15,218 research outputs found

    Scattering Theory for Quantum Hall Anyons in a Saddle Point Potential

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    We study the theory of scattering of two anyons in the presence of a quadratic saddle-point potential and a perpendicular magnetic field. The scattering problem decouples in the centre-of-mass and the relative coordinates. The scattering theory for the relative coordinate encodes the effects of anyon statistics in the two-particle scattering. This is fully characterized by two energy-dependent scattering phase shifts. We develop a method to solve this scattering problem numerically, using a generalized lowest Landau level approximation.Comment: 5 pages. Published version, with clarified presentatio

    Gaussian systems for quantum enhanced multiple phase estimation

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    For a fixed average energy, the simultaneous estimation of multiple phases can provide a better total precision than estimating them individually. We show this for a multimode interferometer with a phase in each mode, using Gaussian inputs and passive elements, by calculating the covariance matrix. The quantum Cram\'{e}r-Rao bound provides a lower bound to the covariance matrix via the quantum Fisher information matrix, whose elements we derive to be the covariances of the photon numbers across the modes. We prove that this bound can be saturated. In spite of the Gaussian nature of the problem, the calculation of non-Gaussian integrals is required, which we accomplish analytically. We find our simultaneous strategy to yield no more than a factor-of-2 improvement in total precision, possibly because of a fundamental performance limitation of Gaussian states. Our work shows that no modal entanglement is necessary for simultaneous quantum-enhanced estimation of multiple phases

    Spectroscopic properties of large open quantum-chaotic cavities with and without separated time scales

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    The spectroscopic properties of an open large Bunimovich cavity are studied numerically in the framework of the effective Hamiltonian formalism. The cavity is opened by attaching leads to it in four different ways. In some cases, short-lived and long-lived resonance states coexist. The short-lived states cause traveling waves in the transmission while the long-lived ones generate superposed fluctuations. The traveling waves oscillate as a function of energy. They are not localized in the interior of the large chaotic cavity. In other cases, the transmission takes place via standing waves with an intensity that closely follows the profile of the resonances. In all considered cases, the phase rigidity fluctuates with energy. It is mostly near to its maximum value and agrees well with the theoretical value for the two-channel case. As shown in the foregoing paper \cite{1}, all cases are described well by the Poisson kernel when the calculation is restricted to an energy region in which the average SS matrix is (nearly) constant.Comment: 13 pages, 4 figure

    Space Complexity of Perfect Matching in Bounded Genus Bipartite Graphs

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    We investigate the space complexity of certain perfect matching problems over bipartite graphs embedded on surfaces of constant genus (orientable or non-orientable). We show that the problems of deciding whether such graphs have (1) a perfect matching or not and (2) a unique perfect matching or not, are in the logspace complexity class \SPL. Since \SPL\ is contained in the logspace counting classes \oplus\L (in fact in \modk\ for all k≄2k\geq 2), \CeqL, and \PL, our upper bound places the above-mentioned matching problems in these counting classes as well. We also show that the search version, computing a perfect matching, for this class of graphs is in \FL^{\SPL}. Our results extend the same upper bounds for these problems over bipartite planar graphs known earlier. As our main technical result, we design a logspace computable and polynomially bounded weight function which isolates a minimum weight perfect matching in bipartite graphs embedded on surfaces of constant genus. We use results from algebraic topology for proving the correctness of the weight function.Comment: 23 pages, 13 figure

    Correlated behavior of conductance and phase rigidity in the transition from the weak-coupling to the strong-coupling regime

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    We study the transmission through different small systems as a function of the coupling strength vv to the two attached leads. The leads are identical with only one propagating mode ΟCE\xi^E_C in each of them. Besides the conductance GG, we calculate the phase rigidity ρ\rho of the scattering wave function ΚCE\Psi^E_C in the interior of the system. Most interesting results are obtained in the regime of strongly overlapping resonance states where the crossover from staying to traveling modes takes place. The crossover is characterized by collective effects. Here, the conductance is plateau-like enhanced in some energy regions of finite length while corridors with zero transmission (total reflection) appear in other energy regions. This transmission picture depends only weakly on the spectrum of the closed system. It is caused by the alignment of some resonance states of the system with the propagating modes ΟCE\xi^E_C in the leads. The alignment of resonance states takes place stepwise by resonance trapping, i.e. it is accompanied by the decoupling of other resonance states from the continuum of propagating modes. This process is quantitatively described by the phase rigidity ρ\rho of the scattering wave function. Averaged over energy in the considered energy window, is correlated with 1−1-. In the regime of strong coupling, only two short-lived resonance states survive each aligned with one of the channel wave functions ΟCE\xi^E_C. They may be identified with traveling modes through the system. The remaining M−2M-2 trapped narrow resonance states are well separated from one another.Comment: Resonance trapping mechanism explained in the captions of Figs. 7 to 11. Recent papers added in the list of reference

    Partial Isometries of a Sub-Riemannian Manifold

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    In this paper, we obtain the following generalisation of isometric C1C^1-immersion theorem of Nash and Kuiper. Let MM be a smooth manifold of dimension mm and HH a rank kk subbundle of the tangent bundle TMTM with a Riemannian metric gHg_H. Then the pair (H,gH)(H,g_H) defines a sub-Riemannian structure on MM. We call a C1C^1-map f:(M,H,gH)→(N,h)f:(M,H,g_H)\to (N,h) into a Riemannian manifold (N,h)(N,h) a {\em partial isometry} if the derivative map dfdf restricted to HH is isometric; in other words, f∗h∣H=gHf^*h|_H=g_H. The main result states that if dim⁥N>k\dim N>k then a smooth HH-immersion f0:M→Nf_0:M\to N satisfying f∗h∣H<gHf^*h|_H<g_H can be homotoped to a partial isometry f:(M,gH)→(N,h)f:(M,g_H)\to (N,h) which is C0C^0-close to f0f_0. In particular we prove that every sub-Riemannian manifold (M,H,gH)(M,H,g_H) admits a partial isometry in Rn\R^n provided n≄m+kn\geq m+k.Comment: 13 pages. This is a revised version of an earlier submission (minor revision
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