References quoted in the ENSDF dataset: 206PT ADOPTED LEVELS
7 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Atomic Nuclei 74, 1435 (2011)
I.N.Borzov
Beta-decay of nuclei near the neutron shell N = 126
RADIOACTIVITY 194,196,198,200,202,204,206,208Os, 202,204,206,208,210,212,214,216Pt, 198,200,202,204,206,208Ir, 202,204,206,208Au(β-); calculated decay energy release, T1/2, β-delayed neutron branching ratios. QRPA approach.
doi: 10.1134/S1063778811100024
Phys.Lett. B 717, 371 (2012)
J.Kurcewicz, F.Farinon, H.Geissel, S.Pietri, C.Nociforo, A.Prochazka, H.Weick, J.S.Winfield, A.Estrade, P.R.P.Allegro, A.Bail, G.Belier, J.Benlliure, G.Benzoni, M.Bunce, M.Bowry, R.Caballero-Folch, I.Dillmann, A.Evdokimov, J.Gerl, A.Gottardo, E.Gregor, R.Janik, A.Kelic-Heil, R.Knobel, T.Kubo, Yu.A.Litvinov, E.Merchan, I.Mukha, F.Naqvi, M.Pfutzner, M.Pomorski, Zs.Podolyak, P.H.Regan, B.Riese, M.V.Ricciardi, C.Scheidenberger, B.Sitar, P.Spiller, J.Stadlmann, P.Strmen, B.Sun, I.Szarka, J.Taieb, S.Terashima, J.J.Valiente-Dobon, M.Winkler, Ph.Woods
Discovery and cross-section measurement of neutron-rich isotopes in the element range from neodymium to platinum with the FRS
NUCLEAR REACTIONS 9B(238U, X)157Nd/158Nd/159Nd/160Nd/161Nd/160Pm/161Pm/162Pm/163Pm/163Sm/164Sm/165Sm/167Eu/168Eu/167Gd/168Gd/169Gd/170Gd/169Tb/170Tb/171Tb/172Tb/171Dy/172Dy/173Dy/174Dy/173Ho/174Ho/175Ho/176Ho/176Er/177Er/178Er/178Tm/179Tm/180Tm/181Tm/181Yb/182Yb/183Yb/184Yb/185Yb/185Lu/186Lu/187Lu/188Lu/190Hf/193Ta/194Ta/195W/196W/197W/198Re/199Re/202Os/203Os/205Ir/206Pt/207Pt/208Pt, E=1 GeV/nucleon; measured time-of-flight, energy loss, fragment σ using FRS at GSI facility; discovered 60 new isotopes. Comparison of σ(A, Z) distributions with ABRABLA, COFRA and EPAX-3 model calculations.
doi: 10.1016/j.physletb.2012.09.021
Phys.Rev. C 93, 025805 (2016)
T.Marketin, L.Huther, G.Martinez-Pinedo
Large-scale evaluation of β-decay rates of r-process nuclei with the inclusion of first-forbidden transitions
RADIOACTIVITY Z=8-110, N=11-236, A=19-339(β-); calculated decay rates for Gamow-Teller and first-forbidden transitions, total decay rates, P0n, P1n, P3n, P4n, P5n delayed-neutron emission probabilities, average energies of electrons antineutrinos and photons after decay. Z=47-48, A=114-154; calculated Q(β-). Z=36-43, A=93-117; Z=37-50, N=65-88; Z=24-32, N=50; Z=42-49, N=82; Z=6-73, N=126; 194,195,196Re, 199,200Os, 198,199,201,202Ir, 203,204Pt, 204Au, 211,212,213Tl, 218,219Bi(β-); calculated half-lives for β- decay. Fully self-consistent covariant density functional theory (CDFT) framework with the ground states calculated with relativistic Hartree-Bogoliubov (RHB) model, and excited states within the proton-neutron relativistic quasiparticle random phase approximation (pn-RQRPA). Comparison with experimental Q values and half-lives. Calculated abundances of heavy nuclei, and evolution of neutron-to-seed ratio resulting from hot and cold r-processes using half-lives from the FRDM and the current model. Supplementary file contains theoretical values of half-lives and Pxn for 5409 neutron-rich nuclei.
doi: 10.1103/PhysRevC.93.025805
At.Data Nucl.Data Tables 125, 1 (2019)
P.Moller, M.R.Mumpower, T.Kawano, W.D.Myers
Nuclear properties for astrophysical and radioactive-ion-beam applications (II)
NUCLEAR STRUCTURE Z=8-136; calculated the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one- and two-neutron separation energies, quantities related to β-delayed one- and two-neutron emission probabilities, average energy and average number of emitted neutrons, β-decay energy release and T1/2 with respect to Gamow-Teller decay with a phenomenological treatment of first-forbidden decays, one- and two-proton separation energies, and α-decay energy release and half-life.
doi: 10.1016/j.adt.2018.03.003
Phys.Rev. C 102, 034326 (2020)
E.M.Ney, J.Engel, T.Li, N.Schunck
Global description of β- decay with the axially deformed Skyrme finite-amplitude method: Extension to odd-mass and odd-odd nuclei
RADIOACTIVITY Z=20, A=50-61(β-); Z=21, A=50-66(β-); Z=22, A=52-73(β-); Z=23, A=53-74(β-); Z=24, A=56-79(β-); Z=25, A=57-80(β-); Z=26, A=60-83(β-); Z=27, A=62-88(β-); Z=28, A=68-93(β-); Z=29, A=68-96(β-); Z=30, A=74-99(β-); Z=31, A=74-102(β-); Z=32, A=80-103(β-); Z=33, A=80-110(β-); Z=34, A=84-113(β-); Z=35, A=84-116(β-); Z=36, A=88-117(β-); Z=37, A=88-120(β-); Z=38, A=90-121(β-); Z=39, A=90-124(β-); Z=40, A=97-125(β-); Z=41, A=96-128(β-); Z=42, A=102-135(β-); Z=43, A=102-138(β-); Z=44, A=106-143(β-); Z=45, A=106-146(β-); Z=46, A=112-147(β-); Z=47, A=112-150(β-); Z=48, A=118-157(β-); Z=49, A=124-160(β-); Z=50, A=128-163(β-); Z=51, A=128-168(β-); Z=52, A=134-171(β-); Z=53, A=134-176(β-); Z=54, A=138-179(β-); Z=55, A=138-182(β-); Z=56, A=140-183(β-); Z=57, A=141-184(β-); Z=58, A=144-185(β-); Z=59, A=146-186(β-); Z=60, A=152-187(β-); Z=61, A=152-188(β-); Z=62, A=156-189(β-); Z=63, A=156-192(β-); Z=64, A=162-207(β-); Z=65, A=162-210(β-); Z=66, A=166-213(β-); Z=67, A=167-218(β-); Z=68, A=172-221(β-); Z=69, A=172-224(β-); Z=70, A=180-227(β-); Z=71, A=180-228(β-); Z=72, A=184-233(β-); Z=73, A=185-238(β-); Z=74, A=190-241(β-); Z=75, A=191-248(β-); Z=76, A=194-255(β-); Z=77, A=195-256(β-); Z=78, A=202-261(β-); Z=79, A=202-262(β-); Z=80, A=206-265(β-); Z=81, A=210-266(β-); Z=82, A=212-267(β-); Z=83, A=214-268(β-); Z=84, A=220-269(β-); Z=85, A=220-270(β-); Z=86, A=224-271(β-); Z=87, A=225-272(β-); Z=88, A=230-273(β-); Z=89, A=231-274(β-); Z=90, A=236-275(β-); Z=91, A=237-278(β-); Z=92, A=242-281(β-); Z=93, A=242-302(β-); Z=94, A=246-305(β-); Z=95, A=247-308(β-); Z=96, A=252-309(β-); Z=97, A=254-314(β-); Z=98, A=260-315(β-); Z=99, A=260-318(β-); Z=100, A=268-323(β-); Z=101, A=268-326(β-); Z=102, A=274-329(β-); Z=103, A=274-332(β-); Z=104, A=282-335(β-); Z=105, A=282-336(β-); Z=106, A=286-339(β-); Z=107, A=290-340(β-); Z=108, A=292-345(β-); Z=109, A=294-348(β-); Z=110, A=300-369(β-); calculated asymptotic quantum numbers of the blocked proton or neutron quasiparticle, HFB binding energy, β2 deformation parameter, β- decay half-lives of 3983 neutron-rich nuclei, Q(β-), percent first-forbidden rate, QRPA energy and B(GT) Gamow-Teller strength for selected nuclei. Statistical extension of the charge-changing Finite-amplitude method (FAM), with a global Skyrme density functional. Comparison with experimental data, and with other theoretical calculations. Relevance to r process in nucleosynthesis.
doi: 10.1103/PhysRevC.102.034326
Nat.Phys. 17, 569 (2021)
I.V.Kortunov, S.Alighanbari, M.G.Hansen, G.S.Giri, V.I.Korobov, S.Schiller
Proton-electron mass ratio by high-resolution optical spectroscopy of ion ensembles in the resolved-carrier regime
ATOMIC MASSES 1H; measured transition frequencies; deduced proton-electron mass ratio by matching a precise ab initio calculation with the measured vibrational frequency.
doi: 10.1038/s41567-020-01150-7
Chin.Phys.C 45, 030003 (2021)
M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi
The AME 2020 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.