Search results for "quantum phase transition"

showing 10 items of 100 documents

Phase diagram of a model adsorbate with internal quantum states

1992

Abstract An adsorbate in the strong binding and small corrugation limit is studied. The resulting two-dimensional fluid is treated in the adiabatic approximation: the translations of the heavy molecules are treated classically, whereas the molecular quantum degrees of freedom are modelled by interacting two state tunneling systems. The complete temperature/coverage phase diagram is obtained to a high degree of precision by a new combination of finite size scaling ideas with Path Integral Monte Carlo techniques. Even this simplified adsorbate model possesses a surprisingly complex phase diagram including first- and second-order transitions as well as tricritical and triple points. We identif…

Quantum phase transitionPhysicsCondensed matter physicsDegrees of freedom (physics and chemistry)Surfaces and InterfacesCondensed Matter PhysicsSurfaces Coatings and FilmsAdiabatic theoremQuantum statePhase (matter)Materials ChemistryPath integral Monte CarloQuantum tunnellingPhase diagramSurface Science
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Magnetic breakdown and charge density wave formation: a quantum oscillation study of the rare-earth tritellurides

2020

The rare-earth tritellurides ($R$Te$_3$, where $R$ = La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Y) form a charge density wave state consisting of a single unidirectional charge density wave for lighter $R$, with a second unidirectional charge density wave, perpendicular and in addition to the first, also present at low temperatures for heavier $R$. We present a quantum oscillation study in magnetic fields up to 65T that compares the single charge density wave state with the double charge density wave state both above and below the magnetic breakdown field of the second charge density wave. In the double charge density wave state it is observed that there remain several small, light pockets…

Quantum phase transitionPhysicsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Rare earthQuantum oscillationsFOS: Physical sciencesModel systemFermi surface02 engineering and technologyMagnetic breakdown021001 nanoscience & nanotechnology01 natural sciencesCondensed Matter - Strongly Correlated ElectronsEffective mass (solid-state physics)0103 physical sciences010306 general physics0210 nano-technologyCharge density wave
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Quantum repulsive Nonlinear Schrödinger models and their ‘Superconductivity’

1995

Abstract The fundamental role played by the quantum repulsive Nonlinear Schrodinger (NLS) equation in the evolution of our understanding of the phenomenon of superconductivity in appropriate metals at very low temperatures is surveyed. The first major work was that in 1947 by N. N. Bogoliubov, who studied the very physical 3-space-dimensions problem and super fluidity; and the survey takes the form of an actual dedication to that outstanding scientist who died four years ago. The 3-space-dimensions NLS equation is not integrable either classically or quantum mechanically. But a number of recently discovered closely related lattices in one space dimension (one space plus one time dimension) …

Quantum phase transitionPhysicsGeneral MathematicsApplied MathematicsQuantum dynamicsGeneral Physics and AstronomyStatistical and Nonlinear Physicssymbols.namesakeTheoretical physicsQuantum mechanicsQuantum processsymbolsQuantum operationQuantum inverse scattering methodQuantum dissipationQuantumSchrödinger's catChaos, Solitons & Fractals
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Characterization of the shape-staggering effect in mercury nuclei

2018

In rare cases, the removal of a single proton (Z) or neutron (N) from an atomic nucleus leads to a dramatic shape change. These instances are crucial for understanding the components of the nuclear interactions that drive deformation. The mercury isotopes (Z = 80) are a striking example1,2: their close neighbours, the lead isotopes (Z = 82), are spherical and steadily shrink with decreasing N. The even-mass (A = N + Z) mercury isotopes follow this trend. The odd-mass mercury isotopes 181,183,185Hg, however, exhibit noticeably larger charge radii. Due to the experimental difficulties of probing extremely neutron-deficient systems, and the computational complexity of modelling such heavy nucl…

Quantum phase transitionPhysicsIsotope010308 nuclear & particles physicsNuclear TheoryGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences3100Atomic orbital13. Climate action0103 physical sciencesAtomic nucleusQuadrupoleNuclear Physics - ExperimentNeutronNuclidePräzisionsexperimente - Abteilung BlaumAtomic physics010306 general physicsSpectroscopyNuclear Experiment
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Critical-Point Boundary for the Nuclear Quantum Phase Transition NearA=100from Mass Measurements ofKr96,97

2010

Mass measurements of (96,97)Kr using the ISOLTRAP Penning-trap spectrometer at CERN-ISOLDE are reported, extending the mass surface beyond N=60 for Z=36. These new results show behavior in sharp contrast to the heavier neighbors where a sudden and intense deformation is present. We interpret this as the establishment of a nuclear quantum phase transition critical-point boundary. The new masses confirm findings from nuclear mean-square charge-radius measurements up to N=60 but are at variance with conclusions from recent gamma-ray spectroscopy.

Quantum phase transitionPhysicsIsotopeSpectrometer010308 nuclear & particles physicsGeneral Physics and AstronomyIsotopes of krypton01 natural sciencesISOLTRAPCritical point (thermodynamics)0103 physical sciencesGamma spectroscopyAtomic physicsNuclear Experiment010306 general physicsSpectroscopyPhysical Review Letters
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Magnetic-field-induced reentrance of Fermi-liquid behavior and spin-lattice relaxation rates in

2009

Abstract A strong departure from Landau–Fermi liquid (LFL) behavior have been recently revealed in observed anomalies in both the magnetic susceptibility χ and the muon and 63Cu nuclear spin-lattice relaxation rates 1 / T 1 of YbCu 5 − x Au x ( x = 0.6 ). We show that the above anomalies along with magnetic-field-induced reentrance of LFL properties are indeed determined by the dependence of the quasiparticle effective mass M ∗ on magnetic field B and temperature T and demonstrate that violations of the Korringa law also come from M ∗ ( B , T ) dependence. We obtain this dependence theoretically utilizing our approach based on fermion condensation quantum phase transition (FCQPT) notion. Ou…

Quantum phase transitionPhysicsMagnetoresistanceCondensed matter physicsSpin–lattice relaxationGeneral Physics and Astronomy01 natural sciencesMagnetic susceptibility010305 fluids & plasmasEffective mass (solid-state physics)0103 physical sciencesQuasiparticleStrongly correlated materialFermi liquid theory010306 general physicsPhysics Letters A
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Energy scales and magnetoresistance at a quantum critical point

2009

The magnetoresistance (MR) of CeCoIn_5 is notably different from that in many conventional metals. We show that a pronounced crossover from negative to positive MR at elevated temperatures and fixed magnetic fields is determined by the scaling behavior of quasiparticle effective mass. At a quantum critical point (QCP) this dependence generates kinks (crossover points from fast to slow growth) in thermodynamic characteristics (like specific heat, magnetization etc) at some temperatures when a strongly correlated electron system transits from the magnetic field induced Landau Fermi liquid (LFL) regime to the non-Fermi liquid (NFL) one taking place at rising temperatures. We show that the abov…

Quantum phase transitionPhysicsMagnetoresistanceCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)General Physics and AstronomyFOS: Physical sciences01 natural sciences010305 fluids & plasmasMagnetizationCondensed Matter - Strongly Correlated ElectronsEffective mass (solid-state physics)Quantum critical point0103 physical sciencesQuasiparticleStrongly correlated materialCondensed Matter::Strongly Correlated Electrons010306 general physicsScaling
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Quantum simulation of the cooperative Jahn-Teller transition in 1D Ion crystals

2012

The Jahn-Teller effect explains distortions and nondegenerate energy levels in molecular and solid-state physics via a coupling of effective spins to collective bosons. Here we propose and theoretically analyze the quantum simulation of a many-body Jahn-Teller model with linear ion crystals subjected to magnetic field gradients. We show that the system undergoes a quantum magnetic structural phase transition which leads to a reordering of particle positions and the formation of a spin-phonon quasicondensate in mesoscopic ion chains.

Quantum phase transitionPhysicsMesoscopic physicsSpinsCondensed matter physicsJahn–Teller effectGeneral Physics and AstronomyQuantum simulatorFísica01 natural sciences010305 fluids & plasmasIon0103 physical sciencesCondensed Matter::Strongly Correlated Electrons010306 general physicsQuantumBoson
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Geometric-phase backaction in a mesoscopic qubit-oscillator system

2012

We illustrate a reverse Von Neumann measurement scheme in which a geometric phase induced on a quantum harmonic oscillator is measured using a microscopic qubit as a probe. We show how such a phase, generated by a cyclic evolution in the phase space of the harmonic oscillator, can be kicked back on the qubit, which plays the role of a quantum interferometer. We also extend our study to finite-temperature dissipative Markovian dynamics and discuss potential implementations in micro- and nanomechanical devices coupled to an effective two-level system. © 2012 American Physical Society.

Quantum phase transitionPhysicsNANOMECHANICAL RESONATOR; BACK-ACTION; QUANTUM; OPTOMECHANICS; MECHANICS; EVOLUTION; MODEAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaPhase qubitOptical phase spaceClassical mechanicsGeometric phaseQuantum harmonic oscillatorPhase spaceQubitQuantum mechanicsGeometric phases atomic physics quantum interferometryHarmonic oscillator
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The quantum trajectory approach to geometric phase for open systems

2005

The quantum jump method for the calculation of geometric phase is reviewed. This is an operational method to associate a geometric phase to the evolution of a quantum system subjected to decoherence in an open system. The method is general and can be applied to many different physical systems, within the Markovian approximation. As examples, two main source of decoherence are considered: dephasing and spontaneous decay. It is shown that the geometric phase is to very large extent insensitive to the former, i.e. it is independent of the number of jumps determined by the dephasing operator.

Quantum phase transitionPhysicsNuclear and High Energy PhysicsQuantum decoherenceDecoherence-free subspacesDephasingquantum computationGeometric phaseGeneral Physics and AstronomyAstronomy and AstrophysicsOpen quantum systemClassical mechanicsQuantum error correctionQuantum processQuantum dissipationdecoherence
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