molecular models. We focus mainly on the more challenging off-lattice case. We propose a Monte Carlo algorithm, by which the thermodynamic integration path can be sampled efficiently. At the examples of the hard sphere liquid and a hard disk solid with a defect, we discuss several properties of the …

PhysicsStatistical Mechanics (cond-mat.stat-mech)Monte Carlo method: Physics [G04] [Physical chemical mathematical & earth Sciences]General Physics and AstronomyThermodynamic integrationFOS: Physical sciencesMolecular simulationCondensed Matter - Soft Condensed Matter: Physique [G04] [Physique chimie mathématiques & sciences de la terre]Lattice (order)Soft Condensed Matter (cond-mat.soft)Free energiesIsing modelStatistical physicsPhysical and Theoretical ChemistryCondensed Matter - Statistical MechanicsMonte Carlo algorithm
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Structure of rotational bands in 253No

2009

In-beam gamma-ray and conversion electron spectroscopic studies have been performed on the 253 No nucleus. A strongly coupled rotational band has been identified and the improved statistics allows an assignment of the band structure as built on the $\ensuremath 9/2^-[734]_{\nu}$ ground state. The results agree with previously known transition energies but disagree with the tentative structural assignments made in earlier work.

PhysicsStrongly coupledNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsHadronStructure (category theory)Electron01 natural sciences0103 physical sciencesStrong couplingNuclear fusion21.10.-k Properties of nuclei; nuclear energy levels - 23.20.Lv γ transitions and level energies - 29.30.Dn Electron spectroscopy - 27.90.+b A ≤ 220Atomic physics010306 general physicsGround stateElectronic band structure
Eur. Phys. J. A 42, 333 (2009)

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Three-photon resonance ionization of atomic Mn in a hot-cavity laser ion source using Ti:sapphire lasers

2015

Three-photon resonance ionization of atomic manganese (Mn) in a hot-cavity ion source using Ti:sapphire lasers has been demonstrated. Three-step ionization schemes employing different intermediate levels and Rydberg or autoionizing (AI) states in the final ionization step are established. Strong AI resonances were observed via the 3d54s5s f 6S5/2 level at 49 415.35 cm−1, while Rydberg transitions were reached from the 3d54s4d e 6D9/2,7/2,5/2 levels at around 47 210 cm−1. Analyses of the strong Rydberg transitions associated with the 3d54s4d e 6D7/2 lower level indicate that they belong to the dipole-allowed 4d → nf 6F°9/2,7/2,5/2 series converging to the 3d54s 7S3 ground state of Mn II. Fro…

PhysicsThermal ionizationMolar ionization energies of the elementsCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIon sourceAtmospheric-pressure laser ionizationsymbols.namesakeExcited stateIonizationRydberg formulasymbolsAtomic physicsElectron ionizationJournal of Physics B: Atomic, Molecular and Optical Physics
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