13,294 research outputs found

    Charge and Statistics of Quantum Hall Quasi-Particles. A numerical study of mean values and fluctuations

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    We present Monte Carlo studies of charge expectation values and charge fluctuations for quasi-particles in the quantum Hall system. We have studied the Laughlin wave functions for quasi-hole and quasi-electron, and also Jain's definition of the quasi-electron wave function. The considered systems consist of from 50 to 200 electrons, and the filling fraction is 1/3. For all quasi-particles our calculations reproduce well the expected values of charge; -1/3 times the electron charge for the quasi-hole, and 1/3 for the quasi-electron. Regarding fluctuations in the charge, our results for the quasi-hole and Jain quasi-electron are consistent with the expected value zero in the bulk of the system, but for the Laughlin quasi-electron we find small, but significant, deviations from zero throughout the whole electron droplet. We also present Berry phase calculations of charge and statistics parameter for the Jain quasi-electron, calculations which supplement earlier studies for the Laughlin quasi-particles. We find that the statistics parameter is more well behaved for the Jain quasi-electron than it is for the Laughlin quasi-electron.Comment: 39 pages, 27 figure

    Hyperbolic Unfoldings of Minimal Hypersurfaces

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    We study the intrinsic geometry of area minimizing (and also of almost minimizing) hypersurfaces from a new point of view by relating this subject to quasiconformal geometry. For any such hypersurface we define and construct a so-called S-structure which reveals some unexpected geometric and analytic properties of the hypersurface and its singularity set. In this paper, this is used to prove the existence of hyperbolic unfoldings: canonical conformal deformations of the regular part of these hypersurfaces into complete Gromov hyperbolic spaces of bounded geometry with Gromov boundary homeomorphic to the singular set

    Universal microstructure and mechanical stability of jammed packings

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    Jammed packings' mechanical properties depend sensitively on their detailed local structure. Here we provide a complete characterization of the pair correlation close to contact and of the force distribution of jammed frictionless spheres. In particular we discover a set of new scaling relations that connect the behavior of particles bearing small forces and those bearing no force but that are almost in contact. By performing systematic investigations for spatial dimensions d=3-10, in a wide density range and using different preparation protocols, we show that these scalings are indeed universal. We therefore establish clear milestones for the emergence of a complete microscopic theory of jamming. This description is also crucial for high-precision force experiments in granular systems.Comment: 11 pages, 7 figure

    Bifurcation sets arising from non-integer base expansions

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    Given a positive integer MM and q(1,M+1]q\in(1,M+1], let Uq\mathcal U_q be the set of x[0,M/(q1)]x\in[0, M/(q-1)] having a unique qq-expansion: there exists a unique sequence (xi)=x1x2(x_i)=x_1x_2\ldots with each xi{0,1,,M}x_i\in\{0,1,\ldots, M\} such that x=x1q+x2q2+x3q3+. x=\frac{x_1}{q}+\frac{x_2}{q^2}+\frac{x_3}{q^3}+\cdots. Denote by Uq\mathbf U_q the set of corresponding sequences of all points in Uq\mathcal U_q. It is well-known that the function H:qh(Uq)H: q\mapsto h(\mathbf U_q) is a Devil's staircase, where h(Uq)h(\mathbf U_q) denotes the topological entropy of Uq\mathbf U_q. In this paper we {give several characterizations of} the bifurcation set B:={q(1,M+1]:H(p)H(q) for any pq}. \mathcal B:=\{q\in(1,M+1]: H(p)\ne H(q)\textrm{ for any }p\ne q\}. Note that B\mathcal B is contained in the set UR\mathcal{U}^R of bases q(1,M+1]q\in(1,M+1] such that 1Uq1\in\mathcal U_q. By using a transversality technique we also calculate the Hausdorff dimension of the difference B\UR\mathcal B\backslash\mathcal{U}^R. Interestingly this quantity is always strictly between 00 and 11. When M=1M=1 the Hausdorff dimension of B\UR\mathcal B\backslash\mathcal{U}^R is log23logλ0.368699\frac{\log 2}{3\log \lambda^*}\approx 0.368699, where λ\lambda^* is the unique root in (1,2)(1, 2) of the equation x5x4x32x2+x+1=0x^5-x^4-x^3-2x^2+x+1=0.Comment: 28 pages, 1 figures and 1 table. To appear in J. Fractal Geometr
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