Search results for "Phase Transition"

showing 10 items of 1281 documents

Ordering phenomena and phase transitions in the physisorbed quantum systems H2, HD and D2

1991

Abstract Recent experimental results of H2, HD and D2 films physisorbed on graphite are briefly reviewed. In particular, the monolayer phase diagrams, the order-disorder transition of the commensurate (C) phase and the commensurate-incommensurate (C-IC) transition are discussed. It will be shown that the melting transition of the C phase belongs to the three-state Potts universality class, and that the C-IC transition occurs via a series of novel intermediate phase, which could be identified as density-modulated phases characterized by striped and hexagonal patterns of domain walls. Due to this rich variety of phenomena, the hydrogen isotopes can be considered as model systems for two-dimen…

Quantum phase transitionPhase transitionMaterials scienceCondensed matter physicsPhase (matter)Quantum critical pointMonolayerFerroicsQuantum phasesElectrical and Electronic EngineeringCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsPhase diagramPhysica B: Condensed Matter
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Uhlmann curvature in dissipative phase transitions

2018

We study the mean Uhlmann curvature in fermionic systems undergoing a dissipative driven phase transition. We consider a paradigmatic class of lattice fermion systems in non-equilibrium steady-state of an open system with local reservoirs, which are characterised by a Gaussian fermionic steady state. In the thermodynamical limit, in systems with translational invariance we show that a singular behaviour of the Uhlmann curvature represents a sufficient criterion for criticalities, in the sense of diverging correlation length, and it is not otherwise sensitive to the closure of the Liouvillian dissipative gap. In finite size systems, we show that the scaling behaviour of the mean Uhlmann curv…

Quantum phase transitionPhase transitionSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciCritical phenomenaGaussianlcsh:MedicineFOS: Physical sciencesQuantum phase transitionCurvature01 natural sciencesArticle010305 fluids & plasmassymbols.namesake0103 physical sciencesUhlmann curvatureStatistical physics010306 general physicslcsh:ScienceQuantumCondensed Matter - Statistical MechanicsPhysicsQuantum PhysicsMultidisciplinaryStatistical Mechanics (cond-mat.stat-mech)lcsh:RUhlmann geometric phaseFermionDissipative systemsymbolslcsh:QQuantum Physics (quant-ph)
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Violation of the Time-Reversal and Particle-Hole Symmetries in Strongly Correlated Fermi Systems: A Review

2020

In this review, we consider the time reversal T and particle-antiparticle C symmetries that, being most fundamental, can be violated at microscopic level by a weak interaction. The notable example here is from condensed matter, where strongly correlated Fermi systems like heavy-fermion metals and high Tc superconductors exhibit C and T symmetries violation due to so-called non-Fermi liquid (NFL) behavior. In these systems, tunneling differential conductivity (or resistivity) is a very sensitive tool to experimentally test the above symmetry break. When a strongly correlated Fermi system turns out to be near the topological fermion condensation quantum phase transition (FCQPT), it exhibits t…

Quantum phase transitionPhysics and Astronomy (miscellaneous)General Mathematicsmedia_common.quotation_subjectquantum phase transition; fermion condensation; tunneling conductivity; time-reversal symmetryWeak interaction01 natural sciencesAsymmetry010305 fluids & plasmastime-reversal symmetryBaryon asymmetry0103 physical sciencesComputer Science (miscellaneous)quantum phase transition010306 general physicstunneling conductivitymedia_commonPhysicsCondensed matter physicslcsh:MathematicsFermionlcsh:QA1-939Symmetry (physics)T-symmetryChemistry (miscellaneous)Computer Science::Programming LanguagesFermi liquid theoryfermion condensationSymmetry-Basel
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Quantum fluctuations and coherence in high-precision single-electron capture.

2012

The phase of a single quantum state is undefined unless the history of its creation provides a reference point. Thus quantum interference may seem hardly relevant for the design of deterministic single-electron sources which strive to isolate individual charge carriers quickly and completely. We provide a counterexample by analyzing the non-adiabatic separation of a localized quantum state from a Fermi sea due to a closing tunnel barrier. We identify the relevant energy scales and suggest ways to separate the contributions of quantum non-adiabatic excitation and backtunneling to the rare non-capture events. In the optimal regime of balanced decay and non-adiabaticity, our simple electron tr…

Quantum phase transitionPhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsQuantum limitFOS: Physical sciencesGeneral Physics and AstronomyQuantum phasesQuantum imagingQuantum stateQuantum mechanicsQuantum processMesoscale and Nanoscale Physics (cond-mat.mes-hall)Amplitude damping channelQuantum fluctuationPhysical review letters
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Quasi-one-dimensional quantum spin liquid in the $\rm {Cu(C_4H_4N_2)(NO_3)_2}$ insulator

2015

We analyze measurements of the magnetization, differential susceptibility and specific heat of quasi-one dimensional insulator Cu(C$_4$H$_4$N$_2$)(NO$_3$)$_2$ (CuPzN) subjected to magnetic fields. We show that the thermodynamic properties are defined by quantum spin liquid formed with spinons, with the magnetic field tuning the insulator CuPzN towards quantum critical point related to fermion condensation quantum phase transition (FCQPT) at which the spinon effective mass diverges kinematically. We show that the FCQPT concept permits to reveal and explain the scaling behavior of thermodynamic characteristics. For the first time, we construct the schematic $T-H$ (temperature---magnetic field…

Quantum phase transitionPhysicsCondensed Matter::Quantum GasesPhysics and Astronomy (miscellaneous)Condensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciences01 natural sciencesSpinon010305 fluids & plasmasMagnetic fieldCondensed Matter - Strongly Correlated ElectronsMagnetizationEffective mass (solid-state physics)Quantum critical point0103 physical sciencesCondensed Matter::Strongly Correlated ElectronsQuantum spin liquid010306 general physicsPhase diagram
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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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