LA-13686-C Confuence Issued: ]anuay 2000 , ~ Workshop on the Origz”nof the “ Heavy Elements: Astrophysical Models and Experimen~al Challenges Santa Fe, New Mexico %ptembi?r 34,1999 Edited by Robert C. Haight John L. Ullmann Daniel D. Stro&nan Paul E. Koehler* Franz Kaeppeler** *LaboratoyAjWte atLosAhnos.PhysicsDivision,OakRidgeNationalLaboratory, Bldg.6010,MS6354,OakRidge,TN 37831-6354 **[email protected],K Bau425,D-76021, Pos~ach3640,Kdsruhe, Germany Los Alamos NATIONAL LABORATORY LosAlamosN,ewMexico87545 ‘1 .-..= $..:,.,- , -<.,m—.,-—~—...—::—m.—,. .,., ..........-;X-TT---.-, --->. .. ... . .- DISCLAIMER This repo~ was prepared as an account of work sponsored by an agency of the United States Government. 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Workshop on the Origin of the Heavy Elements: Astrophysical Models and Experimental Challenges Edited by R. C. Haight, J. L. Ullmann, D. D. Strottman LosAlamosNationalLaboratory .’ P. E. Koehler OakRidgeNationalLaboratory and F. Kaeppeler ,,., Forschungszentrum Karlsruhe ,,- ABSTRACT t ‘, This Workshop was held on September 3-4, 1999,following the 10th International Symposium on Capture Gamma-RaySpectroscopy. Presentations were made by 14speakers, 6 from the US and 8 horn other countries on topics relevant to s-, r- and rp-process nucleosynthesis. Laboratory experiments, both present and planned, and astrophysical observations were represented as were astrophysical models. Approximately 50 scientistsparticipated inthis Workshop. These Proceedings consist of copies of vu-graphs presented at the Workshop. For iirther ~ormation, the interested readers are referred to the authors. 3 :’ ——.— —.. .., ,. m.. or------- ,. ,. ———. -- Workshop on the Origin of the Heavy Elements: Astrophysical Models and Experimental Challenges Schedule Friday, September 3 1:50-2:00 Welcome r-process Nucleosynthesis 2:00-2:30 Peter Moller Nuclear Mass Models: Past Achievements, Current Status, and Future Challenges 2:30-3:00 Stephen A. Becker Approximating the r-process on Earth with Thermonuclear Explosions 3:00-3:30 Stephane Goriely Uncertainties inthe Th Cosmochronolofg 3:30-4:00 Discussion on the r-process with refreshments 4:00-4:30 l?aolo Mutd . Neutron Capture Cross Sections of Kr-84 and Kr-86 and Their Impact on Stellar Nucleosynthesis Proton-rich Nuclides . 4:30-5:00 Paul Kienle Half-lives ofrp-process WaitingPoint Nuclei 5:00-5:30 H. H. Pitz Photoactivation of 180mTa and Implications for the Nucleosynthesis ofNature’s Rarest Stable Isotope 5:30-7:00 Discussion ofproton-rich nuclei with refieshents - Continued (next page) Workshop Schedule (continued) Saturday, September 4 Astronomical Observations and Models 8:30-9:00 A. Mengoni Structure and EM Dissociation of 9Be 9:00-9:30 Joyce Ann Guzik Sensitivity of Solar Oscillation Frequencies to Element Abundances and Composition Gradients 9:30-10:00 CorinueNeuforge Linking Field Metal-Poor Stars and Globuk Clusters 10:00-10:30 Hideo Harada Thermal Neutron Capture Cross Sections and Resonance Integrals of Fission Products 10:30-11:00 Break and Discussion New Capabilities and Plans 11:00-11:30 0. Shcherbakov Neutron Time-of-flight Sepctrometer GNEIS at the l-GeV Proton Synchrotronsof PNPI 11:30-12:00 Rene Reifhrth The Use of 4pi Detectors at Spallation Neutron Sources 12:00-12:30 Paul Koehler Plans for Measurements at Oak Ridge 12:30-1:00 Working Lunch – 1:00-1:30 Robert Rundberg Plans for Measurements at Los Alamos Nuclear Mass Models: Past Achievements, Current Status and Challenges Future Peter M611er Theoretical Division, Los AlamosNational”Laboratoq, Los Alamos, Nil! 87545 The history of mass models is briefly dkcussed. Features of some commonlyused mass models, such as those developed by Liran%eldes, von Groot~Hilf, Pearson-Tondeur, Myers-Swiatecki, and M611er-Nixare compared and discussed. . We particularly discuss how the models behave when applied to masses outside the region to which parameters were adjusted, that is how reliably the models behave in regions close to the tilp lines ahd in the superheavy-element region. We discuss the deviations that remain between model results and experimental data, and what physical effects need be more realistically described to remove such deviations so that greater model accuracies may be obtained. Our latest manuscripts and mass tables are available from URL http: //t2.lanl.gov and various Iiis horn this U~L. For data related to the M611er-Nixmass model the URL is: . http://t2.lanl.gov/data/astro/motix96/moWx.html “ ...— . ——— ___ ____ ‘CD ... X2 ..’”& Cn ?3 c C6 .>E CD -3 E .- J2 a S -- c1) E a 3 u a 5 .0 -g -. ‘5 “c ‘0 -, m ‘to -.. s E 75 8’”. % ‘ u c x ‘. 0 o .- -- .. . . a) .. E “CD (n ‘c m u) .. (5 ‘- 4--J al “ E D -- u > --- ...-a) 0 .L. Q CL ,, .,, 1- C/3 C6 u) s c 0 c Q) .- .- Co f E -5 c .- u 73 a) ‘CD ) CDCr ii > cl) ,,, , L E (1) a= .- :, c1) u Lo m o c a) E u a) o o c) . . . E 0 a) E cd % L Q c cd :, o a) CD.- 5 m E ,, -E CD cd .’ c co CD c o E 0 ‘, ‘0 c) ,., c 0 ,, c) cd ,., a ,; E ~. E c ,“ cd CD +, c1) L E :,, C6 5 .- .0 CL L (n 3 = c .— ..... _ c1) c 2 -IL !, 1 ,. , $ --,----- ...,4,.. ~. ,,,,,.........fi.,. ......~, ......,,,.!,. .,. .,r,. , :, , .,. -J.!..7/.7.,.:,,..1,... .,,..;,..’<.f;.<,., .,.<. ..., ,.T:s.s--?r .,,:.,. , . ,, .,, Macroscopic-microscopic model: Q Macroscopic models: Liquid-drop, droplet, finite-range liquid-drop and finite-range droplet models. b Microscopic models: Nilsson modified oscillator, two- center oscillator, Woods-Saxon and folded-Yukawa single-particle potentials. ~ For each model several parameter sets. For progress it k necessary to proceed in a consistent man- ner with a clear strategy of model development.