4,425 research outputs found

    The 2D/3D dynamics of wall-bounded low-Rm magnetohydrodynamic (MHD) turbulence

    No full text
    With this experimental study, we give evidence that the dynamics of low-Rm MHD turbulence depends on the diffusion length l_z, which corresponds to the distance over which the Lorentz force is able to diffuse momentum before it is balanced by inertia

    On the structure and classification of Bernstein algebras

    No full text
    We prove that any Bernstein algebra (A,ω)(A, \omega) is isomorphic to a semidirect product V(,Ω)kV \ltimes_{(\cdot, \, \Omega)} \, k associated to a commutative algebra (V,)(V, \cdot) such that (x2)2=0(x^2)^2 = 0, for all xAx\in A and an idempotent endomorphism Ω=Ω2Endk(V)\Omega = \Omega^2 \in {\rm End}_k (V) of VV satisfying two compatibility conditions. The set of types of (1+I)(1 + |I|)-dimensional Bernstein algebras is parametrized by an explicitely constructed (using linear algebra tools) classified object. The automorphisms group of any Bernstein algebra is described as a subgroup of the canonical semidirect product of groups (V,+)GLk(V)(V, +) \ltimes {\rm GL}_k (V).Comment: The final version will appear in Journal of Algebra and its Application

    Approximation properties for modified (p,q)(p,q)-Bernstein-Durrmeyer operators

    No full text
    summary:We introduce modified (p,q)(p,q)-Bernstein-Durrmeyer operators. We discuss approximation properties for these operators based on Korovkin type approximation theorem and compute the order of convergence using usual modulus of continuity. We also study the local approximation property of the sequence of positive linear operators Dn,p,q{D}_{n,p,q}^{\ast } and compute the rate of convergence for the function ff belonging to the class LipM(γ){\rm Lip}_{M}(\gamma )

    Spectroscopie photoassociative des états moléculaires à longue distance de 87^{87}Rb. Analyse Lu-Fano et amélioration de la formule de Le Roy-Bernstein

    No full text
    Nous avons étudié la photoassociation de 87^{87}Rb sous la limite 5S1/2+5P1/2_{1/2}+5{\rm P}_{1/2} (D1_{1}), par spectroscopie de pertes d'atomes froids. Les spectres montrent les progressions vibrationnelles des trois séries d'états moléculaires attractifs 0g0_{\rm g}^{-}, 0u+0_{\rm u}^{+} et 1g1_{\rm g} convergents vers la limite 5S1/2+5P1/25{\rm S}_{1/2}+5{\rm P}_{1/2}. L'analyse de nos données utilise l'approche de Lu-Fano associé au modèle de LeRoy-Bernstein. Pour la série 0g0_{\rm g}^{-}, cette approche met en évidence un écart au modèle. Une amélioration de la formule de LeRoy-Bernstein permet de rendre compte des mesures expérimentales. Pour la série 0u+(P1/2)0_{\rm u}^{+}({\rm P}_{1/2}) avec la même méthode, on montre le couplage avec la série 0u+(P3/2)0_{\rm u}^{+}({\rm P}_{3/2})

    An estimate for F-jumping numbers via the roots of the Bernstein-Sato polynomial

    No full text
    Given a smooth complex algebraic variety XX and a nonzero regular function ff on XX, we give an effective estimate for the difference between the jumping numbers of ff and the FF-jumping numbers of a reduction fpf_p of ff to characteristic p0p\gg 0, in terms of the roots of the Bernstein-Sato polynomial bfb_f of ff. As an application, we show that if bfb_f has no roots of the form lct(f)n-{\rm lct}(f)-n, with nn a positive integer, then the FF-pure threshold of fpf_p is equal to the log canonical threshold of ff for p0p\gg 0 with (p1)lct(f)Z(p-1){\rm lct}(f)\in {\mathbf Z}.Comment: 10 pages; v.2: using a bound for the roots of the Bernstein-Sato polynomial, we deduce a uniform estimate only involving the dimension of the ambient variety and explain how this extends to possibly non-principal ideals. V.3: revised version, to appear in Proceedings of the AM

    Brian\c{c}on-Skoda exponents and the maximal root of reduced Bernstein-Sato polynomials

    No full text
    For a holomorphic function ff on a complex manifold XX, the Brian\c{c}on-Skoda exponent eBS(f)e^{\rm BS}(f) is the smallest integer kk with fk(f)f^k\in(\partial f) (replacing XX with a neighborhood of f1(0)f^{-1}(0)), where (f)(\partial f) denotes the Jacobian ideal of ff. It is shown that eBS(f)dXe^{\rm BS}(f)\le d_X (:=dimX)(:=\dim X) by Brian\c con-Skoda. We prove that eBS(f)[dX2α~f]+1e^{\rm BS}(f)\le[d_X-2\widetilde{\alpha}_f]+1 with α~f-\widetilde{\alpha}_f the maximal root of the reduced Bernstein-Sato polynomial bf(s)/(s+1)b_f(s)/(s+1), assuming the latter exists (shrinking XX if necessary). This implies for instance that eBS(f)dX2e^{\rm BS}(f)\le d_X-2 in the case f1(0)f^{-1}(0) has only rational singularities, that is, if α~f>1\widetilde{\alpha}_f>1.Comment: 10 page

    Triangular Constellations in Flows

    No full text
    Particles advected on the surface of a fluid can exhibit fractal clustering. The local structure of a fractal set is described by its dimension DD, which is the exponent of a power-law relating the mass N{\cal N} in a ball to its radius ε\varepsilon: NεD{\cal N}\sim \varepsilon^D. It is desirable to characterise the {\em shapes} of constellations of points sampling a fractal measure, as well as their masses. The simplest example is the distribution of shapes of triangles formed by triplets of points, which we investigate for fractals generated by chaotic dynamical systems. The most significant parameter describing the triangle shape is the ratio zz of its area to the radius of gyration squared. We show that the probability density of zz has a phase transition: P(z)P(z) is independent of ε\varepsilon and approximately uniform below a critical flow compressibility βc\beta_{\rm c}, which we estimate. For β>βc\beta>\beta_{\rm c} the distribution appears to be described by two power laws: P(z)zα1P(z)\sim z^{\alpha_1} when 1zzc(ε)1\gg z\gg z_{\rm c}(\varepsilon), and P(z)zα2P(z)\sim z^{\alpha_2} when zzc(ε)z\ll z_{\rm c}(\varepsilon)

    Exact two-dimensionalization of low-magnetic-Reynolds-number flows subject to a strong magnetic field

    No full text
    We investigate the behavior of flows, including turbulent flows, driven by a horizontal body-force and subject to a vertical magnetic field, with the following question in mind: for very strong applied magnetic field, is the flow mostly two-dimensional, with remaining weak three-dimensional fluctuations, or does it become exactly 2D, with no dependence along the vertical? We restrict attention to low-magnetic-Reynolds number (Rm) flow. Because liquid metals have low magnetic Prandtl number, such low-RmRm flows can have a kinetic Reynolds number as large as one million and therefore be strongly turbulent. We first focus on the quasi-static approximation, i.e. the asymptotic limit of vanishing magnetic Reynolds number Rm << 1: we prove that the flow becomes exactly 2D asymptotically in time, regardless of the initial condition and provided the interaction parameter N is larger than a threshold value. We call this property absolute two-dimensionalization: the attractor of the system is necessarily a (possibly turbulent) 2D flow. We then consider the full-magnetohydrodynamic equations and we prove that, for low enough Rm and large enough N, the flow becomes exactly two-dimensional in the long-time limit provided the initial vertically-dependent perturbations are infinitesimal. We call this phenomenon linear two-dimensionalization: the (possibly turbulent) 2D flow is an attractor of the dynamics, but it is not necessarily the only attractor of the system. Some 3D attractors may also exist and be attained for strong enough initial 3D perturbations. These results shed some light on the existence of a dissipative anomaly for magnetohydrodynamic flows subject to a strong external magnetic field

    The Decay of Wall Bounded MHD Turbulence at Low RM

    No full text
    We have developed a new spectral method to simulate flows with very fine boundary layers present. We apply it to calculate the evolution of freely decaying MHD turbulence between isolating walls. By comparison them with results obtained in fully periodic domain we quantify the influence of the channel walls on the character of freely decaying MHD turbulence

    Bernstein-Sato polynomials for projective hypersurfaces with weighted homogeneous isolated singularities

    No full text
    We present an efficient method to calculate the roots of the Bernstein-Sato polynomial bf(s)b_f(s) for a defining polynomial ff of a projective hypersurface ZPn1Z\subset{\bf P}^{n-1} of degree dd having only weighted homogeneous isolated singularities. The computation of roots can be reduced to that of the Hilbert series of the Jacobian ring of ff except some special case. For this we prove the E2E_2-degeneration of the pole order spectral sequence. Combined with the self-duality of the Koszul complex and also a theorem of Dimca and Popescu on the weak Lefschetz property of the "torsion part" of the Jacobian ring (with respect to a general linear function), it implies in the case n=3n=3 the discrete connectivity of the absolute values of the roots of bf(s)b_f(s) supported at 0 modulo the roots coming from the singularities of ZZ, except some special case which does not contain any essential indecomposable central hyperplane arrangements in C3{\bf C}^3; more precisely, we have Rf=1d(Z[3,k])RZR_f=\tfrac{1}{d}({\bf Z}\cap[3,k'])\cup R_Z, where Rf,RZR_f,R_Z are the roots of Bernstein-Sato polynomials of f,Zf,Z up to sign, and k=max(2d3,kmax+3)k'=\max(2d-3,k_{\rm max}+3) with kmaxk_{\rm max} the maximal degree of the "torsion part" of the Jacobian ring
    corecore