NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.Zou Found 28 matches. 2024ZH05 Phys.Rev. C 109, 014622 (2024) M.-H.Zhang, Y.-H.Zhang, Y.Zou, Ch.Wang, L.Zhu, F.-Sh.Zhang Predictions of synthesizing elements with Z=119 and 120 in fusion reactions
doi: 10.1103/PhysRevC.109.014622
2024ZO01 J.Phys.(London) G51, 045103 (2024) Y.-T.Zou, J.-H.Cheng, Y.-Y.Xu, Q.Xiao, S.-M.Liu, F.-Q.Shao, T.-P.Yu Laser-assisted two-proton radioactivity RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated the two-proton radioactivity assisted by an ultra-intense laser field within a deformed one-parameter model (OPM); deduced the lasers characterized by shorter wavelengths and higher intensities exert a more significant influence on the rate of the average change in pulse duration, T1/2.
doi: 10.1088/1361-6471/ad2691
2023ME14 New Journal of Physics 25, 093026 (2023) T.Meng, M.X.Ma, B.Tu, P.Ma, Y.W.Zhang, L.Liu, J.Xiao, K.Yao, Y.Zou, Y.Wu, J.G.Wang, B.Wei Study of single electron capture in O6+ + He collisions NUCLEAR REACTIONS He(O, X), E=2.63-37.5 keV/nucleon; measured reaction products; deduced the total and l-solved state-selective single EC σ. Comparison with calculations.
doi: 10.1088/1367-2630/acf1c3
2023XI06 J.Phys.(London) G50, 085102 (2023) Q.Xiao, J.-H.Cheng, B.-L.Wang, Y.-Y.Xu, Y.-T.Zou, T.-P.Yu Half-lives for proton emission and α decay within the deformed Gamow-like model RADIOACTIVITY 109I, 112,113Cs, 117La, 121Pr, 131Eu, 135Tb, 140,141Ho, 144,145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171Au, 176,177Tl, 185Bi, 111Cs, 127Pm, 137Tb(p), 106,108Te, 108,110,112Xe, 114Ba, 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156Yb, 156,158,160,162Hf, 174Hf, 158,160,162,164,166,168W, 180W, 162,164,166,168,170,172,174Os, 186Os, 168,170,172,174,176,178,180,182,184,186,188,190Pt, 170,172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 210Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210Ra, 214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230,232Th, 216,218,220,222,224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288,290Fl, 290,292Lv, 294Og, 105Te, 109Te, 109Xe, 147Sm, 149,151Gd, 151,153Dy, 153,155Er, 155Yb, 157,159Hf, 161,163W, 167W, 161Os, 167,169,171,173Os, 171,173,175,177,179,181,183,185Pt, 175,177,179,181,183,185Hg, 183,185,187,189Pb, 187,189,191,193,195,197,199,201,203,205,207,209,211,213,215,217,219Po, 193,195,197,199Rn, 203,205,207,209,211,213,215,217,219,221Rn, 201,203,205,207,209,211,213,215,217,219,221,223Ra, 211,213,215,217,219,221,223,225,227Th, 221,223,225,227,229,231,233,235U, 229,231,233,235,237,239,241Pu, 233Cm, 239,241,243,245,247Cm, 237Cf, 245,247,249,251,253Cf, 249,251,253,255,257Fm, 255,257,259No, 257Rf, 261Rf, 261Sg, 265Hs, 109I, 113I, 145Pm, 147Eu, 151Tb, 151,153Ho, 155,157Tm, 155Lu, 157,159Ta, 163,165Re, 167,169,171,173,175,177Ir, 173,175,177,179,181,183,185Au, 177,179,181Tl, 187,189,191,193,195Bi, 193,195,197,199,201,203,205,207,209,211,213,215,217,219,221,223,225,227Ac, 211,213,215,217,219,221,223,225,227,229,231Pa, 219Np, 223,225,227,229,231,233,235,237Np, 229Am, 235Am, 239,241,243Am, 243,245,247,249Bk, 247Es, 251,253Es, 249,251Md, 255,257Md, 253,255Lr, 259Lr, 259Db, 261Bh, 110,112I, 114Cs, 152,154Ho, 154,156Tm, 158Lu, 158Ta, 162Ta, 160,162Re, 168Re, 166,168Ir, 172,174Ir, 170Au, 176Au, 180Tl, 186Bi, 192,194Bi, 212,214Bi, 192At, 200,202,204,206,208,210,212,214,216,218At, 200Fr, 204,206,208,210,212,214,216,218,220Fr, 216,218,220,222,224,226Ac, 212Pa, 224Pa, 228,230Pa, 236Np, 236Am, 244Bk, 248Es, 258Md, 272Rg(α); calculated T1/2 with the deformed Gamow-like model, which introduces the effects of nucleus deformation; deduced the deformed model follows the Geiger-Nuttall law. Comparison with available data.
doi: 10.1088/1361-6471/acdfeb
2023ZO02 Astrophys.J.Suppl.Ser. 268, 56 (2023) Y.P.Zou, J.S.Zhang, C.Henkel, D.Romano, Y.H.Zheng, Y.T.Yen, J.L.Chen, Y.X.Wang, Y.Zhao A Systematic Observational Study on Galactic Interstellar Ratio 18O/17O. II. C18O and C17O J = 2-1 Data Analysis
doi: 10.3847/1538-4365/acee6b
2022PA24 Int.J.Mod.Phys. E31, 2250051 (2022) X.Pan, Y.-T.Zou, B.He, X.-H.Li, X.-J.Wu, Z.Zhang Systematic study of two-proton radioactivity half-lives using two-potential approach with different Skyrme interactions RADIOACTIVITY 19Mg, 45Fe, 48Ni, 54Zn, 67Kr, 15Ne, 17Na, 22Si, 24P, 26S, 28Cl, 29,30Ar, 31,32K, 33,34Ca, 35,37Sc, 37,38,39Ti, 39,40V, 41,42Cr, 43,44Mn, 47Co, 49Ni, 52Cu, 55Zn, 56,57,58Ga, 58,59Ge, 60,61,62As, 63,64Se, 65,66Br, 68Kr, 81Mo, 85Ru(2p); analyzed available data; calculated T1/2 using Skyrme energy density functional theory.
doi: 10.1142/S0218301322500513
2022RE08 Phys.Rev. A 106, 012805 (2022) B.Ren, P.Ma, Y.Zhang, L.Wei, J.Han, Z.Xia, J.Wang, T.Meng, W.Yu, Y.Zou, C.-L.Yang, B.Wei Dissociation mechanism of C2H42+ induced by 18-keV/u Ne8+ impact: Symmetric and isomeric cleavage of the C-C bond NUCLEAR REACTIONS C, H(Ne, X), E=18 keV/nucleon; measured reaction products; deduced kinetic-energy release (KER) distributions, C-C bond cleavage dissociation of ethylene dication. Comparison with calculations. The COLTRIMS setup at Fudan University.
doi: 10.1103/PhysRevA.106.012805
2022XU04 Eur.Phys.J. A 58, 16 (2022) Y.-Y.Xu, H.-M.Liu, D.-X.Zhu, X.Pan, Y.-T.Zou, X.-H.Li, P.-C.Chu An improved formula for the favored α decay half-lives RADIOACTIVITY 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156Yb, 156,158,160,162Hf, 174Hf, 158,160,162,164,166,168W, 180W, 162,164,166,168,170,172,174Os, 186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt, 170,172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 210Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 208,210,212,214,216,218,220,222,224,226,228,230,232Th, 218,220,222,224,226,228,230,232,234,236,238U, 230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 244,246Fm, 252,254,256No, 256,258Rf, 260Sg, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288Fl, 290,292Lv, 294Og, 105,107,109Te, 113I, 109,111Xe, 145Pm, 147Sm, 147Eu, 149,151Gd, 151,153Dy, 151,153Ho, 153,155Er, 153,155,157Tm, 155Yb, 155,157Lu, 157,159,161Hf, 157,159,161Ta, 159,161,163,165,167W, 159,161,163,165Re, 161,163,165,167,169,171,173Os, 165,167,169,171,173Ir, 177Ir, 165,167,169,171,173Pt, 177Pt, 181,183,185Pt, 171,173,175,177,179,181,183,185Au, 173,175Hg, 179Hg, 183Hg, 185Hg, 177,179,181Tl, 185,187,189,191Pb, 185,187,189,191,193,195,197Bi, 191,193,195,197,199,201Po, 205,207,209Po, 213,215,217,219Po, 187Po, 191,193,195,197,199,201,203,205,207,209,211,213,215,217,219At, 195,197,199,201,203,205,207,209Rn, 215,217Rn, 197,199,201,203,205,207,209,211,213,215,217,219Fr, 201,203,205Ra, 209,211Ra, 217Ra, 207,209,211,213,215,217,219,221Ac, 227Ac, 209,211,213Th, 219Th, 211,213,215,217,219,221,223,225,227,229,231Pa, 221U, 229U, 233U, 219Np, 223,225Np, 233Np, 231Pu, 235Pu, 239Pu, 233Cm, 239,241Cf, 245Cf, 253Cf, 241,243,245,247Es, 251,253,255Es, 241Fm, 247Fm, 251No, 253,255Lr, 259Lr, 261Rf, 257Db, 263Sg, 263,265Hs, 267Ds, 148Eu, 152,154Ho, 154,156Tm, 156,158Lu, 158Ta, 162,164Re, 164,166,168,170,172Ir, 170,172,174,176,178Au, 184Au, 188Bi, 196Bi, 192,194,196,198,200,202At, 214,216At, 256,258,260Rf, 260Sg, 262,264Hs, 268,270,272Hs, 266Ds, 270Ds, 276,278Ds, 270Cn, 280,282Cn, 284,286,288Fl, 288,290,292,294,296Lv, 294,296,298,300,302,304Og, 296,298,300,302,304,306,308120, 302,304,306,308,310,312122, 308,310,312,314,316,318124, 314,316,318,320,322,324,326126, 320,322,324,326,328,330,332128(α); calculated T1/2 using the modified Hatsukawa formula. Comparison with available data.
doi: 10.1140/epja/s10050-022-00666-1
2022XU13 Chin.Phys.C 46, 114103 (2022) Y.-Y.Xu, D.-X.Zhu, Y.-T.Zou, X.-J.Wu, B.He, X.-H.Li Systematic study on α-decay half-lives of uranium isotopes with a screened electrostatic barrier RADIOACTIVITY 216,217,218U, 221U, 222,223,224,225,226,227,228U, 229U, 230,231,232U, 233U, 234,235,236,237,238,239,240,241,242,243U(α); calculated T1/2 using the Gamow model with a screened electrostatic barrier. Comparison with available data.
doi: 10.1088/1674-1137/ac7fe8
2022ZH39 Chin.Phys.C 46, 044106 (2022) D.-X.Zhu, H.-M.Liu, Y.-Y.Xu, Y.-T.Zou, X.-J.Wu, P.-C.Chu, X.-H.Li Two-proton radioactivity within Coulomb and proximity potential model RADIOACTIVITY 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated T1/2 using the Coulomb and proximity potential model (CPPM). Comparison with available data.
doi: 10.1088/1674-1137/ac45ef
2021LI16 Chin.Phys.C 45, 024108 (2021) H.-M.Liu, Y.-T.Zou, X.Pan, J.-L.Chen, B.He, X.-H.Li New Geiger-Nuttall law for two-proton radioactivity RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr, 22Si, 26S, 34Ca, 36Sc, 38,39Ti, 40V, 42Cr, 47Co, 49Ni, 56Ga, 58,59,60Ge, 61As, 10N, 28Cl, 32K, 57Ga, 62As, 52Cu, 60As(2p); calculated T1/2 using GLDM, ELDM, the four-parameter empirical formula. Comparison with experimental data.
doi: 10.1088/1674-1137/abd01e
2021LI45 Int.J.Mod.Phys. E30, 2150074 (2021) H.-M.Liu, Y.-T.Zou, X.Pan, B.He, X.-H.Li Systematic study of two-proton radioactivity half-lives based on a modified Gamow-like model RADIOACTIVITY 19Mg, 45Fe, 48Ni, 54Zn, 67Kr, 22Si, 26S, 34Ca, 36Sc, 38,39Ti, 40V, 42Cr, 47Co, 49Ni, 58Ga, 58,59Ge, 61As, 10N, 28Cl, 32K, 57Ga, 62As, 52Cu, 60As(2p); calculated T1/2; deduced T1/2 and Q-values reaction. Comparison with available data.
doi: 10.1142/S0218301321500749
2021LI67 Phys.Scr. 96, 12522 (2021) H.-M.Liu, Y.-T.Zou, X.Pan, X.-H.Li, X.-J.Wu, B.He Systematic study of cluster radioactivity half-lives based on a modified Gamow-like model RADIOACTIVITY 222,224,226Ra(14C), 230,232,234U(24Ne), 234,236U, 236,238Pu(28Mg), 221Fr, 221,223Ra, 225Ac(14C), 231Pa, 233,235U(24Ne), 233,235U(25Ne); calculated T1/2. Comparison with available data.
doi: 10.1088/1402-4896/ac3dbc
2021RE10 Phys.Rev. A 104, 022811 (2021) B.Ren, Z.Xia, Y.Zhang, L.Wei, W.Yu, J.Han, B.Wang, Y.Zou, L.Chen, B.Wei Three-body fragmentation mechanism of C2H43+ produced by 18 - keV/uNe8+ impact NUCLEAR REACTIONS C, H(Ne, X), E=18 keV/nucleon; measured reaction products, TOF; deduced Dalitz plot of fragmentation channels. COLTRIMS technique.
doi: 10.1103/PhysRevA.104.022811
2021ZO01 Chin.Phys.C 45, 104101 (2021) Y.-T.Zou, X.Pan, X.-H.Li, H.-M.Liu, X.-J.Wu, B.He Systematic study of two-proton radioactivity with a screened electrostatic barrier RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); analyzed available data; calculated T1/2 using five different theoretical models and/or formulas.
doi: 10.1088/1674-1137/ac1b96
2021ZO02 Phys.Scr. 96, 075301 (2021) Y.-T.Zou, X.Pan, H.-M.Liu, X.-J.Wu, B.He, X.-H.Li Systematic studies on a decay half-lives of neptunium isotopes RADIOACTIVITY 219,223,224,225,233,221,222,229,231,235,237,239,220,226,227,228,232,236Np(α); calculated T1/2. Comparison with available data.
doi: 10.1088/1402-4896/abf795
2020CH43 Eur.Phys.J. A 56, 273 (2020) J.-H.Cheng, X.Pan, Y.-T.Zou, X.-H.Li, Z.Zhang, P.-C.Chu Systematic study of proton radioactivity of spherical proton emitters with Skyrme interactions RADIOACTIVITY 144,145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171Au, 176,177Tl(p); calculated T1/2. Comparison with experimental data.
doi: 10.1140/epja/s10050-020-00280-z
2020LI27 Chin.Phys.C 44, 094106 (2020) H.-M.Liu, Y.-T.Zou, X.Pan, X.-J.Bao, X.-H.Li Systematic study of the α decay preformation factors of the nuclei around the Z = 82, N = 126 shell closures within the generalized liquid drop model RADIOACTIVITY 186,188,190,192,194Po, 196,198,200,202,204,206,208Po, 200,202,204,206,208,210,212Rn, 204Ra, 208Ra, 212Th, 214Th, 216U, 178,180Pb, 184,186,188,190,192,194Pb, 210Pb, 212,214,216,218Po, 214,216,218,220Rn, 216Ra, 218Ra, 216,218,220Th, 218U, 195,197,199,201,203,205,207Po, 197,199,201,203,205,207,209,211At, 195,197Rn, 203Rn, 207,209Rn, 199,201,203,205,207,209,211,213Fr, 203Ra, 209Ra, 205,207Ac, 211Ac, 213,215Pa, 177,179Tl, 213,215Po, 219Po, 213,215,217,219At, 215,217Rn, 215,217,219Fr, 217Ra, 215,217Ac, 219Th, 219Pa, 221Pa, 221U, 209Bi, 189Po, 203Po, 205,207,209,211,213Ra, 215Th, 187,189Pb, 213Bi, 213Rn, 219,221Rn, 215Ra, 219Ra, 217Th, 192At, 200,202,204,206,208At, 200Fr, 204,206,208Fr, 206Ac, 214,216,218At, 216,218Fr, 218Ac, 220Pa, 186Bi, 190,192,194Bi, 210At, 210,212Fr, 212Pa, 210,212,214Bi, 212At, 214Fr, 216Ac(α); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/44/9/094106
2018LI37 At.Data Nucl.Data Tables 123-124, 86 (2018) M.C.Li, X.L.Guo, K.Wang, R.Si, C.Y.Zhang, C.Y.Chen, Y.M.Zou, R.Hutton High-accuracy multi-configuration Dirac-Hartree-Fock calculations of the energy levels and transition properties of Ga-like to Br-like gadolinium ions ATOMIC PHYSICS Gd; calculated excitation energies, lifetimes, wavelengths, E1, E2, E3, M1 and M2 line strenghs, transition rates, oscillator strengths using fully relativistic multi-configuration Dirac-Hartree-Fock method.
doi: 10.1016/j.adt.2017.11.001
2016GU04 Phys.Rev. A 93, 012513 (2016) X.L.Guo, R.Si, S.Li, M.Huang, R.Hutton, Y.S.Wang, C.Y.Chen, Y.M.Zou, K.Wang, J.Yan, C.Y.Li, T.Brage Calculations with spectroscopic accuracy for the ground configuration (3d9) forbidden transition in Co-like ions ATOMIC PHYSICS Z=28-100; calculated fine-structure energy splitting and transition rates. Multiconfiguration Dirac-Hartree-Fock (MCDHF) theory and the relativistic many-body-perturbation theory (RMBPT).
doi: 10.1103/PhysRevA.93.012513
2007LI70 Phys.Rev. A 76, 062503 (2007) Atomic structure of the super-heavy element No I (Z=102) ATOMIC PHYSICS Z=102, 80; calculated level energies using multiconfiguration Dirac-Fock method.
doi: 10.1103/PhysRevA.76.062503
1995ZO03 Nucl.Instrum.Methods Phys.Res. B99, 1 (1995) Y.Zou, Y.Awaya, C.P.Bhalla, T.Kambara, Y.Kanai, M.Oura, Y.Nakai, K.Ando, A.Hitachi, S.Kravis L-Subshell Vacancy Production of Fast Argon Ions in Solids NUCLEAR REACTIONS C, Mg, 27Al, 59Co, Ni, Zn, 87Y, 93Nb, Mo, Sn, Nd, Tb, Ho, Ta, W, Ti, V, Cr, Fe, Cu(Ar, X), E=43-95 MeV; measured Kα satellite, hypersatellite X-ray yields. Model comparison. ATOMIC PHYSICS C, Mg, 27Al, 59Co, Ni, Zn, 87Y, 93Nb, Mo, Sn, Nd, Tb, Ho, Ta, W, Ti, V, Cr, Fe, Cu(Ar, X), E=43-95 MeV; measured Kα satellite, hypersatellite X-ray yields. Model comparison.
doi: 10.1016/0168-583X(94)00704-7
1994GU06 Phys.Rev.Lett. 72, 3000 (1994) P.Gu, P.Haas, W.P.Hogan, S.K.Kim, J.N.Matthews, S.S.Myung, S.Schnetzer, G.B.Thomson, Y.Zou, K.Arisaka, D.Roberts, W.Slater, M.Weaver, R.A.Briere, E.Cheu, D.A.Harris, K.S.McFarland, A.Roodman, B.Schwingenheuer, S.V.Somalwar, Y.W.Wah, B.Winstein, R.Winston, A.R.Barker, E.C.Swallow, G.J.Bock, R.Coleman, M.Crisler, J.Enagonio, R.Ford, Y.B.Hsiung, D.A.Jensen, E.Ramberg, R.Tschirhart, E.M.Collins, G.D.Gollin, T.Nakaya, T.Yamanaka Measurement of the Branching Ratio and a Study of CP for the Leptonic Decay K(L) → e+e-e+e-
doi: 10.1103/PhysRevLett.72.3000
1994RA25 Phys.Lett. 338B, 403 (1994) E.J.Ramberg, G.J.Bock, R.Coleman, M.Crisler, J.Enagonio, R.Ford, Y.B.Hsiung, D.A.Jensen, R.Tschirhart, K.Arisaka, D.Roberts, W.Slater, M.Weaver, R.A.Briere, E.Cheu, D.A.Harris, P.Krolak, G.Makoff, K.S.McFarland, A.Roodman, B.Schwingenheuer, S.Somalwar, Y.W.Wah, B.Winstein, R.Winston, A.R.Barker, E.C.Swallow, E.M.Collins, G.D.Gollin, T.Nakaya, T.Yamanaka, P.Gu, P.Haas, W.P.Hogan, S.Kim, J.N.Matthews, S.S.Myung, S.Schnetzer, G.Thomson, Y.Zou Polarization of (Lambda) and (Lambda-bar) Produced by 800-GeV Protons NUCLEAR REACTIONS 9Be(p, X), E=800 GeV; measured lambda, lambda-bar hyperon polarization; deduced no lambda-bar polarization evidence.
doi: 10.1016/0370-2693(94)91397-8
1989LI25 Chin.J.Nucl.Phys. 11, No.1, 19 (1989) J.Li, S.Wang, D.Xie, G.Ma, Y.Zou, S.Chen Small Angle Elastic Scattering and Total Elastic Scattering Cross Section of 14.2 MeV Neutrons NUCLEAR REACTIONS 27Al, Ti, Fe, Cu, Cd(n, n), E=14.2 MeV; measured σ(θ); deduced σ. Pb, 209Bi, 238U(n, X), E=14.2 MeV; calculated σ.
1988LI14 Chin.J.Nucl.Phys. 10, 46 (1988) Li Jingde, Wang Shiming, Xie Daquan, Ma Gonggui, Zou Yiming, Chen Shuying Small Angle Elastic Scattering and Total Elastic Scattering Cross Sections of Fast Neutrons NUCLEAR REACTIONS 27Al, Ti, Fe, Cu, Cd(n, n), E=14.2 MeV; measured σ(θ), σ. Data for Pb, 209Bi, 238U analyzed. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30762. 1987LI21 Chin.J.Nucl.Phys. 9, 97 (1987) Li Jingde, Ma Gonggui, Xie Daquan, Zou Yiming, Wang Shiming, Chen Shuying Small-Angle Elastic Scattering of 14.2 MeV Neutrons by Heavy Nuclei NUCLEAR REACTIONS W, Pb, 209Bi(n, n), E=14.2 MeV; measured σ(θ). Tof. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30762. 1986LI25 Chin.J.Nucl.Phys. 8, 245 (1986) Li Jingde, Xie Daquan, Ma Gonggui, Zou Yiming, Wang Shiming, Chen Shuying Small Angle Elastic Scattering of 14.2 MeV Neutrons by 238U NUCLEAR REACTIONS 238U(n, n), E=14.2 MeV; measured σ(θ), θ=1.7°-15°. Tof. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30762. Back to query form Note: The following list of authors and aliases matches the search parameter Y.Zou: , Y.M.ZOU, Y.P.ZOU, Y.T.ZOU |