146 research outputs found

    The first direct measurement of ¹²C (¹²C,n) ²³Mg at stellar energies

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    Neutrons produced by the carbon fusion reaction ¹²C(¹²C,n)²³Mg play an important role in stellar nucleosynthesis. However, past studies have shown large discrepancies between experimental data and theory, leading to an uncertain cross section extrapolation at astrophysical energies. We present the first direct measurement that extends deep into the astrophysical energy range along with a new and improved extrapolation technique based on experimental data from the mirror reaction ¹²C(¹²C,p)²³Na. The new reaction rate has been determined with a well-defined uncertainty that exceeds the precision required by astrophysics models. Using our constrained rate, we find that ¹²C(¹²C,n)²³Mg is crucial to the production of Na and Al in Pop-III Pair Instability Supernovae. It also plays a non-negligible role in the production of weak s-process elements as well as in the production of the important galacti

    In-beam spectroscopy of medium- and high-spin states in 133^{133}Ce

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    Medium and high-spin states in 133^{133}Ce were investigated using the 116^{116}Cd(22^{22}Ne, 5n5n) reaction and the Gammasphere array. The level scheme was extended up to an excitation energy of ∼22.8\sim22.8 MeV and spin 93/2 . Eleven bands of quadrupole transitions and two new dipole bands are identified. The connections to low-lying states of the previously known, high-spin triaxial bands were firmly established, thus fixing the excitation energy and, in many cases, the spin parity of the levels. Based on comparisons with cranked Nilsson-Strutinsky calculations and tilted axis cranking covariant density functional theory, it is shown that all observed bands are characterized by pronounced triaxiality. Competing multiquasiparticle configurations are found to contribute to a rich variety of collective phenomena in this nucleus.Comment: 20 pages, 11 figure

    Probing the single-particle character of rotational states in 19^{19}F using a short-lived isomeric beam

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    A beam containing a substantial component of both the JÏ€=5+J^{\pi}=5^+, T1/2=162T_{1/2}=162 ns isomeric state of 18^{18}F and its 1+1^+, 109.77-min ground state has been utilized to study members of the ground-state rotational band in 19^{19}F through the neutron transfer reaction (d(d,p)p) in inverse kinematics. The resulting spectroscopic strengths confirm the single-particle nature of the 13/2+^+ band-terminating state. The agreement between shell-model calculations, using an interaction constructed within the sdsd shell, and our experimental results reinforces the idea of a single-particle/collective duality in the descriptions of the structure of atomic nuclei

    The role of the g9/2 orbital in the development of collectivity in the A = 60 region: The case of 61Co

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    An extensive study of the level structure of 61Co has been performed following the complex 26Mg(48Ca, 2a4npg)61Co reaction at beam energies of 275, 290 and 320 MeV using Gammasphere and the Fragment Mass Analyzer (FMA). The low-spin structure is discussed within the framework of shell-model calculations using the GXPF1A effective interaction. Two quasi-rotational bands consisting of stretched-E2 transitions have been established up to spins I = 41/2 and (43/2), and excitation energies of 17 and 20 MeV, respectively. These are interpreted as signature partners built on a neutron {\nu}(g9/2)2 configuration coupled to a proton {\pi}p3/2 state, based on Cranked Shell Model (CSM) calculations and comparisons with observations in neighboring nuclei. In addition, four I = 1 bands were populated to high spin, with the yrast dipole band interpreted as a possible candidate for the shears mechanism, a process seldom observed thus far in this mass region

    Evidence for Multiple Chiral Doublet Bands in 133^{133}Ce

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    Two distinct sets of chiral-partner bands have been identified in the nucleus 133^{133}Ce. They constitute a multiple chiral doublet (Mχ\chiD), a phenomenon predicted by relativistic mean field (RMF) calculations and observed experimentally here for the first time. The properties of these chiral bands are in good agreement with results of calculations based on a combination of the constrained triaxial RMF theory and the particle-rotor model.Comment: Minor changes based on referee reviews and corrections of some typo

    Key 19^{19}Ne states identified affecting γ\gamma-ray emission from 18^{18}F in novae

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    Detection of nuclear-decay γ\gamma rays provides a sensitive thermometer of nova nucleosynthesis. The most intense γ\gamma-ray flux is thought to be annihilation radiation from the β+\beta^+ decay of 18^{18}F, which is destroyed prior to decay by the 18^{18}F(pp,α\alpha)15^{15}O reaction. Estimates of 18^{18}F production had been uncertain, however, because key near-threshold levels in the compound nucleus, 19^{19}Ne, had yet to be identified. This Letter reports the first measurement of the 19^{19}F(3^{3}He,tγt\gamma)19^{19}Ne reaction, in which the placement of two long-sought 3/2+^+ levels is suggested via triton-γ\gamma-γ\gamma coincidences. The precise determination of their resonance energies reduces the upper limit of the rate by a factor of 1.5−171.5-17 at nova temperatures and reduces the average uncertainty on the nova detection probability by a factor of 2.1.Comment: 6 pages, 4 figure

    New γ\gamma-ray Transitions Observed in 19^{19}Ne with Implications for the 15^{15}O(α\alpha,γ\gamma)19^{19}Ne Reaction Rate

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    The 15^{15}O(α\alpha,γ\gamma)19^{19}Ne reaction is responsible for breakout from the hot CNO cycle in Type I x-ray bursts. Understanding the properties of resonances between Ex=4E_x = 4 and 5 MeV in 19^{19}Ne is crucial in the calculation of this reaction rate. The spins and parities of these states are well known, with the exception of the 4.14- and 4.20-MeV states, which have adopted spin-parities of 9/2−^- and 7/2−^-, respectively. Gamma-ray transitions from these states were studied using triton-γ\gamma-γ\gamma coincidences from the 19^{19}F(3^{3}He,tγt\gamma)19^{19}Ne reaction measured with GODDESS (Gammasphere ORRUBA Dual Detectors for Experimental Structure Studies) at Argonne National Laboratory. The observed transitions from the 4.14- and 4.20-MeV states provide strong evidence that the JπJ^\pi values are actually 7/2−^- and 9/2−^-, respectively. These assignments are consistent with the values in the 19^{19}F mirror nucleus and in contrast to previously accepted assignments

    Fast-timing measurements in the ground-state band of 114Pd

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    Using a hybrid Gammasphere array coupled to 25 LaBr3(Ce) detectors, the lifetimes of the first three levels of the yrast band in 114Pd, populated via 252Cf decay, have been measured. The measured lifetimes are τ2+ = 103(10) ps, τ4+ = 22(13) ps, and τ6+ 10 ps for the 2+ 1 , 4+ 1 , and 6+ 1 levels, respectively. Palladium-114 was predicted to be the most deformed isotope of its isotopic chain, and spectroscopic studies have suggested it might also be a candidate nucleus for low-spin stable triaxiality. From the lifetimes measured in this work, reduced transition probabilities B(E2; J → J − 2) are calculated and compared with interacting boson model, projected shell model, and collective model calculations from the literature. The experimental ratio RB(E2) = B(E2; 4+ 1 → 2+ 1 )/B(E2; 2+ 1 → 0+ 1 ) = 0.80(42) is measured for the first time in 114Pd and compared with the known values RB(E2) in the palladium isotopic chain: the systematics suggest that, for N = 68, a transition from γ -unstable to a more rigid γ -deformed nuclear shape occurs.This work was financially supported by the Science and Technology Facility Council (STFC) Grants No. ST/L005840/1, No. ST/L005743/1, and No. ST/G000751/1. This work has also been partially supported by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics under Contract No. DE-AC02-06CH11357 (ANL). E.R.G. would like to acknowledge the STFC for funding via his Ph.D. studentship. D.J.H. acknowledges the National Science Foundation, Grant No. PHY-1502092. E.A.S. and O.Y. would like to acknowledge the project DFNI-E02/6
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