0000000001084358

AUTHOR

Edmond Orignac

showing 11 related works from this author

Polarization angle dependence of the breathing modes in confined one-dimensional dipolar bosons

2021

Probing the radial collective oscillation of a trapped quantum system is an accurate experimental tool to investigate interactions and dimensionality effects. We consider a fully polarized quasi-one dimensional dipolar quantum gas of bosonic dysprosium atoms in a parabolic trap at zero temperature. We model the dipolar gas with an effective quasi-one dimensional Hamiltonian in the single-mode approximation, and derive the equation of state using a variational approximation based on the Lieb-Liniger gas Bethe Ansatz wavefunction or perturbation theory. We calculate the breathing mode frequencies while varying polarization angles by a sum-rule approach, and find them in good agreement with re…

[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]FOS: Physical sciences02 engineering and technology01 natural sciencescollective modesBethe ansatzSupersolidsymbols.namesakedipolar gas supersoliddipolar gas0103 physical sciencesQuantum systemtrapped atoms010306 general physicsWave functionUltracold atoms - Dipolar atoms - Luttinger liquidsBosonPhysicsCondensed Matter::Quantum Gasesdipolar interactionsBrewster's angle021001 nanoscience & nanotechnologyPolarization (waves)3. Good healthsupersolidQuantum Gases (cond-mat.quant-gas)Quantum electrodynamicssymbols0210 nano-technologyHamiltonian (quantum mechanics)Condensed Matter - Quantum Gases
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Response functions in multicomponent Luttinger liquids

2012

We derive an analytic expression for the zero temperature Fourier transform of the density-density correlation function of a multicomponent Luttinger liquid with different velocities. By employing Schwinger identity and a generalized Feynman identity exact integral expressions are derived, and approximate analytical forms are given for frequencies close to each component singularity. We find power-like singularities and compute the corresponding exponents. Numerical results are shown for the case of three components.

Statistics and ProbabilityBosonizationFOS: Physical sciences01 natural sciences010305 fluids & plasmassymbols.namesakeIdentity (mathematics)Condensed Matter - Strongly Correlated ElectronsSingularityCorrelation functionLuttinger liquid0103 physical sciencesFeynman diagramLuttinger liquids (theory)010306 general physics71.10.Pm 02.30.Nw 02.30.UuMathematical physicsPhysicsStrongly Correlated Electrons (cond-mat.str-el)Statistical and Nonlinear PhysicsFourier transformsymbolsGravitational singularityStatistics Probability and Uncertaintybosonization[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]
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Accessing finite momentum excitations of the one-dimensional Bose-Hubbard model using superlattice modulation spectroscopy

2018

We investigate the response to superlattice modulation of a bosonic quantum gas confined to arrays of tubes emulating the one-dimensional Bose-Hubbard model. We demonstrate, using both time-dependent density matrix renormalization group and linear response theory, that such a superlattice modulation gives access to the excitation spectrum of the Bose-Hubbard model at finite momenta. Deep in the Mott-insulator, the response is characterized by a narrow energy absorption peak at a frequency approximately corresponding to the onsite interaction strength between bosons. This spectroscopic technique thus allows for an accurate measurement of the effective value of the interaction strength. On th…

BosonizationPhysicsCondensed Matter::Quantum GasesCondensed matter physics[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Density matrix renormalization groupMott insulatorSuperlatticeFOS: Physical sciencesBose–Hubbard model01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasSuperfluidityBose-Hubbard modelQuantum Gases (cond-mat.quant-gas)Atomic and Molecular PhysicsDMRG0103 physical sciencesBosonizationand Optics010306 general physicsCondensed Matter - Quantum GasesFrequency modulationBoson
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Probing the bond order wave phase transitions of the ionic Hubbard model by superlattice modulation spectroscopy

2017

An exotic phase, the bond order wave, characterized by the spontaneous dimerization of the hopping, has been predicted to exist sandwiched between the band and Mott insulators in systems described by the ionic Hubbard model. Despite growing theoretical evidences, this phase still evades experimental detection. Given the recent realization of the ionic Hubbard model in ultracold atomic gases, we propose here to detect the bond order wave using superlattice modulation spectroscopy. We demonstrate, with the help of time-dependent density-matrix renormalization group and bosonization, that this spectroscopic approach reveals characteristics of both the Ising and Kosterlitz-Thouless transitions …

BosonizationHubbard model[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]SuperlatticeGeneral Physics and AstronomyIonic bondingFOS: Physical sciences01 natural sciencesCondensed Matter - Strongly Correlated ElectronsPhysics and Astronomy (all)0103 physical sciencesBosonizationCold atoms010306 general physicsPhysicsCondensed Matter::Quantum GasesCondensed matter physicsDensity Matrix Renormalization GroupStrongly Correlated Electrons (cond-mat.str-el)010308 nuclear & particles physicsMott insulatorBerezinskii-Kosterlitz-Thouless transitionIsing transitionRenormalization groupBond orderQuantum Gases (cond-mat.quant-gas)Ising modelCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum Gases
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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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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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Polar bosons in one-dimensional disordered optical lattices

2013

We analyze the effects of disorder and quasi-disorder on the ground-state properties of ultra-cold polar bosons in optical lattices. We show that the interplay between disorder and inter-site interactions leads to rich phase diagrams. A uniform disorder leads to a Haldane-insulator phase with finite parity order, whereas the density-wave phase becomes a Bose-glass at very weak disorder. For quasi-disorder, the Haldane insulator connects with a gapped generalized incommesurate density wave without an intermediate critical region.

Anderson localization[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]PACS : 67.85.-d 05.30.Jp 61.44.Fw 75.10.PqFOS: Physical sciences01 natural sciencesCondensed Matter::Disordered Systems and Neural NetworksUltracold atoms010305 fluids & plasmasDensity wave theoryCondensed Matter - Strongly Correlated ElectronsUltracold atomQuantum mechanics0103 physical sciencesAnderson localization010306 general physicsBosonPhase diagramPhysicsCondensed Matter::Quantum Gasesdipolar interactionsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Parity (physics)Disordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksAubry-André transitionCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsQuantum Gases (cond-mat.quant-gas)PolarCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum Gases
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Variational Bethe ansatz approach for dipolar one-dimensional bosons

2020

We propose a variational approximation to the ground state energy of a one-dimensional gas of interacting bosons on the continuum based on the Bethe Ansatz ground state wavefunction of the Lieb-Liniger model. We apply our variational approximation to a gas of dipolar bosons in the single mode approximation and obtain its ground state energy per unit length. This allows for the calculation of the Tomonaga-Luttinger exponent as a function of density and the determination of the structure factor at small momenta. Moreover, in the case of attractive dipolar interaction, an instability is predicted at a critical density, which could be accessed in lanthanide atoms.

[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Dipolar interactionsFOS: Physical sciences02 engineering and technologyGas atomici interagenti01 natural sciencesBethe ansatzVariational methods in quantum mechanicsCondensed Matter - Strongly Correlated ElectronsQuantum mechanics0103 physical sciencesLieb–Liniger model010306 general physicsWave function[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesLieb-Liniger modelStrongly Correlated Electrons (cond-mat.str-el)one dimensional bosonsFunction (mathematics)021001 nanoscience & nanotechnologyQuantum Gases (cond-mat.quant-gas)Exponent[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]0210 nano-technologyStructure factorGround stateCondensed Matter - Quantum Gases
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Incommensurate phases of a bosonic two-leg ladder under a flux

2016

A boson two--leg ladder in the presence of a synthetic magnetic flux is investigated by means of bosonization techniques and Density Matrix Renormalization Group (DMRG). We follow the quantum phase transition from the commensurate Meissner to the incommensurate vortex phase with increasing flux at different fillings. When the applied flux is $\rho \pi$ and close to it, where $\rho$ is the filling per rung, we find a second incommensuration in the vortex state that affects physical observables such as the momentum distribution, the rung-rung correlation function and the spin-spin and charge-charge static structure factors.

Quantum phase transitionBosonizationBosonisation[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]IncommensurationsFOS: Physical sciencesGeneral Physics and Astronomychamps de jauge artificiels01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)Condensed Matter - Strongly Correlated ElectronsCorrelation functionGauge fieldsCondensed Matter::Superconductivity0103 physical sciencesBosonizationtranstion commensurable-incommensurable010306 general physicsCommensurate-Incommensurate transitions[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsartificial gauge fieldsDensity matrix renormalization groupGauge fields; Incommensurations; Meissner to vortex transition; Physics and Astronomy (all)Vortex stateMagnetic fluxVortexQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality.Quantum Gases (cond-mat.quant-gas)Meissner to vortex transitionCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality
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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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Statics and dynamics of weakly coupled antiferromagnetic spin-1/2 ladders in a magnetic field

2011

We investigate weakly coupled spin-1/2 ladders in a magnetic field. The work is motivated by recent experiments on the compound (C5H12N)2CuBr4 (BPCB). We use a combination of numerical and analytical methods, in particular the density matrix renormalization group (DMRG) technique, to explore the phase diagram and the excitation spectra of such a system. We give detailed results on the temperature dependence of the magnetization and the specific heat, and the magnetic field dependence of the nuclear magnetic resonance (NMR) relaxation rate of single ladders. For coupled ladders, treating the weak interladder coupling within a mean-field or quantum Monte Carlo approach, we compute the transit…

Strongly Correlated Electrons (cond-mat.str-el)neutronsFOS: Physical sciencesddc:500.2NMRCondensed Matter - Strongly Correlated ElectronsLuttinger liquidspin-1/2 laddersDMRG[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]PACS: 75.10.Jm 75.40.Gb 75.40.Cx 75.30.KzCondensed Matter::Strongly Correlated Electronsbosonization[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]
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