Search results for "Vector"

showing 10 items of 2660 documents

Systematic derivation of hydrodynamic equations for viscoelastic phase separation

2021

(abridged) We present a detailed derivation of a simple hydrodynamic two-fluid model, which aims at the description of the phase separation of non-entangled polymer solutions, where viscoelastic effects play a role. It is directly based upon the coarse-graining of a well-defined molecular model, such that all degrees of freedom have a clear and unambiguous molecular interpretation. The considerations are based upon a free-energy functional, and the dynamics is split into a conservative and a dissipative part, where the latter satisfies the Onsager relations and the Second Law of thermodynamics. The model is therefore fully consistent with both equilibrium and non-equilibrium thermodynamics.…

PhysicsStatistical Mechanics (cond-mat.stat-mech)media_common.quotation_subjectConstitutive equationScalar (physics)Degrees of freedom (physics and chemistry)Four-vectorEquations of motionFOS: Physical sciencesSecond law of thermodynamicsCondensed Matter - Soft Condensed MatterCondensed Matter PhysicsClassical mechanicsDissipative systemSoft Condensed Matter (cond-mat.soft)General Materials ScienceVector fieldCondensed Matter - Statistical Mechanicsmedia_common
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Supersymmetric associated vector coherent states and generalized Landau levels arising from two-dimensional supersymmetry

2008

We describe a method for constructing vector coherent states for quantum supersymmetric partner Hamiltonians. The method is then applied to such partner Hamiltonians arising from a generalization of the fractional quantum Hall effect. Explicit examples are worked out.

PhysicsStatistical and Nonlinear PhysicsSupersymmetryLandau quantizationEigenfunctionQuantum mechanicsFractional quantum Hall effectCoherent statesSupersymmetric quantum mechanicsQuantumSettore MAT/07 - Fisica MatematicaMathematical PhysicsEigenvalues and eigenvectorsLandau levelsMathematical physics
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Viability of light-Higgs strongly-coupled scenarios

2013

Contrary to what is sometimes stated, the current electroweak precision data easily allow for massive composite resonance states at the natural EW scale, i.e., well over the TeV. The oblique parameters S and T are analyzed by means of an effective Lagrangian that implements the $SU(2)_L\otimes SU(2)_R\to SU(2)_{L+R}$ pattern of electroweak symmetry breaking. They are computed at the one-loop level and incorporating the newly discovered Higgs-like boson and possible spin-1 composite resonances. Imposing a proper ultraviolet behaviour is crucial and allows us to determine S and T at next-to-leading order in terms of a few resonance parameters. Electroweak precision data force the vector and a…

PhysicsStrongly coupledHigh Energy Physics - PhenomenologyParticle physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::PhenomenologyEffective lagrangianElectroweak interactionHiggs bosonFOS: Physical sciencesTechnicolorPseudovectorProceedings of The European Physical Society Conference on High Energy Physics — PoS(EPS-HEP 2013)
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Topological Hamiltonian as an exact tool for topological invariants

2012

We propose the concept of `topological Hamiltonian' for topological insulators and superconductors in interacting systems. The eigenvalues of topological Hamiltonian are significantly different from the physical energy spectra, but we show that topological Hamiltonian contains the information of gapless surface states, therefore it is an exact tool for topological invariants.

PhysicsSuperconductivityHigh Energy Physics - TheoryStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciencesCondensed Matter PhysicsTopology01 natural sciences010305 fluids & plasmassymbols.namesakeCondensed Matter - Strongly Correlated ElectronsGapless playbackHigh Energy Physics - Theory (hep-th)Topological insulator0103 physical sciencessymbolsTopological invariantsGeneral Materials Science010306 general physicsHamiltonian (quantum mechanics)Mathematics::Symplectic GeometryEigenvalues and eigenvectorsJournal of Physics Condensed Matter
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Study of the dynamic growth of wetting layers in the confined Ising model with competing surface fields

2006

A two-dimensional magnetic Ising system confined in an L × D geometry () in the presence of competing magnetic fields (h) acting at opposite walls along the D-direction exhibits an interface between domains of different orientation that runs parallel to the walls. In the limit of infinite film thickness () this interface undergoes a wetting transition that occurs at the critical curve Tw(h), so that for T<Tw(h) such an interface is bound to the walls, while for Tw(h)≤T≤Tcb the interface is freely fluctuating around the centre of the film, where Tcb is the bulk critical temperature. Starting from a monodomain structure with the interface bound to one wall, we study the onset of the interface…

PhysicsSurface (mathematics)Condensed matter physicsCondensed Matter Physics01 natural sciencesCritical curve010305 fluids & plasmasMagnetic fieldWetting transitionPosition (vector)Orientation (geometry)0103 physical sciencesGeneral Materials ScienceIsing modelWetting010306 general physicsJournal of Physics: Condensed Matter
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Three-prong τ decays with charged kaons

1998

Final states with charged kaons in three-prong τ decays are studied by exploiting the particle identification from the dE/dx measurement. The results are based on a sample of about 1.6 × 105 detected τ pairs collected with the ALEPH detector between 1991 and 1995 around the Z peak. The following branching ratios have been measured: B(τ- → K−K+π−ντ) = (1.63 ± 0.21 ± 0.17) × 10−3, B(τ− → K−π+π−ντ) = (2.14 ± 0.37 ± 0.29) × 10−3, B(τ− → K−K+π−π0ντ) = (0.75 ± 0.29 ± 0.15) × 10−3, and B(τ− → K−π+π−π0ντ) = (0.61 ± 0.39 ± 0.18) × 10−3. The first two measurements are more precise than the current world averages, while the last two channels are investigated for the first time. The 95% C.L. upper limi…

PhysicsSystematic errorTime projection chamberPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologySettore FIS/01 - Fisica SperimentaleVECTOR01 natural sciencesMESONSParticle identificationPHYSICS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentAtomic physics010306 general physicsEngineering (miscellaneous)Particle Physics - Experiment
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Cosmological Applications of Extended Electromagnetism

2013

Extended electromagnetism (EE) has been applied to cosmology in various papers. In all of them, the zero order energy density of the EE vector field plays the same role as vacuum energy. Perturbations of this field have been studied by using different approaches. Firstly, some basic equations and ideas are summarized and, then, the CMBFAST code is used to calculate the cosmic microwave background angular power spectrum for appropriate values of the EE parameters. Comparisons of the resulting spectra with a good observational one compatible with WMAP7 (Wilkinson map anisotropy probe 7 years data) seem to be promising. We are currently looking for a set of parameters leading to the best fitti…

PhysicsTheoretical physicsClassical mechanicsField (physics)Vacuum energyElectromagnetismCMBFASTMathematics::History and OverviewCosmic microwave backgroundVector fieldLambda-CDM modelAstrophysics::Cosmology and Extragalactic AstrophysicsCosmology
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Measurement of the tt¯Z and tt¯W cross sections in proton-proton collisions at s=13  TeV with the ATLAS detector

2019

A measurement of the associated production of a top-quark pair (tt) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb-1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The ttZ and ttW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σttZ=0.95±0.08stat±0.10syst…

PhysicsTop quarkParticle physicsMuonLarge Hadron Collider010308 nuclear & particles physicsElectron01 natural sciencesVertex (geometry)Vector boson0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Pattern selection in the 2D FitzHugh–Nagumo model

2018

We construct square and target patterns solutions of the FitzHugh–Nagumo reaction–diffusion system on planar bounded domains. We study the existence and stability of stationary square and super-square patterns by performing a close to equilibrium asymptotic weakly nonlinear expansion: the emergence of these patterns is shown to occur when the bifurcation takes place through a multiplicity-two eigenvalue without resonance. The system is also shown to support the formation of axisymmetric target patterns whose amplitude equation is derived close to the bifurcation threshold. We present several numerical simulations validating the theoretical results.

PhysicsTuring instabilityApplied MathematicsGeneral MathematicsNumerical analysis010102 general mathematicsMathematical analysisSquare pattern01 natural sciencesSquare (algebra)010305 fluids & plasmasFitzHugh–Nagumo modelNonlinear systemAmplitudeBounded function0103 physical sciencesAmplitude equationMathematics (all)FitzHugh–Nagumo model0101 mathematicsEigenvalues and eigenvectorsBifurcationRicerche di Matematica
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Isovector spin-multipole strength distributions in double- β -decay triplets

2017

In this work the energetics and strength distributions of isovector spin-dipole and spin-quadrupole transitions from the ground states of the pairs ($^{76}\mathrm{Ge}, ^{76}\mathrm{Se}$), ($^{82}\mathrm{Se}, ^{82}\mathrm{Kr}$), ($^{96}\mathrm{Zr}, ^{96}\mathrm{Mo}$), ($^{100}\mathrm{Mo}, ^{100}\mathrm{Ru}$), ($^{116}\mathrm{Cd}, ^{116}\mathrm{Sn}$), ($^{128}\mathrm{Te}, ^{128}\mathrm{Xe}$), ($^{130}\mathrm{Te}, ^{130}\mathrm{Xe}$), and ($^{136}\mathrm{Xe}, ^{136}\mathrm{Ba}$), of double-$\ensuremath{\beta}$-decay initial and final nuclei, to the ${J}^{\ensuremath{\pi}}={0}^{\ensuremath{-}},{1}^{\ensuremath{-}},{2}^{\ensuremath{-}},{1}^{+},{2}^{+}$, and ${3}^{+}$ excited states of the interm…

PhysicsValence (chemistry)ta114Isovector010308 nuclear & particles physicsdouble beta decaycollective models01 natural sciencesExcited state0103 physical sciencesQuasiparticlecharge-exchange reactionsAtomic physics010306 general physicsMultipole expansionSpin (physics)Physical Review C
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