J/A+A/513/A61ivo://CDS.VizieR/J/A+A/513/A61doi:10.26093/cds/vizier.35130061CDSPanov I.V.Korneev I.Yu.Rauscher T.Martinez-Pinedo G.Kelic-Heil A.,Zinner N.T.Thielemann F.-K.2023-04-24T14:18:08Z2010-06-03T11:55:33ZCDS support team

CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France

cds-question@unistra.fratomic-physicsNeutron-induced reaction rates, including fission, are calculated in the temperature range 10^8^<=T(K)<=10^10^ within the framework of the statistical model for targets with atomic number 84<=Z<=118 (from Po to Uuo) from the neutron to the proton drip-line. Four sets of rates have been calculated, utilizing - where possible - consistent nuclear data for neutron separation energies and fission barriers from Thomas-Fermi (TF), Extended Thomas-Fermi plus Strutinsky Integral (ETFSI), Finite-Range Droplet Model (FRDM) and Hartree-Fock-Bogolyubov (HFB) predictions. Tables of calculated values as well as analytic seven parameter fits in the standard REACLIB format are supplied. We also discuss the sensitivity of the rates to the input, aiming at a better understanding of the uncertainties introduced by the nuclear input.2010A&A...513A..61Phttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/513/A61CatalogResearchIsServedByTAP VizieR generic servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/A+A/513/A61https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/A+A/513/A61http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/A+A/513/A61https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/A+A/513/A61https://vizier.iucaa.in/viz-bin/votable?-source=J/A+A/513/A61http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/A+A/513/A61GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/A+A/513/A61/ratesNeutron-induced fission and capture rates for the 4 different models (tables 7--9 of paper)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintMmeta.id;stat.fitcharElTarget element (corresponding to Z)phys.atmol.elementcharAAtomic mass number of the targetphys.atmol.numberintZ[84,118] Charge number of the targetphys.atmol.elementintT9[0.10/10.00] TemperatureGKphys.temperaturefloatpfPartition function of the targetphys.atmoldoublenfNeutron-induced fission rate for ground statecm**3.s**-1.mol**-1arith.rate;phys.atmol.collisionaldoublenf*Neutron-induced fission rate with thermally populated target statescm**3.s**-1.mol**-1arith.rate;phys.atmol.collisionaldoublengNeutron capture rate for the ground statecm**3.s**-1.mol**-1arith.rate;phys.atmol.collisionaldoubleng*Neutron capture rate with thermally populated target statescm**3.s**-1.mol**-1arith.rate;phys.atmol.collisionaldoubleJ/A+A/513/A61/fittingCombined table from original tablesReacmeta.notechara2Coefficient a2 of the forward reaction r_i_ (1)meta.notedoublea3Coefficient a3 of the forward reaction r_i_ (1)meta.notedoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintElTarget element (corresponding to Z)phys.atmol.elementcharAAtomic mass number of the targetphys.atmol.numberintZ[84,118] Charge number of the targetphys.atmol.elementinti[0/1] Number of fitting curve (1)meta.idinta0Coefficient a0 of the forward reaction r_i_ (1)meta.notedoublea1Coefficient a1 of the forward reaction r_i_ (1)meta.notedoublea4Coefficient a4 of the forward reaction r_i_ (1)meta.notedoublea5Coefficient a5 of the forward reaction r_i_ (1)meta.notedoublea6Coefficient a6 of the forward reaction r_i_ (1)meta.notedoublezeta? Mean square error for direct reactions (Eq.(5))stat.errordoublenullable