References quoted in the XUNDL dataset: 152SM 152EU EC DECAY:13.5 Y:XUNDL-10
6 references found.
Clicking on a keynumber will list datasets that reference the given article.
Nucl.Instrum.Methods Phys.Res. A271, 507 (1988)
W.Karle, M.Knopp, K.-H.Speidel
Applications of Large Barium Fluoride Scintillators to In-Beam Gamma-Ray Spectroscopy
RADIOACTIVITY 152Eu(β-), (β+), (EC); measured γγ(t). 152Sm level deduced T1/2. Large volume BaF2 scintillators.
NUCLEAR REACTIONS 40Ca(α, α'), E=13.62 MeV; measured γα-coin. 40Ca level deduced T1/2. Large volume BaF2 scintillators.
doi: 10.1016/0168-9002(88)90312-9
J.Instrum. 6, 08008 (2011)
D.S.Cross, G.C.Ball, P.E.Garrett, S.Triambak, S.J.Williams, C.Andreoiu, R.Churchman, A.B.Garnsworthy, G.Hackman, J.R.Leslie, J.N.Orce, C.S.Sumithrarachchi, C.E.Svensson
Commissioning the DANTE array of BaF2 detectors at TRIUMF-ISAC using a fast-timing lifetime measurement
RADIOACTIVITY 152Eu(EC); measured decay products, Eγ, Iγ; deduced 152Sm first excited state T1/2. Comparison with available data.
doi: 10.1088/1748-0221/6/08/p08008
Phys.Rev. C 84, 034613 (2011)
J.Randrup, P.Moller, A.J.Sierk
Fission-fragment mass distributions from strongly damped shape evolution
NUCLEAR REACTIONS 239Pu(n, F)240Pu, E=8-14 MeV; 234,236U(n, F)235U/236U, E=8-14 MeV; 234U(γ, F)234U, E=8-14 MeV; 222,224,226,228Th(γ, F)222Th/224Th/226Th/228Th, E=8-14 MeV; calculated fission fragment mass and charge yields, comparison with experimental data. Random walks on a five-dimensional potential energy surface within the framework of the Smoluchowski equation of motion.
NUCLEAR STRUCTURE 222,224,226,228Th, 240Pu; calculated fission fragment mass and charge distributions. 222Th; calculated contours of three shapes relevant to fission, and the most probable symmetric fragment division in 111Rh isotope.
doi: 10.1103/PhysRevC.84.034613
Phys.Rev. C 89, 021302 (2014)
C.Plaisir, L.Gaudefroy, V.Meot, A.Blanc, J.M.Daugas, O.Roig, N.Arnal, T.Bonnet, F.Gobet, F.Hannachi, M.Tarisien, M.Versteegen, T.Roger, M.Rejmund, A.Navin, C.Schmitt, G.Fremont, J.Goupil, J.Pancin, C.Spitaels, M.Zielinska
In-flight fast-timing measurements in 152Sm
NUCLEAR REACTIONS 152Sm(136Xe, 152Sm'), E=5.09 MeV/nucleon; measured time-of-flight of recoiling nuclei using VAMOS spectrometer, Eγ, Iγ, γγ-coin level half-lives by in-flight fast-timing (IFFT) technique using LaBr3 detectors at GANIL facility. Coulomb excitation. 152Sm; deduced levels, J, π, transition quadrupole moments from level half-lives of ground-state band members. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.89.021302
At.Data Nucl.Data Tables 107, 1 (2016), Erratum At.Data Nucl.Data Tables 114, 371 (2017)
B.Pritychenko, M.Birch, B.Singh, M.Horoi
Tables of E2 transition probabilities from the first 2+ states in even-even nuclei
COMPILATION 4,6,8,10He, 6,8,10,12,14Be, 10,12,14,16,18,20C, 12,14,16,18,20,22,24,26O, 16,18,20,22,24,26,28,30,32Ne, 20,22,24,26,28,30,32,34,36,38Mg, 24,26,28,30,32,34,36,38,40,42Si, 28,30,32,34,36,38,40,42,44,46S, 32,34,36,38,40,42,44,46,48Ar, 36,38,40,42,44,46,48,50,52,54Ca, 42,44,46,48,50,52,54,56,58Ti, 46,48,50,52,54,56,58,60,62,64Cr, 48,50,52,54,56,58,60,62,64,66,68Fe, 52,54,56,58,60,62,64,66,68,70,72,74,76Ni, 60,62,64,66,68,70,72,74,76,78,80Zn, 62,64,66,68,70,72,74,76,78,80,82,84,86Ge, 66,68,70,72,74,76,78,80,82,84,86Se, 72,74,76,78,80,82,84,86,88,90,92,94,96Kr, 76,78,80,82,84,86,88,90,92,94,96,98,100,102Sr, 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108Zr, 84,86,88,90,92,94,96,98,100,102,104,106,108,110Mo, 88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118Ru, 92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128Pd, 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Cd, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138Te, 110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144Xe, 118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148Ba, 122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152Ce, 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156Nd, 130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160Sm, 138,140,142,144,146,148,150,152,154,156,158,160,162,164Gd, 140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170Dy, 144Er, 148,150,152,154,156,158,160,162,164,166,168,170,172,174Er, 152,154,156,158,160,162,164,166,168,170,172,174,176,178Yb, 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192W, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Os, 168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204Pt, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210Hg, 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226,228,230,232Ra, 214,216,218,220,222,224,226,228,230,232,234,236Th, 226,228,230,232,234,236,238,240,242U, 236,238,240,242,244,246Pu, 238,240,242,244,246,248,250Cm, 244,246,248,250,252Cf, 246,248Fm, 252,254,256Fm, 252,254No, 256Rf; compiled evaluated B(E2) values, T1/2, deformation parameters, first 2+ state energies in even-even nuclei.
NUCLEAR STRUCTURE 6He, 10,12Be, 10,12,14,16,18,20C, 16,18,20,22O, 18,20,22,24,26,28,30Ne, 20,22,24,26,28,30,32,34Mg, 24,26,28,30,32,34,36,38,40Si, 30,32,34,36,38,40,42,44S, 32,34,36,38,40,42,44,46Ar, 38,40,42Ca, 46,48,50Ca, 42,44,46,48,50,52,54,56Ti, 46,48,50,52,54,56,58,60,62Cr, 50,52,54,56,58,60,62,64,66Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 62,64,66,68,70,72,74,76,78Zn, 104,106Sn; calculated transition energies, B(E2). Nuclear shell model.
doi: 10.1016/j.adt.2015.10.001
Chin.Phys.C 41, 030003 (2017)
M.Wang, G.Audi, F.G.Kondev, W.J.Huang, S.Naimi, X.Xu
The AME2016 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses data.
doi: 10.1088/1674-1137/41/3/030003