4,844 research outputs found

    Theoretical studies on structural and decay properties of Z=119Z=119 superheavy nuclei

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    In this manuscript, we analyze the structural properties of Z=119Z=119 superheavy nuclei in the mass range of 284 ≤\le A ≤\le 375 within the framework of deformed relativistic mean field theory (RMF) and calculate the binding energy, radii, quadrupole deformation parameter, separation energies and density profile. Further, a competition between possible decay modes such as α−\alpha-decay, β−\beta-decay and spontaneous fission (SF) of the isotopic chain of Z=119Z=119 superheavy nuclei under study is systematically analyzed within self-consistent relativistic mean field model. Moreover, our analysis confirmed that α−\alpha-decay is restricted within the mass range 284 ≤\leq A ≤\leq 296 and thus being the dominant decay channel in this mass range. However, for the mass range 297 ≤\leq A ≤\leq 375 the nuclei are unable to survive fission and hence SF is the principal mode of decay for these isotopes. There is no possibility of β−\beta-decay for the considered isotopic chain. In addition, we forecasted the mode of decay 284−296^{284-296}119 as one α\alpha chain from 284^{284}119 and 296^{296}119, two consistent α\alpha chains from 285^{285}119 and 295^{295}119, three consistent α\alpha chains from 286^{286}119 and 294^{294}119, four consistent alpha chains from 287^{287}119, six consistent alpha chains from 288−293^{288-293}119. Also from our analysis we inferred that for the isotopes 264−266,269^{264-266,269}Bh both α\alpha decay and SF are equally competent and can decay via either of these two modes. Thus, such studies can be of great significance to the experimentalists in very near future for synthesizing Z=119Z=119 superheavy nuclei.Comment: 14 pages, 6 figures. arXiv admin note: text overlap with arXiv:1611.00232, arXiv:1704.0315

    Structural and decay properties of Z=132,138Z=132,138 superheavy nuclei

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    In this paper, we analyze the structural properties of Z=132Z=132 and Z=138Z=138 superheavy nuclei within the ambit of axially deformed relativistic mean-field framework with NL3∗3^{*} parametrization and calculate the total binding energies, radii, quadrupole deformation parameter, separation energies, density distributions. We also investigate the phenomenon of shape coexistence by performing the calculations for prolate, oblate and spherical configurations. For clear presentation of nucleon distributions, the two-dimensional contour representation of individual nucleon density and total matter density has been made. Further, a competition between possible decay modes such as α\alpha-decay, β\beta-decay and spontaneous fission of the isotopic chain of superheavy nuclei with Z=132Z=132 within the range 312 ≤\le A ≤\le 392 and 318 ≤\le A ≤\le 398 for Z=138Z=138 is systematically analyzed within self-consistent relativistic mean field model. From our analysis, we inferred that the α\alpha-decay and spontaneous fission are the principal modes of decay in majority of the isotopes of superheavy nuclei under investigation apart from β\beta decay as dominant mode of decay in 318−322138^{318-322}138 isotopes.Comment: 16 pages, 10 figures , 8 table

    Applicability of shape parameterizations for giant dipole resonance in warm and rapidly rotating nuclei

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    We investigate how well the shape parameterizations are applicable for studying the giant dipole resonance (GDR) in nuclei, in the low temperature and/or high spin regime. The shape fluctuations due to thermal effects in the GDR observables are calculated using the actual free energies evaluated at fixed spin and temperature. The results obtained are compared with Landau theory calculations done by parameterizing the free energy. We exemplify that the Landau theory could be inadequate where shell effects are dominating. This discrepancy at low temperatures and high spins are well reflected in GDR observables and hence insists on exact calculations in such cases.Comment: 10 pages, 2 figure

    Intriguing aspects of F-region plasma irregularities revealed by the Gadanki radar observations during the SAFAR campaign

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    Intriguing new results of F-region irregularities observed using the Gadanki MST radar during the SAFAR campaigns, which were conducted during the equinox and summer of 2008 that corresponds to low solar activity condition, are presented. The summer observations are first of its kind from Gadanki. Observations revealed remarkably different morphology of the F-region irregularities in summer when compared to that in equinox. In summer, the F-region irregularities were observed as horizontally stratified structures, while in equinox they were observed as plume structures. Further, the irregularities in summer commenced during the post-midnight hours in contrast to their commencement in the post-sunset hours and occurrence extending to post-midnight hours in equinox. In addition, an intriguing observation of the summer time irregularities is that they occurred when the background electron density was remarkably low as characterized by the disappearance of the F layer trace in the ionograms. An interesting event of equinox that was observed for 10 h and extended beyond the sunrise time displayed multiple plume structures having periods similar to those of the E-region velocity variations. These observations are discussed with due focus on the genesis of postmidnight F-region irregularities and their possible linkage to the E-region dynamics

    Nuclear reaction studies of unstable nuclei using relativistic mean field formalisms in conjunction with Glauber model

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    We study nuclear reaction cross-sections for stable and unstable projectiles and targets within Glauber model, using densities obtained from various relativistic mean field formalisms. The calculated cross-sections are compared with the experimental data in some specific cases. We also evaluate the differential scattering cross-sections at several incident energies, and observe that the results found from various densities are similar at smaller scattering angles, whereas a systematic deviation is noticed at large angles. In general, these results agree fairly well with the experimental data.Comment: 9 pages, 7 figures, submitted to PR
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