552 research outputs found

    Structural and optical properties of vacuum-deposited ZnS nanostructures

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    In this paper some structural, substructural and optical proper- ties of zinc sulfide nanostructures obtained by a CSVS method on bulk ZnSe are investigated. Examination of optical and substructural properties was performed by infrared spectro- scopy and X-ray diffraction, respectively. The results of these studies enabled determination of the dependence of the main structural film parameters (texture, lattice parameters, grain and X-ray scattering domain sizes, and microstrain) on the growth conditions. IR-spectral distributions of transmission coefficient T(n) for bilayered ZnS/ZnSe nanostructures are obtained. When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3323

    Observation of inverse diproton photodisintegration at intermediate energies

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    The reaction pp->{pp}_s\gamma, where {pp}_s is a proton pair with an excitation energy E_{pp}<3 MeV, has been observed with the ANKE spectrometer at COSY-Juelich for proton beam energies of T_p=0.353, 0.500, and 0.550 GeV. This is equivalent to photodisintegration of a free 1S_0 diproton for photon energies E\gamma ~ T_p/2. The differential cross sections measured for c.m. angles 0 deg.<\theta_{pp}<20 deg. exhibit a steep increase with angle that is compatible with E1 and E2 multipole contributions. The ratio of the measured cross sections to those of np->d\gamma is on the 10^{-3}-10^{-2} level. The increase of the pp->{pp}_s\gamma cross section with T_p might reflect the influence of the Delta(1232) excitation.Comment: 4 pages + 4 figure

    First measurements of spin correlations in the np -> d pi^0 reaction

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    The transverse spin correlations Axx and Ayy in the np-> d pi^0 reaction have been measured for the first time in quasi-free kinematics at the COSY-ANKE facility using a polarised deuteron beam incident on a polarised hydrogen cell target. The results obtained for neutron energies close to 353 MeV and 600 MeV are in good agreement with the partial wave analysis of data on the isospin-related pp-> d pi^+ reaction, though the present results cover also the small-angle region, which was largely absent from these data

    Resonance-like coherent production of a pion pair in the reaction pdpdππpd \rightarrow pd\pi\pi in the GeV region

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    The reaction p+dp+d+Xp + d \rightarrow p + d + X was studied at 0.8-2.0 GeV proton beam energies with the ANKE magnetic spectrometer at the COSY synchrotron storage ring. The proton-deuteron pairs emerging with high momenta, 0.6-1.8 GeV/cc, were detected at small angles with respect to the proton beam. Distribution over the reaction missing mass MxM_x reveals a local enhancement near the threshold of the pion pair production specific for the so-called ABC effect. The enhancement has a structure of a narrow bump placed above a smooth continuum. The invariant mass of the dππd\pi\pi system in this enhancement region exhibits a resonance-like peak at Mdππ2.36M_{d\pi\pi} \approx 2.36 GeV/c2c^2 with the width Γ0.10\Gamma \approx 0.10 GeV/c2c^2. A possible interpretation of these features is discussed.Comment: 14 pages, 16 figures, submitted to Eur. Phys. J. A. v2: Added references [42,43] in section IV.A. v3: revised version according to referee remarks v4: revised version according to referee remark

    An approximation of matrix exponential by a truncated Laguerre series

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    The Laguerre functions ln,ταl_{n,\tau}^\alpha, n=0,1,n=0,1,\dots, are constructed from generalized Laguerre polynomials. The functions ln,ταl_{n,\tau}^\alpha depend on two parameters: scale τ>0\tau>0 and order of generalization α>1\alpha>-1, and form an orthogonal basis in L2[0,)L_2[0,\infty). Let the spectrum of a square matrix AA lie in the open left half-plane. Then the matrix exponential HA(t)=eAtH_A(t)=e^{At}, t>0t>0, belongs to L2[0,)L_2[0,\infty). Hence the matrix exponential HAH_A can be expanded in a series HA=n=0Sn,τ,α,Aln,ταH_A=\sum_{n=0}^\infty S_{n,\tau,\alpha,A}\,l_{n,\tau}^\alpha. An estimate of the norm HAn=0NSn,τ,α,Aln,ταL2[0,)\Bigl\lVert H_A-\sum_{n=0}^N S_{n,\tau,\alpha,A}\,l_{n,\tau}^\alpha\Bigr\rVert_{L_2[0,\infty)} is proposed. Finding the minimum of this estimate over τ\tau and α\alpha is discussed. Numerical examples show that the optimal α\alpha is often almost 0, which essentially simplifies the problem.Comment: 20 pages, 4 figure

    Measurement of the Spin-Dependence of the pbar-p Interaction at the AD-Ring

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    We propose to use an internal polarized hydrogen storage cell gas target in the AD ring to determine for the first time the two total spin-dependent pbar-p cross sections sigma_1 and sigma_2 at antiproton beam energies in the range from 50 to 450 MeV. The data obtained are of interest by themselves for the general theory of pbar-p interactions since they will provide a first experimental constraint of the spin-spin dependence of the nucleon-antinucleon potential in the energy range of interest. In addition, measurements of the polarization buildup of stored antiprotons are required to define the optimum parameters of a future, dedicated Antiproton Polarizer Ring (APR), intended to feed a double-polarized asymmetric pbar-p collider with polarized antiprotons. Such a machine has recently been proposed by the PAX collaboration for the new Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt, Germany. The availability of an intense stored beam of polarized antiprotons will provide access to a wealth of single- and double-spin observables, thereby opening a new window on QCD spin physics.Comment: 51 pages, 23 figures, proposal submitted to the SPS committee of CER

    Forward K+ production in subthreshold pA collisions at 1.0 GeV

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    K+ meson production in pA (A = C, Cu, Au) collisions has been studied using the ANKE spectrometer at an internal target position of the COSY-Juelich accelerator. The complete momentum spectrum of kaons emitted at forward angles, theta < 12 degrees, has been measured for a beam energy of T(p)=1.0 GeV, far below the free NN threshold of 1.58 GeV. The spectrum does not follow a thermal distribution at low kaon momenta and the larger momenta reflect a high degree of collectivity in the target nucleus.Comment: 4 pages, 3 figure
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