References quoted in the XUNDL dataset: 244MD 197AU(50TI,3N):NUC ID:XUNDL-2
4 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Lett. B 764, 265 (2017)
J.Konki, J.Khuyagbaatar, J.Uusitalo, P.T.Greenlees, K.Auranen, H.Badran, M.Block, R.Briselet, D.M.Cox, M.Dasgupta, A.Di Nitto, Ch.E.Dullmann, T.Grahn, K.Hauschild, A.Herzan, R.-D.Herzberg, F.P.Hessberger, D.J.Hinde, R.Julin, S.Juutinen, E.Jager, B.Kindler, J.Krier, M.Leino, B.Lommel, A.Lopez-Martens, D.H.Luong, M.Mallaburn, K.Nishio, J.Pakarinen, P.Papadakis, J.Partanen, P.Peura, P.Rahkila, K.Rezynkina, P.Ruotsalainen, M.Sandzelius, J.Saren, C.Scholey, J.Sorri, S.Stolze, B.Sulignano, Ch.Theisen, A.Ward, A.Yakushev, V.Yakusheva
Towards saturation of the electron-capture delayed fission probability: The new isotopes 240Es and 236Bk
RADIOACTIVITY 240Es(EC), (α), 236Bk(EC) [from 209Bi(34S, 3n)240Es, E=174, 178 MeV]; measured decay products, Eα, Iα; deduced T1/2, branching ratios, electron-capture delayed fission (ECDF) probability. Comparison with available data.
doi: 10.1016/j.physletb.2016.11.038
Nucl.Phys. A1002, 121958 (2020)
J.Khuyagbaatar
Spontaneous fission half-lives of the heaviest nuclei: Semi-empirical predictions
RADIOACTIVITY 246,248,250,252,254,256,258,260,262,264,266,268Cf, 248,250,252,254,256,258,260,262,264,266,268,270Fm, 250,252,254,256,258,260,262,264,266,268,270No, 252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288Rf, 254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290Sg, 254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292Hs, 252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300Ds, 254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302Cn, 256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304Fl, 284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322Lv, 286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324Og, 288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326120(SF); calculated T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.121958
Phys.Rev.Lett. 125, 142504 (2020)
J.Khuyagbaatar, H.M.Albers, M.Block, H.Brand, R.A.Cantemir, A.Di Nitto, C.E.Dullmann, M.Gotz, S.Gotz, F.P.Hessberger, E.Jager, B.Kindler, J.V.Kratz, J.Krier, N.Kurz, B.Lommel, L.Lens, A.Mistry, B.Schausten, J.Uusitalo, and A.Yakushev
Search for Electron-Capture Delayed Fission in the New Isotope 244Md
RADIOACTIVITY 244,245Md(α), (EC) [from 197Au(50Ti, X), E=239.8, 231.5 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, T1/2. Comparison with available data.
doi: 10.1103/PhysRevLett.125.142504
Phys.Rev.Lett. 124, 252502 (2020)
J.L.Pore, J.M.Gates, R.Orford, C.M.Campbell, R.M.Clark, H.L.Crawford, N.E.Esker, P.Fallon, J.A.Gooding, J.T.Kwarsick, A.O.Macchiavelli, C.Morse, D.Rudolph, A.Samark-Roth, C.Santamaria, R.S.Shah, M.A.Stoyer
Identification of the New Isotope 244Md
RADIOACTIVITY 244Md, 240Es, 236Bk(α) [from 209Bi(40Ar, 5n), E ∼ 200 MeV]; measured decay products, Eα, Iα; deduced α-decay energies, T1/2.
doi: 10.1103/PhysRevLett.124.252502