Search results for "BOSON"

showing 10 items of 1360 documents

Correlation Dynamics During a Slow Interaction Quench in a One-Dimensional Bose Gas

2014

We investigate the response of a one-dimensional Bose gas to a slow increase of its interaction strength. We focus on the rich dynamics of equal-time single-particle correlations treating the Lieb-Liniger model within a bosonization approach and the Bose-Hubbard model using the time-dependent density-matrix renormalization group method. For short distances, correlations follow a power-law with distance with an exponent given by the adiabatic approximation. In contrast, for long distances, correlations decay algebraically with an exponent understood within the sudden quench approximation. This long distance regime is separated from an intermediate distance one by a generalized Lieb-Robinson …

BosonizationPhysicsCondensed Matter::Quantum GasesLieb-Robinson boundBose gas[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]General Physics and AstronomyFOS: Physical sciencesTomonaga-Luttinger LiquidRenormalization groupPower lawExponential functionAdiabatic theoremequal-time Green's functionsQuantum Gases (cond-mat.quant-gas)Light coneQuantum mechanicsinteraction quenchExponentCondensed Matter - Quantum GasesPACS: 67.85.−d 03.75.Kk 03.75.Lm 67.25.D−
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Quantum criticality on a chiral ladder: An SU(2) infinite density matrix renormalization group study

2019

In this paper we study the ground-state properties of a ladder Hamiltonian with chiral $\text{SU}(2)$-invariant spin interactions, a possible first step toward the construction of truly two-dimensional nontrivial systems with chiral properties starting from quasi-one-dimensional ones. Our analysis uses a recent implementation by us of $\text{SU}(2)$ symmetry in tensor network algorithms, specifically for infinite density matrix renormalization group. After a preliminary analysis with Kadanoff coarse graining and exact diagonalization for a small-size system, we discuss its bosonization and recap the continuum limit of the model to show that it corresponds to a conformal field theory, in agr…

BosonizationPhysicsConformal field theoryDensity matrix renormalization group02 engineering and technologyQuantum entanglementRenormalization group021001 nanoscience & nanotechnology01 natural sciences0103 physical sciencesddc:530Algebraic number010306 general physics0210 nano-technologyScalingSpecial unitary groupMathematical physics
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Topological Devil's staircase in atomic two-leg ladders

2019

Abstract We show that a hierarchy of topological phases in one dimension—a topological Devil’s staircase—can emerge at fractional filling fractions in interacting systems, whose single-particle band structure describes a topological or a crystalline topological insulator. Focusing on a specific example in the BDI class, we present a field-theoretical argument based on bosonization that indicates how the system, as a function of the filling fraction, hosts a series of density waves. Subsequently, based on a numerical investigation of the low-lying energy spectrum, Wilczek–Zee phases, and entanglement spectra, we show that they are symmetry protected topological phases. In sharp contrast to t…

Bosonizationcold-atoms; fractional topological phase; strongly correlated; two-leg ladderGeneral Physics and AstronomyFOS: Physical sciencesQuantum entanglementcold-atomTopology01 natural sciencesSettore FIS/03 - Fisica della Materia010305 fluids & plasmasUltracold atom0103 physical sciencesddc:530Limit (mathematics)010306 general physicsElectronic band structurePhysicsstrongly correlatedSeries (mathematics)Symmetry (physics)cold-atomsQuantum Gases (cond-mat.quant-gas)Topological insulatorfractional topological phaseCondensed Matter - Quantum Gasestwo-leg ladder
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Adiabatic-antiadiabatic crossover in a spin-Peierls chain

2004

We consider an XXZ spin-1/2 chain coupled to optical phonons with non-zero frequency $\omega_0$. In the adiabatic limit (small $\omega_0$), the chain is expected to spontaneously dimerize and open a spin gap, while the phonons become static. In the antiadiabatic limit (large $\omega_0$), phonons are expected to give rise to frustration, so that dimerization and formation of spin-gap are obtained only when the spin-phonon interaction is large enough. We study this crossover using bosonization technique. The effective action is solved both by the Self Consistent Harmonic Approximation (SCHA)and by Renormalization Group (RG) approach starting from a bosonized description. The SCHA allows to an…

Bosonizationmedia_common.quotation_subjectFOS: Physical sciencesFrustrationddc:500.201 natural sciencesOmega010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsCondensed Matter::Superconductivity0103 physical sciences[PHYS.COND.CM-SM]Physics [physics]/Condensed Matter [cond-mat]/Statistical Mechanics [cond-mat.stat-mech]010306 general physicsCondensed Matter - Statistical MechanicsSpin-½media_commonCoupling constantPhysicsStrongly Correlated Electrons (cond-mat.str-el)Statistical Mechanics (cond-mat.stat-mech)Condensed matter physicsOrder (ring theory)Renormalization groupCondensed Matter PhysicsCoupling (probability)Electronic Optical and Magnetic Materials75.10.Pq 63.70.+hCondensed Matter::Strongly Correlated Electrons[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]
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Deformation and mixing of coexisting shapes in neutron-deficient polonium isotopes

2015

Coulomb-excitation experiments are performed with postaccelerated beams of neutron-deficient Po196,198,200,202 isotopes at the REX-ISOLDE facility. A set of matrix elements, coupling the low-lying states in these isotopes, is extracted. In the two heaviest isotopes, Po200,202, the transitional and diagonal matrix elements of the 2+1 state are determined. In Po196,198 multistep Coulomb excitation is observed, populating the 4+1,0+2, and 2+2 states. The experimental results are compared to the results from the measurement of mean-square charge radii in polonium isotopes, confirming the onset of deformation from Po196 onwards. Three model descriptions are used to compare to the data. Calculati…

CHARGE RADIINuclear and High Energy PhysicsTRANSITION-PROBABILITYchemistry.chemical_elementCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciences114 Physical sciencessymbols.namesakeMatrix (mathematics)NUCLEAR-DATA SHEETSCOULOMB-EXCITATION0103 physical sciencesSTATE PROPERTIESNuclear Physics - ExperimentNeutronfysiikka010306 general physicsEVEN-EVEN NUCLIDESMixing (physics)isotopesPoloniumINTRUDER STATESGAMMA-RAY SPECTROSCOPYPhysicsSPIN STATESisotoopitPO ISOTOPESIsotopeta114010308 nuclear & particles physicsBohr modelchemistryPhysics and AstronomysymbolsAtomic physicsInteracting boson modelphysicspolonium25.70.De 23.20.Js 25.60.−t 27.80.+w
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Measurement and interpretation of the $W$-pair cross-section in $e^+e^-$ interactions at 161 GeV

1997

In 1996 LEP ran at a centre-of-mass energy of 161~GeV, just above the threshold of W-pair production. DELPHI accumulated data corresponding to an integrated luminosity of $9.93 {\mathrm{~pb^{-1}}}$, and observed 29 events that are considered as candidates for W-pair production. From these, a cross-section for the doubly resonant $e^+e^-\to\mathrm{WW}$ process of $3.67~^{+0.97}_{-0.85} \pm 0.19{\mathrm{~pb}}$ has been measured. Within the Standard Model, this cross-section corresponds to a mass of the W-boson of ${\mathrm{80.40~\pm~0.44~(stat.)~\pm~0.09~(syst.) ~\pm 0.03~(LEP)~GeV}}/c^2$. Alternatively, if $m_{\mathrm{W}}$ is held fixed at its current value determined by other experiments, t…

COLLISIONSNuclear and High Energy PhysicsParticle physicsElectron–positron annihilation01 natural sciencesBOSON MASS; ROOT-S=1.8 TEV; COLLISIONS; COUPLINGSPartícules (Física nuclear)Standard ModelInterpretation (model theory)Nuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsDetectors de radiacióDELPHIPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsROOT-S=1.8 TEVCOUPLINGSLARGE ELECTRON POSITRON COLLIDERBOSON MASSCross section (geometry)PARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentParticle Physics - ExperimentPhysics Letters B
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Search for neutral heavy leptons produced in Z decays

1997

Weak isosinglet Neutral Heavy Leptons ($\nu_m$) have been searched for using data collected by the DELPHI detector corresponding to $3.3\times 10^{6}$ hadronic~Z$^{0}$ decays at LEP1. Four separate searches have been performed, for short-lived $\nu_m$ production giving monojet or acollinear jet topologies, and for long-lived $\nu_m$ giving detectable secondary vertices or calorimeter clusters. No indication of the existence of these particles has been found, leading to an upper limit for the branching ratio $BR($Z$^0\rightarrow \nu_m \overline{\nu})$ of about $1.3\times10^{-6}$ at 95\% confidence level for $\nu_m$ masses between 3.5 and 50 GeV/$c^2$. Outside this range the limit weakens rap…

COLLISIONSParticle physicsE+E ANNIHILATIONPhysics and Astronomy (miscellaneous)Electron–positron annihilationHadronMASSJet (particle physics)HIGH-ENERGY-PHYSICS; MONOJET PRODUCTION; E+E ANNIHILATION; MONTE-CARLO; BOSON; LIMITS; MASS; LEP; PERFORMANCE; COLLISIONSHIGH-ENERGY-PHYSICS01 natural sciences7. Clean energyMONOJET PRODUCTIONNuclear physicsLIMITSMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsDELPHIBosonPhysics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyBOSONLEPPERFORMANCELARGE ELECTRON POSITRON COLLIDERPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderPARTICLE PHYSICSHigh Energy Physics::ExperimentNeutrinoParticle Physics - ExperimentLepton
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Appearances of pseudo-bosons from Black-Scholes equation

2016

It is a well known fact that the Black-Scholes equation admits an alternative representation as a Schr\"odinger equation expressed in terms of a non self-adjoint hamiltonian. We show how {\em pseudo-bosons}, linear or not, naturally arise in this context, and how they can be used in the computation of the pricing kernel.

ComputationFOS: Physical sciencesStatistical and Nonlinear PhysicsBlack–Scholes modelMathematical Physics (math-ph)Mathematics::Spectral Theory01 natural sciences010305 fluids & plasmasSchrödinger equationsymbols.namesakeStochastic discount factor0103 physical sciencessymbols010306 general physicsHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaMathematical PhysicsStatistical and Nonlinear PhysicBosonMathematical physicsMathematics
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Pseudo-bosons and Riesz Bi-coherent States

2016

After a brief review on D-pseudo-bosons we introduce what we call Riesz bi-coherent states, which are pairs of states sharing with ordinary coherent states most of their features. In particular, they produce a resolution of the identity and they are eigenstates of two different annihilation operators which obey pseudo-bosonic commutation rules.

Condensed Matter::Quantum GasesIdentity (mathematics)Theoretical physicsAnnihilationRiesz representation theoremQuantum mechanicsCoherent statesCommutationEigenvalues and eigenvectorsMathematicsResolution (algebra)Boson
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Nuclear structure of97Yin the interacting boson fermion plus broken pair model and the nature of the 3.523 MeV high-spin isomer

1998

Nuclear structure of 97Y is described in the interacting boson fermion plus broken pair model, including quasiproton and quasiproton-two-quasineutron configurations in the basis states. In particular, the yrast bands and the decay of the 27/2- high-spin isomer are accounted for in this approach.

Condensed Matter::Quantum GasesNuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsBasis (linear algebra)YrastNuclear structureFermionSpin (physics)BosonPhysical Review C
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