2,484 research outputs found

    The Degasperis-Procesi equation as a non-metric Euler equation

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    In this paper we present a geometric interpretation of the periodic Degasperis-Procesi equation as the geodesic flow of a right invariant symmetric linear connection on the diffeomorphism group of the circle. We also show that for any evolution in the family of bb-equations there is neither gain nor loss of the spatial regularity of solutions. This in turn allows us to view the Degasperis-Procesi and the Camassa-Holm equation as an ODE on the Fr\'echet space of all smooth functions on the circle.Comment: 17 page

    Pilot Experiments with Electrodialysis and Ozonation for the Production of a Fertilizer from Urine

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    Pilot tests were performed with a process combination of electrodialysis and ozonation for the removal of micropollutants and the concentration of nutrients in urine. In continuous and batch experiments, maximum concentration factors up to 3.5 and 4.1 were obtained, respectively. The desalination capacity did not decrease significantly during continuous operation periods of several weeks. Membrane cleaning after 195 days resulted in approximately 35% increase in desalination rate. The Yeast Estrogen Screen (YES), a bioassay that selectively detects oestrogenic compounds, confirmed that about 90% of the oestrogenic activity was removed by electrodialysis. HPLC analysis showed that ibuprofen was removed to a high extent, while other micropollutants were below the detection limit. In view of the fact that ibuprofen is among the most rapidly transported micropollutants in electrodialysis processes, this result indicates that electrodialysis provides an effective barrier for micropollutants. Standardised plant growth tests were performed in the field with the salt solution resulting from the treatment by electrodialysis and subsequent ozonation. The results show that the plant height is comparable to synthetic fertilisers, but the crop yield is slightly lower. The latter is probably caused by volatilisation losses during field application, which can be prevented by improved application technologies

    The geometry of a vorticity model equation

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    We provide rigorous evidence of the fact that the modified Constantin-Lax-Majda equation modeling vortex and quasi-geostrophic dynamics describes the geodesic flow on the subgroup of orientation-preserving diffeomorphisms fixing one point, with respect to right-invariant metric induced by the homogeneous Sobolev norm H1/2H^{1/2} and show the local existence of the geodesics in the extended group of diffeomorphisms of Sobolev class HkH^{k} with k≥2k\ge 2.Comment: 24 page

    A structural evaluation of the tungsten isotopes via thermal neutron capture

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    Total radiative thermal neutron-capture γ\gamma-ray cross sections for the 182,183,184,186^{182,183,184,186}W isotopes were measured using guided neutron beams from the Budapest Research Reactor to induce prompt and delayed γ\gamma rays from elemental and isotopically-enriched tungsten targets. These cross sections were determined from the sum of measured γ\gamma-ray cross sections feeding the ground state from low-lying levels below a cutoff energy, Ecrit_{\rm crit}, where the level scheme is completely known, and continuum γ\gamma rays from levels above Ecrit_{\rm crit}, calculated using the Monte Carlo statistical-decay code DICEBOX. The new cross sections determined in this work for the tungsten nuclides are: σ0(182W)=20.5(14)\sigma_{0}(^{182}{\rm W}) = 20.5(14) b and σ11/2+(183Wm,5.2s)=0.177(18)\sigma_{11/2^{+}}(^{183}{\rm W}^{m}, 5.2 {\rm s}) = 0.177(18) b; σ0(183W)=9.37(38)\sigma_{0}(^{183}{\rm W}) = 9.37(38) b and σ5−(184Wm,8.33μs)=0.0247(55)\sigma_{5^{-}}(^{184}{\rm W}^{m}, 8.33 \mu{\rm s}) = 0.0247(55) b; σ0(184W)=1.43(10)\sigma_{0}(^{184}{\rm W}) = 1.43(10) b and σ11/2+(185Wm,1.67min)=0.0062(16)\sigma_{11/2^{+}}(^{185}{\rm W}^{m}, 1.67 {\rm min}) = 0.0062(16) b; and, σ0(186W)=33.33(62)\sigma_{0}(^{186}{\rm W}) = 33.33(62) b and σ9/2+(187Wm,1.38μs)=0.400(16)\sigma_{9/2^{+}}(^{187}{\rm W}^{m}, 1.38 \mu{\rm s}) = 0.400(16) b. These results are consistent with earlier measurements in the literature. The 186^{186}W cross section was also independently confirmed from an activation measurement, following the decay of 187^{187}W, yielding values for σ0(186W)\sigma_{0}(^{186}{\rm W}) that are consistent with our prompt γ\gamma-ray measurement. The cross-section measurements were found to be insensitive to choice of level density or photon strength model, and only weakly dependent on Ecrit_{\rm crit}. Total radiative-capture widths calculated with DICEBOX showed much greater model dependence, however, the recommended values could be reproduced with selected model choices. The decay schemes for all tungsten isotopes were improved in these analyses.Comment: 25 pages, 15 figures, 15 table

    Many-body approach to proton emission and the role of spectroscopic factors

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    The process of proton emission from nuclei is studied by utilizing the two-potential approach of Gurvitz and Kalbermann in the context of the full many-body problem. A time-dependent approach is used for calculating the decay width. Starting from an initial many-body quasi-stationary state, we employ the Feshbach projection operator approach and reduce the formalism to an effective one-body problem. We show that the decay width can be expressed in terms of a one-body matrix element multiplied by a normalization factor. We demonstrate that the traditional interpretation of this normalization as the square root of a spectroscopic factor is only valid for one particular choice of projection operator. This causes no problem for the calculation of the decay width in a consistent microscopic approach, but it leads to ambiguities in the interpretation of experimental results. In particular, spectroscopic factors extracted from a comparison of the measured decay width with a calculated single-particle width may be affected.Comment: 17 pages, Revte
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