1,106 research outputs found

    Triaxial deformation in 10Be

    Get PDF
    The triaxial deformation in 10^{10}Be is investigated using a microscopic α+α+n+n\alpha+\alpha+n+n model. The states of two valence neutrons are classified based on the molecular-orbit (MO) model, and the π\pi-orbit is introduced about the axis connecting the two α\alpha-clusters for the description of the rotational bands. There appear two rotational bands comprised mainly of Kπ=0+K^\pi = 0^+ and Kπ=2+K^\pi = 2^+, respectively, at low excitation energy, where the two valence neutrons occupy Kπ=3/2K^\pi = 3/2^- or Kπ=1/2K^\pi = 1/2^- orbits. The triaxiality and the KK-mixing are discussed in connection to the molecular structure, particularly, to the spin-orbit splitting. The extent of the triaxial deformation is evaluated in terms of the electro-magnetic transition matrix elements (Davydov-Filippov model, Q-invariant model), and density distribution in the intrinsic frame. The obtained values turned out to be γ=15o20o\gamma = 15^o \sim 20^o.Comment: 15 pages, latex, 3 figure

    Systematic analyses of the t t clustering effect in He isotopes

    Get PDF
    A systematic study on the ground state structure of He isotopes including 10He is presented through a new method developed on the basis of antisymmetrized molecular dynamics AMD , the generator coordinate method GCM , and the stochastic variational method SVM . In this approach, variational calculations are carried out by means of the GCM with the AMD wave functions produced by means of the SVM. A role of the t t cluster component is examined with the present method, allowing the wider configuration space containing simultaneously the t t valence neutrons structure and 4He valence neutrons strucutur

    Static and Dynamic Chain Structures in the Mean-Field Theory

    Full text link
    We give a brief overview of recent work examining the presence of α\alpha-clusters in light nuclei within the Skyrme-force Hartree-Fock model. Of special significance are investigations into α\alpha-chain structures in carbon isotopes and 16^{16}O. Their stability and possible role in fusion reactions are examined in static and time-dependent Hartree-Fock calculations. We find a new type of shape transition in collisions and a centrifugal stabilization of the 4α4\alpha chain state in a limited range of angular momenta. No stabilization is found for the 3α3\alpha chain.Comment: Fusionn 11 Conference, St. Malo, France, 201

    A massive star origin for an unusual helium-rich supernova in an elliptical galaxy

    Full text link
    The unusual helium-rich (type Ib) supernova SN 2005E is distinguished from any supernova hitherto observed by its faint and rapidly fading light curve, prominent calcium lines in late-phase spectra and lack of any mark of recent star formation near the supernova location. These properties are claimed to be explained by a helium detonation in a thin surface layer of an accreting white dwarf (Perets et al. 2010). Here we report on observations of SN 2005cz appeared in an elliptical galaxy, whose observed properties resemble those of SN 2005E in that it is helium-rich and unusually faint, fades rapidly, shows much weaker oxygen emission lines than those of calcium in the well-evolved spectrum. We argue that these properties are best explained by a core-collapse supernova at the low-mass end (812M8-12 M_{\odot}) of the range of massive stars that explode (Smartt 2009). Such a low mass progenitor had lost its hydrogen-rich envelope through binary interaction, having very thin oxygen-rich and silicon-rich layers above the collapsing core, thus ejecting a very small amount of radioactive 56^{56}Ni and oxygen. Although the host galaxy NGC 4589 is an elliptical, some studies have revealed evidence of recent star-formation activity (Zhang et al. 2008), consistent with the core-collapse scenario.Comment: Accepted by Nature (24 March 2010), 32 pages including Supplementary Informatio

    Important role of the spin-orbit interaction in forming the 1/2^+ orbital structure in Be isotopes

    Get PDF
    The structure of the second 0^+ state of ^{10}Be is investigated using a microscopic α+α+n+n\alpha+\alpha+n+n model based on the molecular-orbit (MO) model. The second 0^+ state, which has dominantly the (1/2^+)^2 configuration, is shown to have a particularly enlarged αα\alpha-\alpha structure. The kinetic energy of the two valence neutrons occupying along the αα\alpha-\alpha axis is reduced remarkably due to the strong α\alpha clustering and, simultaneously, the spin-orbit interaction unexpectedly plays important role to make the energy of this state much lower. The mixing of states with different spin structure is shown to be important in negative-parity states. The experimentally observed small-level spacing between 1^- and 2^- (~ 300 keV) is found to be an evidence of this spin-mixing effect. ^{12}{Be} is also investigated using α+α+4n\alpha+\alpha+4n model, in which four valence neutrons are considered to occupy the (3/2^-)^2(1/2^+)^2 configuration. The energy surface of ^{12}Be is shown to exhibit similar characteristics, that the remarkable α\alpha clustering and the contribution of the spin-orbit interaction make the binding of the state with (3/2^-)^2(1/2^+)^2 configuration properly stronger in comparison with the closed p-shell (3/2^-)^2(1/2^-)^2 configuration.Comment: 14 pages, 4 figure

    Molecular-orbital structure in neutron-rich C isotopes

    Get PDF
    The molecule-like structure of the C isotopes (A=12, 14, 16) is investigated using a microscopic α+α+α+n+n+\alpha+\alpha+\alpha+n+n+\cdot \cdot \cdot model. The valence neutrons are classified based on the molecular-orbit (MO) model, and both π\pi-orbit and σ\sigma-orbit are introduced around three α\alpha-clusters. The valence neutrons which occupy the π\pi-orbit increase the binding energy and stabilize the linear-chain of 3α\alpha against the breathing-like break-up. However, 14^{14}C with the π\pi-orbit does not show clear energy minimum against the bending-like path. The combination of the valence neutrons in the π\pi- and the σ\sigma-orbit is promising to stabilize the linear-chain state against the breathing- and bending- modes, and it is found that the excited states of 16^{16}C with the (3/2π)2(1/2σ)2(3/2^-_\pi)^2(1/2^-_\sigma)^2 configuration for the four valence neutrons is one of the most promising candidates for such structure

    SN 2006bp: Probing the Shock Breakout of a Type II-P Supernova

    Full text link
    HET optical spectroscopy and unfiltered ROTSE-III photometry spanning the first 11 months since explosion of the Type II-P SN 2006bp are presented. Flux limits from the days before discovery combined with the initial rapid brightening suggest the supernova was first detected just hours after shock breakout. Optical spectra obtained about 2 days after breakout exhibit narrow emission lines corresponding to HeII 4200, HeII 4686, and CIV 5805 in the rest frame, and these features persist in a second observation obtained 5 hours later; however, these emission lines are not detected the following night nor in subsequent observations. We suggest that these lines emanate from material close to the explosion site, possibly in the outer layers of the progenitor that have been ionized by the high energy photons released at shock breakout. A P-Cygni profile is observed around 4450 A in the +2 and +3 day spectra. Previous studies have attributed this feature to high velocity H-beta, but we discuss the possibility that this profile is instead due to HeII 4687. Further HET observations (14 nights in total) covering the spectral evolution across the photometric plateau up to 73 days after breakout and during the nebular phase around day +340 are presented, and expansion velocities are derived for key features. The measured decay slope for the unfiltered light curve is 0.0073 +/- 0.0004 mag/day between days +121 and +335, which is significantly slower than the decay of rate 56Co. We combine our HET measurements with published X-ray, UV, and optical data to obtain a quasi-bolometric light curve through day +60. We see a slow cooling over the first 25 days, but no sign of an early sharp peak; any such feature from the shock breakout must have lasted less than ~1 day.[ABRIDGED]Comment: ApJ accepted, 43 page
    corecore