Search results for " superconductivity"

showing 10 items of 319 documents

Simulating Terahertz Field-Induced Ferroelectricity in Quantum Paraelectric SrTiO3

2021

Recent experiments have demonstrated that light can induce a transition from the quantum paraelectric to the ferroelectric phase of SrTiO3. Here, we investigate this terahertz field-induced ferroelectric phase transition by solving the time-dependent lattice Schrödinger equation based on first-principles calculations. We find that ferroelectricity originates from a light-induced mixing between ground and first excited lattice states in the quantum paraelectric phase. In agreement with the experimental findings, our study shows that the nonoscillatory second harmonic generation signal can be evidence of ferroelectricity in SrTiO3. We reveal the microscopic details of this exotic phase transi…

Condensed Matter - Materials SciencepressureCondensed Matter::Materials ScienceLight induced phase transitionGeneral Physics and AstronomyMaterials Science (cond-mat.mtrl-sci)FOS: Physical scienceslight induced superconductivitytemperature dependenceSettore FIS/03 - Fisica Della Materia
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Pseudogap in high-temperature superconductors from realistic Fr\"ohlich and Coulomb interactions

2012

It has been recently shown that the competition between unscreened Coulomb and Fr\"{o}hlich electron-phonon interactions can be described in terms of a short-range spin exchange $J_p$ and an effective on-site interaction $\tilde{U}$ in the framework of the polaronic $t$-$J_p$-$\tilde{U}$ model. This model, that provides an explanation for high temperature superconductivity in terms of Bose-Einstein condensation (BEC) of small and light bipolarons, is now studied as a charged Bose-Fermi mixture. Within this approximation, we show that a gap between bipolaron and unpaired polaron bands results in a strong suppression of low-temperature spin susceptibility, specific heat and tunneling conducta…

Condensed Matter::Quantum GasesCondensed Matter - Strongly Correlated ElectronsCondensed Matter::OtherCondensed Matter::SuperconductivityCondensed Matter - SuperconductivityCondensed Matter::Strongly Correlated Electrons
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High temperature superconductivity from realistic long-range Coulomb and Fr\"ohlich interactions

2012

In the last years ample experimental evidence has shown that charge carriers in high-temperature superconductors are strongly correlated but also coupled with lattice vibrations (phonons), signaling that the true origin of high-Tc superconductivity can only be found in a proper combination of Coulomb and electron-phonon interactions. On this basis, we propose and study a model for high-Tc superconductivity, which accounts for realistic Coulomb repulsion, strong electron-phonon (Fr\"ohlich) interaction and residual on-site (Hubbard \tilde{U}) correlations without any ad-hoc assumptions on their relative strength and interaction range. In the framework of this model, which exhibits a phase tr…

Condensed Matter::Quantum GasesCondensed Matter - Strongly Correlated ElectronsCondensed Matter::SuperconductivityCondensed Matter - Superconductivity
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Melting the Superconducting State in the Electron Doped Cuprate Pr$_{1.85}% $Ce$_{0.15}$CuO$_{4-\delta}$ with Intense near-infrared and Terahertz Pul…

2016

We studied the superconducting (SC) state depletion process in an electron doped cuprate Pr$_{1.85}$Ce$_{0.15}$CuO$_{4-\delta}$ by pumping with near-infrared (NIR) and narrow-band THz pulses. When pumping with THz pulses tuned just above the SC gap, we find the absorbed energy density required to deplete superconductivity, $A_{dep}$, matches the thermodynamic condensation energy. Contrary, by NIR pumping $A_{dep}$ is an order of magnitude higher, despite the fact that the SC gap is much smaller than the energy of relevant bosonic excitations. The result implies that only a small subset of bosons contribute to pairing.

Condensed Matter::Quantum GasesCondensed Matter - Strongly Correlated ElectronsCondensed Matter::SuperconductivityCondensed Matter - SuperconductivityPhysics::Optics
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Superlight small bipolarons from realistic long-range Coulomb and Fröhlich interactions

2011

We report analytical and numerical results on the two-particle states of the polaronic t-Jp model derived recently with realistic Coulomb and electron-phonon (Frohlich) interactions in doped polar insulators. Eigenstates and eigenvalues are calculated for two different geometries. Our results show that the ground state is a bipolaronic singlet, made up of two polarons. The bipolaron size increases with increasing ratio of the polaron hopping integral t to the exchange interaction Jp but remains small compared to the system size in the whole range 0<t/Jp<1. Furthermore, the model exhibits a phase transition to a superconducting state with a critical temperature well in excess of 100K. In the…

Condensed Matter::Quantum GasesPhysicsBipolaronCondensed matter physicsCondensed Matter - SuperconductivityExchange interactionCharge (physics)Condensed Matter PhysicsPolaronElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsDensity of statesCoulombCondensed Matter::Strongly Correlated ElectronsGround stateSpin-½Physical Review B
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Quasi-Two-Dimensional Superfluid Fermionic Gases

2005

We study a quasi two-dimensional superfluid Fermi gas where the confinement in the third direction is due to a strong harmonic trapping. We investigate the behavior of such a system when the chemical potential is varied and find strong modifications of the superfluid properties due to the discrete harmonic oscillator states. We show that such quasi two-dimensional behavior can be created and observed with current experimental capabilities.

Condensed Matter::Quantum GasesPhysicsCondensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesGeneral Physics and AstronomyTrappingFermionRoton01 natural sciences010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)SuperfluidityQuantum electrodynamics0103 physical sciencesHarmonicMatter wave010306 general physicsFermi gasHarmonic oscillatorPhysical Review Letters
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Laser-induced collective excitations in a two-component Fermi gas

2002

We consider the linear density response of a two-component (superfluid) Fermi gas of atoms when the perturbation is caused by laser light. We show that various types of laser excitation schemes can be transformed into linear density perturbations, however, a Bragg spectroscopy scheme is needed for transferring energy and momentum into a collective mode. This makes other types of laser probing schemes insensitive for collective excitations and therefore well suited for the detection of the superfluid order parameter. We show that for the special case when laser light is coupled between the two components of the Fermi gas, density response is always absent in a homogeneous system.

Condensed Matter::Quantum GasesPhysicsLinear densityCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter - SuperconductivityFOS: Physical sciencesEnergy–momentum relationLaserAtomic and Molecular Physics and Opticslaw.inventionSuperconductivity (cond-mat.supr-con)SuperfluiditylawMesoscale and Nanoscale Physics (cond-mat.mes-hall)QuasiparticleAtomic physicsFermi gasSpectroscopyExcitationPhysical Review A
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Hartree-Fock-Bogoliubov theory of polarized Fermi systems

2008

Condensed Fermi systems with an odd number of particles can be described by means of polarizing external fields having a time-odd character. We illustrate how this works for Fermi gases and atomic nuclei treated by density functional theory or Hartree-Fock-Bogoliubov (HFB) theory. We discuss the method based on introducing two chemical potentials for different superfluid components, whereby one may change the particle-number parity of the underlying quasiparticle vacuum. Formally, this method is a variant of non-collective cranking, and the procedure is equivalent to the so-called blocking. We present and exemplify relations between the two-chemical-potential method and the cranking approxi…

Condensed Matter::Quantum GasesPhysicsNuclear TheoryCondensed Matter - SuperconductivityNuclear TheoryHartree–Fock methodFOS: Physical sciencesAtomic and Molecular Physics and OpticsSuperconductivity (cond-mat.supr-con)Nuclear Theory (nucl-th)SuperfluidityQuantum mechanicsQuantum electrodynamicsAtomic nucleusQuasiparticleParity (mathematics)Nuclear theoryFermi Gamma-ray Space TelescopePhysical Review A
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Quasiparticles and quantum phase transition in universal low-temperature properties of heavy-fermion metals

2006

We demonstrate, that the main universal features of the low temperature experimental $H-T$ phase diagram of CeCoIn5 and other heavy-fermion metals can be well explained using Landau paradigm of quasiparticles. The main point of our theory is that above quasiparticles form so-called fermion-condensate state, achieved by a fermion condensation quantum phase transition (FCQPT). When a heavy fermion liquid undergoes FCQPT, the fluctuations accompanying above quantum critical point are strongly suppressed and cannot destroy the quasiparticles. The comparison of our theoretical results with experimental data on CeCoIn5 have shown that the electronic system of above substance provides a unique opp…

Condensed Matter::Quantum GasesPhysicsQuantum phase transitionStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsCondensed Matter - SuperconductivityCondensationFOS: Physical sciencesGeneral Physics and AstronomyFermionSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsQuantum critical pointHeavy fermionQuasiparticleCondensed Matter::Strongly Correlated ElectronsElectronic systemsPhase diagramEurophysics Letters (EPL)
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Momentum-dependent pseudogaps in the half-filled two-dimensional Hubbard model

2012

We compute unbiased spectral functions of the two-dimensional Hubbard model by extrapolating Green functions, obtained from determinantal quantum Monte Carlo simulations, to the thermodynamic and continuous time limits. Our results clearly resolve the pseudogap at weak to intermediate coupling, originating from a momentum selective opening of the charge gap. A characteristic pseudogap temperature T*, determined consistently from the spectra and from the momentum dependence of the imaginary-time Green functions, is found to match the dynamical mean-field critical temperature, below which antiferromagnetic fluctuations become dominant. Our results identify a regime where pseudogap physics is …

Condensed Matter::Quantum GasesPhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsHubbard modelCondensed Matter - SuperconductivityQuantum Monte CarloFOS: Physical sciencesCharge (physics)FermionCondensed Matter PhysicsCoupling (probability)Electronic Optical and Magnetic MaterialsSuperconductivity (cond-mat.supr-con)MomentumCondensed Matter - Strongly Correlated ElectronsQuantum Gases (cond-mat.quant-gas)Condensed Matter::Strongly Correlated ElectronsStrongly correlated materialCondensed Matter - Quantum GasesPseudogapPhysical Review B
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