Search results for "Condensed Matter - Strongly Correlated Electrons"

showing 10 items of 322 documents

Uhlmann number in translational invariant systems

2019

We define the Uhlmann number as an extension of the Chern number, and we use this quantity to describe the topology of 2D translational invariant Fermionic systems at finite temperature. We consider two paradigmatic systems and we study the changes in their topology through the Uhlmann number. Through the linear response theory we linked two geometrical quantities of the system, the mean Uhlmann curvature and the Uhlmann number, to directly measurable physical quantities, i.e. the dynamical susceptibility and to the dynamical conductivity, respectively.

0301 basic medicineSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciMathematics::Analysis of PDEsFOS: Physical scienceslcsh:MedicineCurvatureArticleCondensed Matter - Strongly Correlated Electrons03 medical and health sciences0302 clinical medicineTopological insulatorsInvariant (mathematics)lcsh:ScienceCondensed Matter - Statistical MechanicsMathematicsMathematical physicsPhysical quantityQuantum PhysicsMultidisciplinaryChern classStatistical Mechanics (cond-mat.stat-mech)Strongly Correlated Electrons (cond-mat.str-el)lcsh:RUhlmann number Chern number 2D topological Fermionic systems finite temperature dynamical susceptibility dynamical conductivity030104 developmental biologylcsh:QQuantum Physics (quant-ph)Theoretical physicsLinear response theory030217 neurology & neurosurgeryScientific Reports
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Strong enhancement of superconductivity at high pressures within the charge-density-wave states of 2H-TaS 2 and 2H-TaSe 2

2016

We present measurements of the superconducting and charge density wave critical temperatures (Tc and TCDW) as a function of pressure in the transition metal dichalchogenides 2H-TaSe2 and 2H-TaS2. Resistance and susceptibility measurements show that Tc increases from temperatures below 1 K up to 8.5 K at 9.5 GPa in 2H-TaS2 and 8.2 K at 23 GPa in 2H-TaSe2. We observe a kink in the pressure dependence of TCDW at about 4 GPa that we attribute to the lock-in transition from incommensurate CDW to commensurate CDW. Above this pressure, the commensurate TCDW slowly decreases coexisting with superconductivity within our full pressure range.

7470Xa[PHYS.COND.CM-S]Physics [physics]/Condensed Matter [cond-mat]/Superconductivity [cond-mat.supr-con]Superconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - SuperconductivityFOS: Physical sciences7445Lr7425Dw[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]
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Internal-strain mediated coupling between polar Bi and magnetic Mn ions in the defect-free quadruple-perovskite BiMn$_3$Mn$_4$O$_{12}$

2011

By means of neutron powder diffraction, we investigated the effect of the polar Bi$^{3+}$ ion on the magnetic ordering of the Mn$^{3+}$ ions in BiMn$_3$Mn$_4$O$_{12}$, the counterpart with \textit{quadruple} perovskite structure of the \textit{simple} perovskite BiMnO$_3$. The data are consistent with a \textit{noncentrosymmetric} spacegroup $Im$ which contrasts the \textit{centrosymmetric} one $I2/m$ previously reported for the isovalent and isomorphic compound LaMn$_3$Mn$_4$O$_{12}$, which gives evidence of a Bi$^{3+}$-induced polarization of the lattice. At low temperature, the two Mn$^{3+}$ sublattices of the $A'$ and $B$ sites order antiferromagnetically (AFM) in an independent manner …

75.47.LxCondensed Matter - Strongly Correlated Electrons75.80.+qStrongly Correlated Electrons (cond-mat.str-el)75.25.-jFOS: Physical sciences75.85.+t
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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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Compact two-electron wave function for bond dissociation and Van der Waals interactions: A natural amplitude assessment

2014

Electron correlations in molecules can be divided in short range dynamical correlations, long range Van der Waals type interactions and near degeneracy static correlations. In this work we analyze for a one-dimensional model of a two-electron system how these three types of correlations can be incorporated in a simple wave function of restricted functional form consisting of an orbital product multiplied by a single correlation function $f(r_{12})$ depending on the interelectronic distance $r_{12}$. Since the three types of correlations mentioned lead to different signatures in terms of the natural orbital (NO) amplitudes in two-electron systems we make an analysis of the wave function in t…

Atomic Physics (physics.atom-ph)General Physics and AstronomyFOS: Physical sciencesPhysics - Atomic Physicssymbols.namesakeCondensed Matter - Strongly Correlated ElectronsAtomic orbitalQuantum mechanicsPhysics - Chemical PhysicsPhysics::Atomic PhysicsSDG 7 - Affordable and Clean EnergyPhysical and Theoretical ChemistryWave functionAnsatzPhysicsChemical Physics (physics.chem-ph)Quantum Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyta114Electronic correlationStrongly Correlated Electrons (cond-mat.str-el)Computational Physics (physics.comp-ph)Diatomic molecule3. Good healthBond lengthAmplitudesymbolsvan der Waals forceQuantum Physics (quant-ph)Physics - Computational Physics
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Long-range interactions and the sign of natural amplitudes in two-electron systems

2013

In singlet two-electron systems the natural occupation numbers of the one-particle reduced density matrix are given as squares of the natural amplitudes which are defined as the expansion coefficients of the two-electron wave function in a natural orbital basis. In this work we relate the sign of the natural amplitudes to the nature of the two-body interaction. We show that long-range Coulomb-type interactions are responsible for the appearance of positive amplitudes and give both analytical and numerical examples that illustrate how the long-distance structure of the wave function affects these amplitudes. We further demonstrate that the amplitudes show an avoided crossing behavior as func…

Atomic Physics (physics.atom-ph)General Physics and AstronomyInteraction strengthFOS: Physical sciences02 engineering and technologyElectron01 natural sciencesPhysics - Atomic PhysicsCondensed Matter - Strongly Correlated Electronssymbols.namesakeQuantum mechanics0103 physical sciencesCoulombPhysical and Theoretical ChemistryWave functionPhysicsQuantum Physicsta114010304 chemical physicsStrongly Correlated Electrons (cond-mat.str-el)Avoided crossingComputational Physics (physics.comp-ph)021001 nanoscience & nanotechnologyAmplitudesymbolsReduced density matrix0210 nano-technologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Physics - Computational Physics
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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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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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Thermal entanglement of a spin-1/2 Ising–Heisenberg model on a symmetrical diamond chain

2011

International audience; The entanglement quantum properties of a spin-1/2 Ising-Heisenberg model on a symmetrical diamond chain were analyzed. Due to the separable nature of the Ising-type exchange interactions between neighboring Heisenberg dimers, calculation of the entanglement can be performed exactly for each individual dimer. Pairwise thermal entanglement was studied in terms of the isotropic Ising-Heisenberg model and analytical expressions for the concurrence (as a measure of bipartite entanglement) were obtained. The effects of external magnetic field H and next-nearest neighbor interaction J(m) between nodal Ising sites were considered. The ground state structure and entanglement …

CRYPTOGRAPHYFOS: Physical sciences02 engineering and technologyQuantum entanglement01 natural sciencesCondensed Matter - Strongly Correlated ElectronsMAGNETIC-PROPERTIESSYSTEMSQuantum mechanics0103 physical sciencesGeneral Materials ScienceFIELD010306 general physicsSpin (physics)QuantumANTIFERROMAGNETSPhysicsCoupling constantCOMPOUND CU-3(CO3)(2)(OH)(2)Strongly Correlated Electrons (cond-mat.str-el)Heisenberg modelQUANTUM ENTANGLEMENTConcurrenceQuantum Physics021001 nanoscience & nanotechnologyCondensed Matter PhysicsCondensed Matter - Other Condensed MatterSTATESFRUSTRATIONIsing model0210 nano-technologyGround stateOther Condensed Matter (cond-mat.other)Journal of Physics: Condensed Matter
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Anomalous High-Pressure Jahn-Teller Behavior inCuWO4

2012

High-pressure optical-absorption measurements performed in CuWO4 up to 20 GPa provide experimental evidence of the persistence of the Jahn-Teller (JT) distortion in the whole pressure range both in the low-pressure triclinic and in the highpressure monoclinic phase. The electron-lattice coupling associated with the eg(Exe) and t2g(Txe) orbitals of Cu2+ in CuWO4 are obtained from correlations between the JT distortion of the CuO6 octahedron and the associated structure of Cu2+ d-electronic levels. This distortion and its associated JT energy (EJT) decrease upon compression in both phases. However, both the distortion and associated EJT increase sharply at the phase transition pressure (PT = …

Chemical Physics (physics.chem-ph)Condensed Matter - Materials ScienceMaterials scienceStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsJahn–Teller effectMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral Physics and AstronomyTriclinic crystal systemCondensed Matter - Strongly Correlated ElectronsAtomic orbitalOctahedronPhysics - Chemical PhysicsDistortionPhase (matter)MultiferroicsMonoclinic crystal systemPhysical Review Letters
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