31,995 research outputs found

    Spin Wave Theory of Spin 1/2 XY Model with Ring Exchange on a Triangular Lattice

    Full text link
    We present the linear spin wave theory calculation of the superfluid phase of a hard-core boson JJ-KK model with nearest neighbour exchange JJ and four-particle ring-exchange KK at half filling on the triangular lattice, as well as the phase diagrams of the system at zero and finite temperatures. We find that the pure JJ model (XY model) which has a well known uniform superfluid phase with an ordered parameter Mx=0M_x=\neq 0 at zero temperature is quickly destroyed by the inclusion of a negative-KK ring-exchange interactions, favouring a state with a (4π3,0)(\frac{4\pi}{3}, 0) ordering wavevector. We further study the behaviour of the finite-temperature Kosterlitz-Thouless phase transition (TKTT_{KT}) in the uniform superfluid phase, by forcing the universal quantum jump condition on the finite-temperature spin wave superfluid density. We find that for K \textless 0, the phase boundary monotonically decreases to T=0 at K/J=4/3K/J = -4/3, where a phase transition is expected and TKTT_{KT} decreases rapidly while for positive KK, TKTT_{KT} reaches a maximum at some K0K\neq 0. It has been shown on a square lattice using quantum Monte Carlo(QMC) simulations that for small K\textgreater 0 away from the XY point, the zero-temperature spin stiffness value of the XY model is decreased\cite{F}. Our result seems to agree with this trend found in QMC simulations

    Coherent pairing states for the Hubbard model

    Full text link
    We consider the Hubbard model and its extensions on bipartite lattices. We define a dynamical group based on the η\eta-pairing operators introduced by C.N.Yang, and define coherent pairing states, which are combinations of eigenfunctions of η\eta-operators. These states permit exact calculations of numerous physical properties of the system, including energy, various fluctuations and correlation functions, including pairing ODLRO to all orders. This approach is complementary to BCS, in that these are superconducting coherent states associated with the exact model, although they are not eigenstates of the Hamiltonian.Comment: 5 pages, RevTe

    Coherent States from Combinatorial Sequences

    Get PDF
    We construct coherent states using sequences of combinatorial numbers such as various binomial and trinomial numbers, and Bell and Catalan numbers. We show that these states satisfy the condition of the resolution of unity in a natural way. In each case the positive weight functions are given as solutions of associated Stieltjes or Hausdorff moment problems, where the moments are the combinatorial numbers.Comment: 4 pages, Latex; Conference 'Quantum Theory and Symmetries 2', Krakow, Poland, July 200

    Ultrastructural alteration of mouse lung by prolonged exposure to mixtures of helium and oxygen

    Get PDF
    Observed changes consist mainly of blebbing of capillary endothelium and alveolar epithelium, which is quite possibly indicative of cellular edema; also, there can be observed highly-convoluted basement membrane, alveolar debris, and increased numbers of platelets

    Condition for tripartite entanglement

    Get PDF
    We propose a scheme for classifying the entanglement of a tripartite pure qubit state. This classification scheme consists of an ordered list of seven elements. These elements are the Cayley hyper-determinant, and its six associated 2×22 \times 2 subdeterminants. In particular we show that this classification provides a necessary and sufficient condition for separability.Comment: 8 pages, to appear in the Proceedings of "Quantum Theory and Symmetries 7", Prague, Aug 7-13, 201

    Transform fault earthquakes in the North Atlantic: Source mechanisms and depth of faulting

    Get PDF
    The centroid depths and source mechanisms of 12 large earthquakes on transform faults of the northern Mid-Atlantic Ridge were determined from an inversion of long-period body waveforms. The earthquakes occurred on the Gibbs, Oceanographer, Hayes, Kane, 15 deg 20 min, and Vema transforms. The depth extent of faulting during each earthquake was estimated from the centroid depth and the fault width. The source mechanisms for all events in this study display the strike slip motion expected for transform fault earthquakes; slip vector azimuths agree to 2 to 3 deg of the local strike of the zone of active faulting. The only anomalies in mechanism were for two earthquakes near the western end of the Vema transform which occurred on significantly nonvertical fault planes. Secondary faulting, occurring either precursory to or near the end of the main episode of strike-slip rupture, was observed for 5 of the 12 earthquakes. For three events the secondary faulting was characterized by reverse motion on fault planes striking oblique to the trend of the transform. In all three cases, the site of secondary reverse faulting is near a compression jog in the current trace of the active transform fault zone. No evidence was found to support the conclusions of Engeln, Wiens, and Stein that oceanic transform faults in general are either hotter than expected from current thermal models or weaker than normal oceanic lithosphere
    corecore