1,067 research outputs found

    Experimental evidence of a natural parity state in 26^{26}Mg and its impact to the production of neutrons for the s process

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    We have studied natural parity states in 26^{26}Mg via the 22^{22}Ne(6^{6}Li,d)26^{26}Mg reaction. Our method significantly improves the energy resolution of previous experiments and, as a result, we report the observation of a natural parity state in 26^{26}Mg. Possible spin-parity assignments are suggested on the basis of published γ\gamma-ray decay experiments. The stellar rate of the 22^{22}Ne(α\alpha,γ\gamma)26^{26}Mg reaction is reduced and may give rise to an increase in the production of s-process neutrons via the 22^{22}Ne(α\alpha,n)25^{25}Mg reaction.Comment: Published in PR

    Finite type approximations of Gibbs measures on sofic subshifts

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    Consider a H\"older continuous potential ϕ\phi defined on the full shift A^\nn, where AA is a finite alphabet. Let X\subset A^\nn be a specified sofic subshift. It is well-known that there is a unique Gibbs measure μϕ\mu_\phi on XX associated to ϕ\phi. Besides, there is a natural nested sequence of subshifts of finite type (Xm)(X_m) converging to the sofic subshift XX. To this sequence we can associate a sequence of Gibbs measures (μϕm)(\mu_{\phi}^m). In this paper, we prove that these measures weakly converge at exponential speed to μϕ\mu_\phi (in the classical distance metrizing weak topology). We also establish a strong mixing property (ensuring weak Bernoullicity) of μϕ\mu_\phi. Finally, we prove that the measure-theoretic entropy of μϕm\mu_\phi^m converges to the one of μϕ\mu_\phi exponentially fast. We indicate how to extend our results to more general subshifts and potentials. We stress that we use basic algebraic tools (contractive properties of iterated matrices) and symbolic dynamics.Comment: 18 pages, no figure

    Multi-channel R-matrix analysis of CNO cycle reactions

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    The CNO cycle is the main process for hydrogen burning in stars somewhat more massive than the Sun. The reaction cross sections at Gamow energies are typically in the femto to pico-barn range and are consequently very difficult to measure experimentally. The CNO reaction rates are based on extrapolations of experimental data from higher energies. We are developing a multi-channel R-matrix code (AZURE) to provide a new and more comprehensive tool for fitting experimental data and making extrapolations to lower energies in all reaction and scattering channels. The 14N(p,γ )15O reaction is the slowest reaction of the CNO cycle and thus it determines the energy production rate of CNO burning. Furthermore, this reaction plays an important role in the determination of Globular Cluster age, since the position of the turnoff point, at which the GC stars escape from the Main Sequence, is powered by the onset of the CNO burning, whose bottleneck is the 14N(p, γ )15O. We have made a reanalysis of the most recent experimental data on the ground state and the 6.18 MeV transitions. The ratio of the cross sections of the 15N(p, γ )16O and 15N(p,α)12C reactions determines how much catalytic material passes to higher CNO cycles and has an effect on the production of heavier elements, particularly 16O and 17O. Simultaneous analysis of both reactions for all channels suggests that the ratio σγ/σα is smaller than previously reported

    Independent measurement of the Hoyle state β\beta feeding from 12B using Gammasphere

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    Using an array of high-purity Compton-suppressed germanium detectors, we performed an independent measurement of the β\beta-decay branching ratio from 12B^{12}\mathrm{B} to the second-excited (Hoyle) state in 12C^{12}\mathrm{C}. Our result is 0.64(11)%0.64(11)\%, which is a factor 2\sim 2 smaller than the previously established literature value, but is in agreement with another recent measurement. This could indicate that the Hoyle state is more clustered than previously believed. The angular correlation of the Hoyle state γ\gamma cascade has also been measured for the first time. It is consistent with theoretical predictions
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