525 research outputs found

    On the Equivalence Between Type I Liouville Dynamical Systems in the Plane and the Sphere

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    ProducciĂłn CientĂ­ficaSeparable Hamiltonian systems either in sphero-conical coordinates on an S2 sphere or in elliptic coordinates on a R2 plane are described in a unified way. A back and forth route connecting these Liouville Type I separable systems is unveiled. It is shown how the gnomonic projection and its inverse map allow us to pass from a Liouville Type I separable system with a spherical configuration space to its Liouville Type I partners where the configuration space is a plane and back. Several selected spherical separable systems and their planar cousins are discussed in a classical context

    Projective dynamics and classical gravitation

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    Given a real vector space V of finite dimension, together with a particular homogeneous field of bivectors that we call a "field of projective forces", we define a law of dynamics such that the position of the particle is a "ray" i.e. a half-line drawn from the origin of V. The impulsion is a bivector whose support is a 2-plane containing the ray. Throwing the particle with a given initial impulsion defines a projective trajectory. It is a curve in the space of rays S(V), together with an impulsion attached to each ray. In the simplest example where the force is identically zero, the curve is a straight line and the impulsion a constant bivector. A striking feature of projective dynamics appears: the trajectories are not parameterized. Among the projective force fields corresponding to a central force, the one defining the Kepler problem is simpler than those corresponding to other homogeneities. Here the thrown ray describes a quadratic cone whose section by a hyperplane corresponds to a Keplerian conic. An original point of view on the hidden symmetries of the Kepler problem emerges, and clarifies some remarks due to Halphen and Appell. We also get the unexpected conclusion that there exists a notion of divergence-free field of projective forces if and only if dim V=4. No metric is involved in the axioms of projective dynamics.Comment: 20 pages, 4 figure

    Projective dynamics and first integrals

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    We present the theory of tensors with Young tableau symmetry as an efficient computational tool in dealing with the polynomial first integrals of a natural system in classical mechanics. We relate a special kind of such first integrals, already studied by Lundmark, to Beltrami's theorem about projectively flat Riemannian manifolds. We set the ground for a new and simple theory of the integrable systems having only quadratic first integrals. This theory begins with two centered quadrics related by central projection, each quadric being a model of a space of constant curvature. Finally, we present an extension of these models to the case of degenerate quadratic forms.Comment: 39 pages, 2 figure

    Kustaanheimo-Stiefel Regularization and the Quadrupolar Conjugacy

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    In this note, we present the Kustaanheimo-Stiefel regularization in a symplectic and quaternionic fashion. The bilinear relation is associated with the moment map of the S1S^{1}- action of the Kustaanheimo-Stiefel transformation, which yields a concise proof of the symplecticity of the Kustaanheimo-Stiefel transformation symplectically reduced by this circle action. The relation between the Kustaanheimo-Stiefel regularization and the Levi-Civita regularization is established via the investigation of the Levi-Civita planes. A set of Darboux coordinates (which we call Chenciner-F\'ejoz coordinates) is generalized from the planar case to the spatial case. Finally, we obtain a conjugacy relation between the integrable approximating dynamics of the lunar spatial three-body problem and its regularized counterpart, similar to the conjugacy relation between the extended averaged system and the averaged regularized system in the planar case.Comment: 19 pages, corrected versio

    Pauli graphs, Riemann hypothesis, Goldbach pairs

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    Let consider the Pauli group Pq=\mathcal{P}_q= with unitary quantum generators XX (shift) and ZZ (clock) acting on the vectors of the qq-dimensional Hilbert space via X∣s>=∣s+1>X|s> =|s+1> and Z∣s>=ωs∣s>Z|s> =\omega^s |s>, with ω=exp⁥(2iπ/q)\omega=\exp(2i\pi/q). It has been found that the number of maximal mutually commuting sets within Pq\mathcal{P}_q is controlled by the Dedekind psi function ψ(q)=q∏p∣q(1+1p)\psi(q)=q \prod_{p|q}(1+\frac{1}{p}) (with pp a prime) \cite{Planat2011} and that there exists a specific inequality ψ(q)q>eÎłlog⁥log⁥q\frac{\psi (q)}{q}>e^{\gamma}\log \log q, involving the Euler constant ÎłâˆŒ0.577\gamma \sim 0.577, that is only satisfied at specific low dimensions q∈A={2,3,4,5,6,8,10,12,18,30}q \in \mathcal {A}=\{2,3,4,5,6,8,10,12,18,30\}. The set A\mathcal{A} is closely related to the set AâˆȘ{1,24}\mathcal{A} \cup \{1,24\} of integers that are totally Goldbach, i.e. that consist of all primes p2p2) is equivalent to Riemann hypothesis. Introducing the Hardy-Littlewood function R(q)=2C2∏p∣np−1p−2R(q)=2 C_2 \prod_{p|n}\frac{p-1}{p-2} (with C2∌0.660C_2 \sim 0.660 the twin prime constant), that is used for estimating the number g(q)∌R(q)qln⁥2qg(q) \sim R(q) \frac{q}{\ln^2 q} of Goldbach pairs, one shows that the new inequality R(Nr)log⁥log⁥NrâȘ†eÎł\frac{R(N_r)}{\log \log N_r} \gtrapprox e^{\gamma} is also equivalent to Riemann hypothesis. In this paper, these number theoretical properties are discusssed in the context of the qudit commutation structure.Comment: 11 page

    Qudits of composite dimension, mutually unbiased bases and projective ring geometry

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    The d2d^2 Pauli operators attached to a composite qudit in dimension dd may be mapped to the vectors of the symplectic module Zd2\mathcal{Z}_d^{2} (Zd\mathcal{Z}_d the modular ring). As a result, perpendicular vectors correspond to commuting operators, a free cyclic submodule to a maximal commuting set, and disjoint such sets to mutually unbiased bases. For dimensions d=6, 10, 15, 12d=6,~10,~15,~12, and 18, the fine structure and the incidence between maximal commuting sets is found to reproduce the projective line over the rings Z6\mathcal{Z}_{6}, Z10\mathcal{Z}_{10}, Z15\mathcal{Z}_{15}, Z6×F4\mathcal{Z}_6 \times \mathbf{F}_4 and Z6×Z3\mathcal{Z}_6 \times \mathcal{Z}_3, respectively.Comment: 10 pages (Fast Track communication). Journal of Physics A Mathematical and Theoretical (2008) accepte

    Carbon Nanotubes Synthesized in Channels of Alpo4-5 Single Crystals : First X-Ray Scattering Investigations

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    Following the synthesis of aligned single-wall carbon nanotubes in the channels of AlPO4-5 zeolite single crystals, we present the first X-ray diffraction and diffuse scattering results. They can be analysed in terms of a partial filling of the zeolite channels by nanotubes with diameter around 4A. The possible selection of only one type of nanotube during the synthesis, due to the constraints imposed by the zeolite host, is discussed.Comment: to appear in Solid State Com
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