Les Termes Pétroliers 1981
DOI: 10.1007/978-94-011-8080-1_13
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Cited by 10 publications
(15 citation statements)
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“…The C-burning phase raises the very interesting question of the fusion of light heavy ions below the Coulomb barrier, and in particular of the origin of the very pronounced structures observed in the 12 C + 12 C fusion cross section at low energies. The devoted experimental and theoretical works do not provide fully satisfactory solutions ( [23,174,175]).…”
Section: Carbon Burningmentioning
confidence: 99%
“…The C-burning phase raises the very interesting question of the fusion of light heavy ions below the Coulomb barrier, and in particular of the origin of the very pronounced structures observed in the 12 C + 12 C fusion cross section at low energies. The devoted experimental and theoretical works do not provide fully satisfactory solutions ( [23,174,175]).…”
Section: Carbon Burningmentioning
confidence: 99%
“…The inverse transformation of 187 Os via free-electron captures is certainly responsible for additional corrections to the stellar 187 Re/ 187 Os abundance ratio (e.g. [5,125]). Further complications arise because these two nuclides can be concomitantly destroyed by neutron captures in certain stellar locations [125].…”
Section: "Long-lived" Nucleo-cosmochronometers: Generalitiesmentioning
confidence: 99%
“…The long-lived 176 Lu (t 1/2 = 41 Gy) has the remarkable property of being shielded from the r-process, and thus to be a pure s-process product. It has been proposed by Dave and his collaborators [19], and independently by [6], to be a potential chronometer for the s-process, the other long-lived radionuclides probing the r-process instead. These early works pointed out some possible uncertainties in the solar 176 Lu abundance, as well as in its production predicted from s-process models.…”
Section: Lu a Long-lived S-process Radionuclidementioning
confidence: 99%
“…Reaction rates for medium or heavy nuclei, applied in astrophysical applications, have been calculated until now on the Data tables are only available in electronic form at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/487/767 basis of the Hauser-Feshbach (HF) statistical model (Hauser & Feshbach 1952), adopting simplified schemes to estimate the capture reaction cross section of a given target nucleus, not only in its ground state but also in the different thermally populated states of the stellar plasma at a given temperature (Arnould 1972;Holmes et al 1976;Woosley et al 1978, Sargood 1982Thielemann et al 1987;Cowan et al 1991;Rauscher & Thielemann 2001;Aikawa et al 2005). Such schemes include a number of approximations that have never been tested, such as the neglect of delayed particle emission during the electromagnetic decay cascade or the absence of the preequilibrium contribution at increasing incident energies or for exotic neutron-rich nuclei.…”
Section: Introductionmentioning
confidence: 99%