9,946 research outputs found

    Husimi function and phase-space analysis of bilayer quantum Hall systems at ν=2/λ\nu=2/\lambda

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    We propose localization measures in phase space of the ground state of bilayer quantum Hall (BLQH) systems at fractional filling factors ν=2/λ\nu=2/\lambda, to characterize the three quantum phases (shortly denoted by spin, canted and ppin) for arbitrary U(4)U(4)-isospin λ\lambda. We use a coherent state (Bargmann) representation of quantum states, as holomorphic functions in the 8-dimensional Grassmannian phase-space G24=U(4)/[U(2)×U(2)]\mathbb{G}^4_{2}=U(4)/[U(2)\times U(2)] (a higher-dimensional generalization of the Haldane's 2-dimensional sphere S2=U(2)/[U(1)×U(1)]\mathbb{S}^2=U(2)/[U(1)\times U(1)]). We quantify the localization (inverse volume) of the ground state wave function in phase-space throughout the phase diagram (i.e., as a function of Zeeman, tunneling, layer distance, etc, control parameters) with the Husimi function second moment, a kind of inverse participation ratio that behaves as an order parameter. Then we visualize the different ground state structure in phase space of the three quantum phases, the canted phase displaying a much higher delocalization (a Schr\"odinger cat structure) than the spin and ppin phases, where the ground state is highly coherent. We find a good agreement between analytic (variational) and numeric diagonalization results.Comment: 13 pages, 6 figures. New section added. Novel results and insights further highlighte

    Complexified sigma model and duality

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    We show that the equations of motion associated with a complexified sigma-model action do not admit manifest dual SO(n,n) symmetry. In the process we discover new type of numbers which we called `complexoids' in order to emphasize their close relation with both complex numbers and matroids. It turns out that the complexoids allow to consider the analogue of the complexified sigma-model action but with (1+1)-worldsheet metric, instead of Euclidean-worldsheet metric. Our observations can be useful for further developments of complexified quantum mechanics.Comment: 15 pages, Latex, improved versio

    Canonical gravity in two time and two space dimensions

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    We describe a program for developing a canonical gravity in 2+2 dimensions (two time and two space dimensions). Our procedure is similar to the usual canonical gravity but with two times rather than just one time. Our work may be of particular interest as an alternative approach to loop quantum gravity in 2+2 dimensions.Comment: 13 pages, Latex, improved versio

    Scalable Bayesian nonparametric measures for exploring pairwise dependence via Dirichlet Process Mixtures

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    In this article we propose novel Bayesian nonparametric methods using Dirichlet Process Mixture (DPM) models for detecting pairwise dependence between random variables while accounting for uncertainty in the form of the underlying distributions. A key criteria is that the procedures should scale to large data sets. In this regard we find that the formal calculation of the Bayes factor for a dependent-vs.-independent DPM joint probability measure is not feasible computationally. To address this we present Bayesian diagnostic measures for characterising evidence against a "null model" of pairwise independence. In simulation studies, as well as for a real data analysis, we show that our approach provides a useful tool for the exploratory nonparametric Bayesian analysis of large multivariate data sets

    General Approach to Functional Forms for the Exponential Quadratic Operators in Coordinate-Momentum Space

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    In a recent paper [Nieto M M 1996 Quantum and Semiclassical Optics, 8 1061; quant-ph/9605032], the one dimensional squeezed and harmonic oscillator time-displacement operators were reordered in coordinate-momentum space. In this paper, we give a general approach for reordering multi-dimensional exponential quadratic operator(EQO) in coordinate-momentum space. An explicit computational formula is provided and applied to the single mode and double-mode EQO through the squeezed operator and the time displacement operator of the harmonic oscillator.Comment: To appear in J. Phys. A: Mathematics and Genera
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