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dc.contributor.authorThielemann, Friedrich-Karl
dc.contributor.authorFreiburghaus, C.
dc.contributor.authorRauscher, T.
dc.contributor.authorKratz, K.L.
dc.contributor.authorPfeiffer, B.
dc.contributor.authorCowan, J.J.
dc.contributor.editorHamilton, J.H.
dc.contributor.editorRamayya, A.V.
dc.date.accessioned2014-11-27T09:59:31Z
dc.date.available2014-11-27T09:59:31Z
dc.date.issued1998
dc.identifier.citationThielemann , F-K , Freiburghaus , C , Rauscher , T , Kratz , K L , Pfeiffer , B & Cowan , J J 1998 , Astrophysical and nuclear physics aspects of the r-process . in J H Hamilton & A V Ramayya (eds) , Fission and Properties of Neutron-Rich Nuclei . World Scientific Publishing , Singapore , pp. 47-62 , International Conference on Fission and Properties of Neutron-Rich Nuclei , SANIBEL ISL , 10/11/97 .
dc.identifier.citationconference
dc.identifier.isbn981-02-3537-2
dc.identifier.urihttp://hdl.handle.net/2299/14830
dc.description.abstractThe formation of elements as heavy as Th and U and beyond is due to the rapid neutron-capture process (r-process), which causes the production of highly unstable nuclei near the neutron drip-line and functions via neutron captures, (gamma, n)-photodisintegrations, beta(-)-decays and beta-delayed processes. Neutrino-induced reactions may also play a possible role. Observations of abundances in old (low metallicity) stars indicate that it operates very early in galactic evolution, and is thus related to massive star progenitors forming supernovae and/or neutron stars. The abundances, being in all individual observations identical to solar r-abundances (at least for 4>130), indicate a unique process and witness the interplay between nuclear structure far from beta-stability and the appropriate astrophysical environment. In previous studies we pursued a model-independent approach for the r-process as a function of neutron number densities n(n), temperatures T, and durations times tau. The present study follows the expansion of matter with an initial entropy S and an expansion timescales tau (more suited for astrophysical environments), which can also follow the freeze-out of reactions with declining temperatures and densities explicitely. We compare the similarities and differences between the two approaches. Special emphasis is given to constraints on nuclear properties far from stability, resulting from a comparison with solar r-process abundances in either approach. In particular the behavior of shell closures is examined. In addition, investigations are presented to test whether some features can also provide clear constraints on the permitted astrophysical conditions. We discuss supernova and neutron star merger scenarios with respect to these findings.en
dc.format.extent16
dc.language.isoeng
dc.publisherWorld Scientific Publishing
dc.relation.ispartofFission and Properties of Neutron-Rich Nuclei
dc.titleAstrophysical and nuclear physics aspects of the r-processen
dc.contributor.institutionCentre for Astrophysics Research (CAR)
rioxxterms.typeOther
herts.preservation.rarelyaccessedtrue


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