1,076 research outputs found

    Approximation of some classes of set-valued periodic functions by generalized trigonometric polynomials

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    Generalizations of some known results on the best, best linear and best one-sided approxima- tions by trigonometric polynomials of the classes of 2\pi - periodic functions presented in the form of convolutions to the case of set-valued functions are obtaine

    On interpolation and extremal properties of periodic perfect splines

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    Existing and extremal property of periodic perfect spline, which interpolates given function in the mean were proved.Comment: 5 pages in English and Russia

    Features of the second-order visual filters sensitive to the spatial frequency modulations

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    We investigated selectivity of 2nd order visual filters sensitive to the spatial frequency (SF) modulations to orientation and to SF of modulation. We carried out psychophysical experiment using masking paradigm. It was found that 2nd order filters are selective to SF of modulation (with bandwidth +1.5 octaves), and do not show any selectivity to orientation of modulation. We suppose receptive fields of 2nd order mechanisms have concentric form.Comment: 3 pages, 4 figure

    Optimum Branching Problem Revisited

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    Given a digraph G=(VG,AG)G = (V_G, A_G), a \emph{branching} in GG is a set of arcs BAGB \subseteq A_G such that the underlying undirected graph spanned by BB is acyclic and each node in GG is entered (\emph{covered}) by at most one arc from BB. Tarjan developed efficient algorithms (based on the cycle contraction technique) for the following problem: given a digraph GG with a \emph{weight} function w ⁣:AGRw \colon A_G \to \R, find a branching BB of the minimum weight w(B):=aBw(a)w(B) := \sum_{a \in B} w(a) among all branchings with the maximum ardinality \abs{B}. We generalize this notion as follows: for a digraph GG and a matroid \calM_V on VGV_G, a \emph{matroid branching} in GG w.r.t. \calM_V is a branching in GG such that the covered set of nodes is independent w.r.t. \calM_V. The unweighted (cardinality) problem consists in finding a matroid branching BB with \abs{B} maximum. We show that the general cycle contraction approach is applicable to this problem and leads to an efficient algorithm (provided that an oracle is given for testing independence in the matroids arising as the result of the contraction procedure). In the weighted version we are looking for a matroid branching BB that minimizes w(B)w(B) (for a given weight function w ⁣:AGRw \colon A_G \to \R) among all matroid branchings of the maximum cardinality. We show that if \calM_V is a rainbow matroid (that is, nodes of GG are marked with colors and it is forbidden to cover more than one node of any color), then there exists an O(min(n2,mlogn))O(\min(n^2, m \log n)) method, matching the complexity of Tarjan's algorithm (here n := \abs{V_G}, m := \abs{A_G}).Comment: 12 page

    Determination of Low-Energy Parameters of Neutron--Proton Scattering on the Basis of Modern Experimental Data from Partial-Wave Analyses

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    The triplet and singlet low-energy parameters in the effective-range expansion for neutron--proton scattering are determined by using the latest experimental data on respective phase shifts from the SAID nucleon--nucleon database. The results differ markedly from the analogous parameters obtained on the basis of the phase shifts of the Nijmegen group and contradict the parameter values that are presently used as experimental ones. The values found with the aid of the phase shifts from the SAID nucleon--nucleon database for the total cross section for the scattering of zero-energy neutrons by protons, σ0=20.426\sigma_{0}=20.426 b, and the neutron--proton coherent scattering length, f=3.755f=-3.755 fm, agree perfectly with the experimental cross-section values obtained by Houk, σ0=20.436±0.023\sigma_{0}=20.436\pm 0.023 b, and experimental scattering-length values obtained by Houk and Wilson, f=3.756±0.009f=-3.756\pm 0.009 fm, but they contradict cross-section values of σ0=20.491±0.014\sigma_{0}=20.491\pm 0.014 b according to Dilg and coherent-scattering-length values of f=3.7409±0.0011f=-3.7409\pm 0.0011 fm according to Koester and Nistler.Comment: 17 pages, to be published in Physics of Atomic Nucle

    LL-approximation of BB-splines by trigonometric polynomials

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    This note is a continuation of our papers [1,2], devoted to LL-approximation of characteristic function of (h,h)(-h, h) by trigonometric polynomials. In the paper [1] the sharp values of the best approximation for the special values of hh were found. In [2] we gave the complete solution of the problem for arbitrary values of hh. In general case [2] the situation is more deep and results are not so simple as in [1]. For applications to the problem of optimal constants in the Jackson-type inequalities we need, however, results on LL-approximation of BB-splines and linear combinations of BB-splines. Here we present some simple results about LL-approximation of BB-splines as well as give the the proof of its sharpness for the special values of hh.Comment: 6 page

    Description of the Low-Energy Doublet Neutron-Deuteron Scattering on the Basis of the Triton Bound and Virtual State Parameters

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    Low-energy doublet neutron-deuteron scattering is described on the basis of the triton bound and virtual state parameters - the energies and the nuclear vertex constants of these states. The van Oers-Seagrave formula is derived from the Bargmann representation of the S matrix for a system having two states. The presence of a pole in this formula is shown to be a direct corollary of the existence of a low-energy triton virtual state. Simple explicit expressions for the nd scattering length and for the pole of the function kcotδk\cot \delta are obtained in terms of the triton bound and virtual state parameters. Numerical calculations of the nd low-energy scattering parameters show their high sensitivity to variations in the asymptotic normalization constant of the virtual state Cv2C_{v}^{2}. The Cv2C_{v}^{2} value fitted in our model to the experimental result for the nd scattering length is Cv2=0.0592C_{v}^{2}=0.0592.Comment: 15 pages, 1 figur

    P-matrix Description of Interaction of Two Charged Hadrons And Low-energy Nuclear-Coulomb Scattering Parameters

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    The scattering of two charged strongly interacting particles is described on the basis of the P-matrix approach. In the P matrix, it is proposed to isolate explicitly the background term corresponding to purely Coulomb interaction, whereby it becomes possible to improve convergence of the expansions used and to obtain a correct asymptotic behavior of observables at high energies. The expressions for the purely Coulomb background P matrix, its poles and residues, and purely Coulomb eigenfunctions of the P-matrix approach are obtained. The nuclear-Coulomb low-energy scattering parameters of two charged hadrons are investigated on the basis of this approach combined with the method of isolating the background P matrix. Simple explicit expressions for the nuclear-Coulomb scattering length and effective range in terms of the residual P matrix are derived. These expressions give a general form of the nuclear-Coulomb low-energy scattering parameters for models of finite-range strong interaction. Specific applications of the general expressions derived in this study are exemplified by considering some exactly solvable models of strong interaction containing hard core repulsion, and, for these models, the nuclear-Coulomb low-energy scattering parameters for arbitrary values of the orbital angular momentum are found explicitly. In particular, the nuclear-Coulomb scattering length and effective range are obtained explicitly for the boundary-condition model, the model of a hard-core delta-shell potential, the Margenau model, and the model of hard-core square-well potential.Comment: 23 page

    Free multiflows in bidirected and skew-symmetric graphs

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    A graph (digraph) G=(V,E)G=(V,E) with a set TVT\subseteq V of terminals is called inner Eulerian if each nonterminal node vv has even degree (resp. the numbers of edges entering and leaving vv are equal). Cherkassky and Lov\'asz showed that the maximum number of pairwise edge-disjoint TT-paths in an inner Eulerian graph GG is equal to 12sTλ(s)\frac12\sum_{s\in T} \lambda(s), where λ(s)\lambda(s) is the minimum number of edges whose removal disconnects ss and T{s}T-\{s\}. A similar relation for inner Eulerian digraphs was established by Lomonosov. Considering undirected and directed networks with ``inner Eulerian'' edge capacities, Ibaraki, Karzanov, and Nagamochi showed that the problem of finding a maximum integer multiflow (where partial flows connect arbitrary pairs of distinct terminals) is reduced to O(logT)O(\log T) maximum flow computations and to a number of flow decompositions. In this paper we extend the above max-min relation to inner Eulerian bidirected and skew-symmetric graphs and develop an algorithm of complexity O(VElogTlog(2+V2/E))O(VE\log T\log(2+V^2/E)) for the corresponding capacitated cases. In particular, this improves the known bound for digraphs. Our algorithm uses a fast procedure for decomposing a flow with O(1) sources and sinks in a digraph into the sum of one-source-one-sink flows.Comment: 21 pages, 4 figures Submitted to a special issue of DA

    Study of the Low-Energy Characteristics of Neutron-Neutron Scattering in the Effective-Range Approximation

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    The influence of the mass difference between the charged and neutral pions on the low-energy characteristics of nucleon-nucleon interaction in the 1S0^{1}S_{0} spin-singlet state is studied within the framework of the effective-range approximation. By making use of the experimental singlet neutron-proton scattering parameters and the experimental value of neutron-neutron virtual-state energy, the following values were obtained for the neutron-neutron scattering length and effective range: ann=16.59(117)a_{nn}=-16.59(117)fm, rnn=2.83(11)r_{nn}=2.83(11)fm. The calculated neutron-neutron scattering length anna_{nn} is in good agreement with one of the two well known and differing experimental values of this quantity, and the calculated effective range rnnr_{nn} is also in good agreement with present-day experimental results.Comment: 12 pages, 1 table. Slightly modified version of the article published in Physics of Atomic Nucle
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