15,048,772 research outputs found

    The Nucleosynthesis and Reaction Rates of Fluorine 19 (19F^{19}F) in the Sun

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    We investigate the abundance of 19F^{19}F in the Sun through the nucleosynthesis scenario. In addition, we calculate the rate equations and reaction rates of the nucleosynthesis of 19F^{19}F at different temperature scale. Other important functions of this nucleosynthesis (nuclear partition function and statistical equilibrium conditions) are also obtained. The resulting stability of 19F^{19}F occurs at nucleus with A = 19 and Mass Excess= -1.4874 MeV. As a result, this will tend to a series of neutron captures and beta-decay until 19F^{19}F is produced. The reaction rate of 15N^{15}N (α\alpha, γ\gamma) 19F^{19}F was dominated by the contribution of three low-energy resonances, which enhanced the final 19F^{19}F abundance in the envelope.Comment: arXiv admin note: substantial text overlap with arXiv:astro-ph/0407551 by other author

    When does the Bombieri-Vinogradov Theorem hold for a given multiplicative function?

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    Let ff and gg be 11-bounded multiplicative functions for which fg=1.=1f*g=1_{.=1}. The Bombieri-Vinogradov Theorem holds for both ff and gg if and only if the Siegel-Walfisz criterion holds for both ff and gg, and the Bombieri-Vinogradov Theorem holds for ff restricted to the primes.Comment: 19 page

    Spectroscopy of 19^{19}Ne for the thermonuclear 15^{15}O(α,γ\alpha,\gamma)19^{19}Ne and 18^{18}F(p,αp,\alpha)15^{15}O reaction rates

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    Uncertainties in the thermonuclear rates of the 15^{15}O(α,γ\alpha,\gamma)19^{19}Ne and 18^{18}F(p,αp,\alpha)15^{15}O reactions affect model predictions of light curves from type I X-ray bursts and the amount of the observable radioisotope 18^{18}F produced in classical novae, respectively. To address these uncertainties, we have studied the nuclear structure of 19^{19}Ne over Ex=4.05.1E_{x} = 4.0 - 5.1 MeV and 6.17.36.1 - 7.3 MeV using the 19^{19}F(3^{3}He,t)19^{19}Ne reaction. We find the JπJ^{\pi} values of the 4.14 and 4.20 MeV levels to be consistent with 9/29/2^{-} and 7/27/2^{-} respectively, in contrast to previous assumptions. We confirm the recently observed triplet of states around 6.4 MeV, and find evidence that the state at 6.29 MeV, just below the proton threshold, is either broad or a doublet. Our data also suggest that predicted but yet unobserved levels may exist near the 6.86 MeV state. Higher resolution experiments are urgently needed to further clarify the structure of 19^{19}Ne around the proton threshold before a reliable 18^{18}F(p,αp,\alpha)15^{15}O rate for nova models can be determined.Comment: 5 pages, 3 figures, Phys. Rev. C (in press

    Quasifission and difference in formation of evaporation residues in the 16^{16}O+184^{184}W and 19^{19}F+181^{181}Ta reactions

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    The excitation functions of capture, complete fusion, and evaporation residue formation in the 16^{16}O+184^{184}W and 19^{19}F+181^{181}Ta reactions leading to the same 200^{200}Pb compound nucleus has been studied theoretically to explain the experimental data showing more intense yield of evaporation residue in the former reaction in comparison with that in the latter reaction. The observed difference is explained by large capture cross section in the former and by increase of the quasifission contribution to the yield of fission-like fragments in the 19^{19}F+181^{181}Ta reaction at large excitation energies. The probability of compound nucleus formation in the 16^{16}O+184^{184}W reaction is larger but compound nuclei formed in both reactions have similar angular momentum ranges at the same excitation energy. The observed decrease of evaporation residue cross section normalized to the fusion cross section in the 19^{19}F+181^{181}Ta reaction in comparison with the one in the 16^{16}O+184^{184}W reaction at high excitation energies is explained by the increase of hindrance in the formation of compound nucleus connected with more quick increase of the quasifission contribution in the 19^{19}F induced reaction. The spin distributions of the evaporation residue cross sections for the two reactions are also presented.Comment: 11 pages, 5 figure

    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 1.5171.5-17 at nova temperatures and reduces the average uncertainty on the nova detection probability by a factor of 2.1.Comment: 6 pages, 4 figure

    Convexity and a sum-product type estimate

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    In this paper we further study the relationship between convexity and additive growth, building on the work of Schoen and Shkredov (\cite{SS}) to get some improvements to earlier results of Elekes, Nathanson and Ruzsa (\cite{ENR}). In particular, we show that for any finite set ARA\subset{\mathbb{R}} and any strictly convex or concave function ff, A+f(A)A24/19(logA)2/19|A+f(A)|\gg{\frac{|A|^{24/19}}{(\log|A|)^{2/19}}} and max{AA, f(A)+f(A)}A14/11(logA)2/11.\max\{|A-A|,\ |f(A)+f(A)|\}\gg{\frac{|A|^{14/11}}{(\log|A|)^{2/11}}}. For the latter of these inequalities, we go on to consider the consequences for a sum-product type problem
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