163 research outputs found

    Kinetic Modeling of Photodegradation of Water-Soluble Polymers in Batch Photochemical Reactor

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    Synthetic water-soluble polymers, well-known refractory pollutants, are abundant in wastewater effluents since they are extensively used in industry in a wide range of applications. These polymers can be effectively degraded by advanced oxidation processes (AOPs). This entry thoroughly covers the development of the photochemical kinetic model of the polyvinyl alcohol (PVA) degradation in UV/H2O2 advanced oxidation batch process that describes the disintegration of the polymer chains in which the statistical moment approach is considered. The reaction mechanism used to describe the photo-degradation of polymers comprises photolysis, polymer chain scission, and mineralization reactions. The impact of operating conditions on the process performance is evaluated. Characterization of the polymer average molecular weights, total organic carbon, and hydrogen peroxide concentrations as essential factors in developing a reliable photochemical model of the UV/H2O2 process is discussed. The statistical moment approach is applied to model the molar population balance of live and dead polymer chains taking into account the probabilistic chain scissions of the polymer. The photochemical kinetic model provides a comprehensive understanding of the impact of the design and operational variables

    Shell model calculations of stellar weak interaction rates: I. Gamow-Teller distributions and spectra of nuclei in the mass range A=45-65

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    Electron capture and beta-decay rates on nuclei in the mass range A=45-65 play an important role in many astrophysical environments. The determination of these rates by large-scale shell model calculations is desirable, but it requires to reproduce the Gamow-Teller strength distributions and spectra of the pf shell nuclei. We show in this paper that large-scale shell model calculations, employing a slightly monopole-corrected version of the wellknown KB3 interaction, fulfill these necessary requirements. In particular, our calculations reproduce the experimentally available GT+ and GT- strength distributions and the nuclear halflives, and describe the nuclear spectra appropriately.Comment: 11 pages, 5 figure

    Meson-exchange enhancement in first-forbidden β\beta -transitions: the case of 50^{50}K and 38^{38}Ca

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    The β\beta- decay of 50^{50}K and 38^{38}Ca have been investigated with the main motive of determining more accurately the first-forbidden β\beta- branches, in particular the rank-zero, Δ\DeltaJ = 0, β\,\beta -transitions. 50^{50}K and 38^{38}Ca have been produced by fragmentation of U and Ti targets respectively, with a 1 GeV proton beam and subsequent on-line mass separation. For 50^{50}K, γ\gamma-ray spectroscopy, as well as delayed neutron spectroscopy by time of flight, were carried out to obtain a detailed decay scheme to 20 (bound and unbound) levels in 50^{50}Ca. The level structur e of 50^{50}Ca can be compared to recent calculations which incorporate 1p1h excitations from the f7/2_{7/2} shell. The first-forbidden β\beta^- transition 50^{50} K(0^-)50\,\to{}^{50}Ca(0+^+) g.s. has been evaluated for the first time by a direct measurement of β\beta- and γ\gamma- activities. Its importance (61.0 ±\pm 7.4%\%) is interpreted as an effect of the meson-exchange current (MEC) l eading to an enhancement factor of 62(5)%\% in comparison with the value predicted by shell-model calculations using the impulse approximation. For the 38^{38} Ca38\,\to{}^{38}K decay, chemical selec tive production was obtained through separation of the molecular ion CaF+^+ without contamination by isobars. In these conditions, the measurement of very weak β\beta-branches, at a level of 103%^{-3}\% decays, could be made and a limit, at the 2σ\sigma-confidence level, has been obtained for the 0+^+\to 0^- branch to the level at Ex_x = 2993 keV (Iβ_\beta < 0.0046%\%). Imp lications of these results on the general trend of meson-exchange enhancements of first-forbidden transitions within the framework of the spherical shell model are discussed

    Spectroscopy of 34,35Si^{34,35}Si by β\beta decay: sd-fp shell gap and single-particle states

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    The 34,35Alβ^{34,35}Al\beta decays were studied at the CERN on-line mass separator ISOLDE by βγ,βγγ\beta-\gamma, \beta-\gamma-\gamma and βnγ\beta-n-\gamma measurements, in order to corroborate thelow-level description of 34Si^{34}Si and to obtain the first information on the level structure of the N=21 isotope 35Si^{35}Si. Earlier observed γ\gamma lines in 34Al^{34} Al decay were confirmed and new gamma transitions following both beta decay and β\beta-delayed neutron emission were established. The first level scheme in 35Si^{35}Si, including three excited states at 910, 974 and 2168 keV, is consistent with Jπ=3/2J^{\pi} =3/2^{-} and 3/2+3/2^{+} for the first two states respectively. Beta-decay half-life of T1/2=38.6(4)T_{1/2} = 38.6 (4) ms and beta-delayed neutron branching PnP_{n} value (Pn=41(13)(P_{n} =41(13) %) were measured unambiguously. The significance of the single-particle energy determination at N=21, Z=14, for assessing the effective interaction in sd-fp shell-model calculations, is discussed and illustrated by predictions for different n-rich isotopes

    Proton instability of 73^{73}Rb

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    The steps of territorial intelligence are based on the emergence of new fashions of exchange within the territory . It acts thus on the territorial visibility and hustles the places of strategic reflexion; by doing this, it takes part within the country, to make move the bond sociétal. This paper subjects a posture of collection and mutualisation of information within the territory

    β\beta-decay half-life of 70^{70}Kr: a bridge nuclide for the rp-process beyond A = 70

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    The β\beta-decay half-life of 70^{70}Kr has been measured for the first time at the ISOLDE PSB Facility at CERN. Mass separated 70^{70}Kr ions were produced by 1 GeV proton induced spallation reactions in a Nb foil. The measured half-life is 57(21) ms. This value is consistent with the half-life calculated assuming a pure Fermi decay, but is clearly lower than the value used in a recent rp-process reaction flow calculation. The result shows that the reaction flow via two-proton-capture of 68^{68}Se is 2.5 times faster than previously calculated assuming an astrophysical temperature of 1.5 GK and a density of 106^{6}g/cm3^{3}

    β\beta- decay of the proton-rich Tz=1/2_{z} = -1/2 nucleus, 71^{71}Kr

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    β\beta- decay of the Tz_{z} = - 1/2 nuclide 71^{71}Kr has been studied at the ISOLDE PSB Facility at CERN. 71^{71}Kr ions were produced in spallation reactions in a Nb foil using the 1 GeV proton beam and studied by means of β\beta-delayed proton, β\beta- and γ\gamma-ray spectroscopy. The half-life and the β\beta-decay energy of 71^{71}Kr were determined using the decay of protons and positrons. These results: T1/2_{1/2} = 100 ± 3 ms and QECQ_\textrm{EC} = 1014^{14} ± 0.32 MeV and the first observation of the b-branch to the 207 keV level in 71^{71}Br makes the extension of the systematics of Gamow-Teller matrix elements of mirror nuclei up to A = 71 possible. Gamow-Teller strength of the same magnitude as that of the fpfp-shell mirror nuclei is observed for the ground state transition

    β\beta - decay of the MT_{T}=-1 nucleus 58^{58}Zn studied by selective laser ionization

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    β\beta - decay of 58^{58}Zn has been studied for the first time. A new laser ion-source concept has been used to produce mass-separated sources for β\beta and γ\gamma - spectroscopy. The half-life of 58^{58}Zn was determined to be 86(18) ms. Comparisons are made with previous data from charge-exchange reactions. Our Gamow-Teller strength to the 1+^{+} state at 1051 keV excitation in 58^{58}Cu agrees well with the value extracted from a recent (3^{3}He, t) study. Extensive shell-model calculations are presented
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