8,425 research outputs found

    Multi-Nucleon Exchange in Quasi-Fission Reactions

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    Nucleon exchange mechanism is investigated in the central collisions of 40{}^{40}Ca + 238{}^{238}U and 48{}^{48}Ca + 238{}^{238}U systems near the quasi-fission regime in the framework of the Stochastic Mean-Field (SMF) approach. Sufficiently below the fusion barrier, di-nuclear structure in the collisions is maintained to a large extend. Consequently, it is possible to describe nucleon exchange as a diffusion process familiar from deep-inelastic collisions. Diffusion coefficients for proton and neutron exchange are determined from the microscopic basis of the SMF approach in the semi-classical framework. Calculations show that after a fast charge equilibration the system drifts toward symmetry over a very long interaction time. Large dispersions of proton and neutron distributions of the produced fragments indicate that diffusion mechanism may help to populate heavy trans-uranium elements near the quasi-fission regime in these collisions

    Nucleon exchange in heavy-ion collisions within stochastic mean-field approach

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    Nucleon exchange mechanism is investigated in deep-inelastic symmetric heavy-ion collisions in the basis of the Stochastic Mean-Field approach. By extending the previous work to off-central collisions, analytical expression is deduced for diffusion coefficient of nucleon exchange mechanism. Numerical calculations are carried out for 40{}^{40}Ca + 40{}^{40}Ca and 90{}^{90}Zr + 90{}^{90}Zr systems and the results are compared with the phenomenological nucleon exchange model. Also, calculations are compared with the available experimental results of deep-inelastic collisions between calcium nuclei.Comment: 8 pages, 7 figure

    Quantal description of nucleon exchange in stochastic mean-field approach

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    Nucleon exchange mechanism is investigated in central collisions of symmetric heavy-ions in the basis of the stochastic mean-field approach. Quantal diffusion coefficients for nucleon exchange are calculated by including non-Markovian effects and shell structure. Variances of fragment mass distributions are calculated in central collisions of 40{}^{40}Ca + 40{}^{40}Ca, 48{}^{48}Ca + 48{}^{48}Ca and 56{}^{56}Ni + 56{}^{56}Ni systems

    Polarization Beam Splitter Based on Self-Collimation of a Hybrid Photonic Crystal

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    A photonic crystal polarization beam splitter based on photonic band gap and self-collimation effects is designed for optical communication wavelengths. The photonic crystal structure consists of a polarization-insensitive self-collimation region and a splitting region. TM- and TE-polarized waves propagate without diffraction in the self-collimation region, whereas they split by 90 degrees in the splitting region. Efficiency of more than 75% for TM- and TE-polarized light is obtained for a polarization beam splitter size of only 17 μm x 17 μm in a wavelength interval of 60 nm including 1.55 μm

    A Search for pair production of the LSP ντ~\tilde{\nu_{\tau}} at the CLIC via RPV Decays

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    In this work we consider pair production of LSP tau-sneutrinos at the Compact Lineer Collider. We assume that tau-sneutrinos decays in to e\textmu pair via RPV interactions. Backgroundless subprocess ee+ν~ν~ˉμ+μ+ee(μμe+e+)e{}^{-}e^{+}\rightarrow\tilde{\nu}\bar{\tilde{\nu}}\rightarrow\mu^{+}\mu^{+}e^{-}e^{-}(\mu^{-}\mu^{-}e^{+}e^{+}) is analyzed in details. Achievable limits on Br(ν~τμe)Br\,(\tilde{\nu}_{\tau}\rightarrow\mu e) at 3σ3\sigma and 5σ5\sigma CL are obtained depending on ντ~\tilde{\nu_{\tau}} mass.Comment: 8 pages, 5 figure

    Quantal Diffusion Description of Multi-Nucleon Transfers in Heavy-Ion Collisions

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    Employing the stochastic mean-field (SMF) approach, we develop a quantal diffusion description of the multi-nucleon transfer in heavy-ion collisions at finite impact parameters. The quantal transport coefficients are determined by the occupied single-particle wave functions of the time-dependent Hartree-Fock equations. As a result, the primary fragment mass and charge distribution functions are determined entirely in terms of the mean-field properties. This powerful description does not involve any adjustable parameter, includes the effects of shell structure and is consistent with the fluctuation-dissipation theorem of the non-equilibrium statistical mechanics. As a first application of the approach, we analyze the fragment mass distribution in 48Ca+238U^{48}\mathrm{Ca}+{}^{238}\mathrm{U} collisions at the bombarding energy Ec.m.=193E_{\text{c.m.}}=193 MeV and compare the calculations with the experimental data.Comment: 15 pages, 8 figures, 2 tables. arXiv admin note: text overlap with arXiv:1706.0356

    Merging of transport theory with TDHF: multinucleon transfer in U+U collisions

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    Multinucleon transfer mechanism in the collision of 238U+238U{}^{238}\text{U}+{}^{238}\text{U} system is investigated at Ec.m.=833E_\text{c.m.} =833 MeV in the framework of the quantal diffusion description based on the stochastic mean-field approach (SMF). Double cross-sections σ(N,Z)\sigma(N,Z) as a function of the neutron and proton numbers, the cross-sections σ(Z)\sigma(Z) and σ(A)\sigma(A) as a function of the atomic numbers and the mass numbers are calculated for production of the primary fragments. The calculation indicates the 238U+238U{}^{238} \text{U}+{}^{238} \text{U} system may be located at an unstable equilibrium state at the potential energy surface with a slightly negative curvature along the beta stability line on the (N,Z)(N,Z)-plane. This behavior may lead to rather large diffusion along the beta stability direction.Comment: 10 pages, 10 figures. arXiv admin note: text overlap with arXiv:1904.0961

    Heavy isotope production in 136Xe+208Pb{}^{136}\text{Xe}+{}^{208}\text{Pb} collisions at Ec.m.=514E_\text{c.m.}=514 MeV

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    Employing the quantal diffusion mechanism for multi-nucleon transfer, the double differential cross-sections are calculated for production of primary projectile-like and target-like fragments in collisions of 136Xe+208Pb{}^{136}\text{Xe}+{}^{208}\text{Pb} system at Ec.m.=514E_\text{c.m.} =514 MeV. Including de-excitation due to neutron emission, the cross-section for production of 210Po{}^{210}\text{Po}, 222Rn{}^{222}\text{Rn} and 224Ra{}^{224}\text{Ra} isotopes are estimated and compared with data.Comment: 7 pages, 3 figures, 2 table
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