NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Deng Found 68 matches. 2024CH08 Phys.Lett. B 848, 138322 (2024) J.-H.Cheng, W.-Y.Zhang, Q.Xiao, J.-G.Deng, T.-P.Yu Determinants in laser-assisted deformed α decay NUCLEAR STRUCTURE A=100-300; analyzed available data; deduced degree of agreement between theoretical T1/2 and experimental data, rate of the change of penetration probability and the rate of the change of α decay half-life for different parent nuclei have different sensitivity to the high-intensity laser, rate of the relative change of penetration probability versus the Coulomb-Sommerfeld parameter.
doi: 10.1016/j.physletb.2023.138322
2022DE15 Chin.Phys.C 46, 061001 (2022) J.-G.Deng, H.-F.Zhang, X.-D.Sun New behaviors of α-particle preformation factors near doubly magic 100Sn RADIOACTIVITY 104,106,108,110Te, 108,110,112Xe, 114Ba, 212,214,216,218Po, 212,214,216,218,220,222Rn, 214,216,218,220,222,224,226Ra(α); calculated T1/2 within the generalized liquid drop model. Comparison with available data.
doi: 10.1088/1674-1137/ac5a9f
2022DE22 Eur.Phys.J. A 58, 165 (2022) Probing the robustness of N = 126 shell closure via the α decay systematics RADIOACTIVITY 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, 214,216,218,220,222,224,226,228,230,232,234,236,238U(α); calculated T1/2 within the generalized liquid drop model (GLDM); deduced α-particle preformation factors. Comparison with experimental data.
doi: 10.1140/epja/s10050-022-00813-8
2021CH48 Phys.Rev. C 104, 034901 (2021) J.Chen, J.Deng, Z.Tang, Z.Xu, L.Yi Nonequilibrium kinetic freeze-out properties in relativistic heavy ion collisions from energies employed at the RHIC beam energy scan to those available at the LHC NUCLEAR REACTIONS Au(Au, X), E=7.7, 11.5, 19.6, 27, 39, 62.4, 200 GeV; Pb(Pb, X), E=2.76, 5.02 TeV; analyzed experimental data for transverse momentum spectra of the identified hadrons from STAR and PHENIX collaborations at RHIC, BNL, and from ALICE collaboration at LHC, CERN using Boltzmann-Gibbs blast-wave (BGBW) and Tsallis blastwave (TBW) fits; deduced kinetic freeze-out parameters in heavy ion collisions of different centralities for charged pions, kaons, and protons, including strange and multistrange particles.
doi: 10.1103/PhysRevC.104.034901
2021DE07 Chin.Phys.C 45, 024104 (2021) Systematic study of α decay half-lives within the Generalized Liquid Drop Model with various versions of proximity energies RADIOACTIVITY 148Gd, 150,154Dy, 154Er, 154,158Yb, 158,162Hf, 160,164,168W, 162,168,172,186Os, 168,174,178,182,190Pt, 174,178,182,186Hg, 180,186,190Pb, 186,194,198,202,206,212,216Po, 194,200,204,208,212,216,220Rn, 202,208,216,220,224Ra, 208,214,218,222,226,230Th, 218,224,230,234U, 228,232,236,240,244Pu, 236,240,244,248,252Cf, 244,252,256Fm, 256No, 256,260Rf, 264,270Hs, 286Fl, 290Lv, 294Og(α); calculated T1/2.
doi: 10.1088/1674-1137/abcc5a
2020CH12 Nucl.Phys. A997, 121717(2020) J.-Ha.Cheng, J.-L.Chen, J.-G.Deng, X.-H.Li, Z.Zhang, P.-C.Chu Systematic study of proton emission half-lives within the two-potential approach with Skyrme-Hartree-Fock
doi: 10.1016/j.nuclphysa.2020.121717
2020DE08 Phys.Rev. C 101, 034307 (2020) J.-G.Deng, H.-F.Zhang, G.Royer Improved empirical formula for α-decay half-lives RADIOACTIVITY A=146-294, Z=62-118(α); calculated α-decay half-lives for even-even nuclei; A=147-285, Z=62-112(α); calculated α-decay half-lives of even Z-odd N nuclei; A=145-261, Z=61-107(α); calculated α-decay half-lives of odd Z-even N nuclei; A=148-256, Z=63-101(α); calculated α-decay half-lives for odd-odd nuclei, in all cases isomers included. 279,281,283,285,287,289,291,293,295,297,299,301,303,305,307,309,311,313,315,317Ts, 281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318Og, 285,287,289,291,293,295,297,299,301,303,305,307,309,311,313,315,317,319119, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320120(α); calculated Qα, half-lives. Improved Royer formulas and WS3+ mass model. Comparison with available experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.101.034307
2020DE37 Phys.Rev. C 102, 044314 (2020) Analytic formula for estimating the α-particle preformation factor RADIOACTIVITY 148Eu, 148,150Gd, 149,151Tb, 150,151,152,153,154Dy, 151,151m,152,152m,153m,154Ho, 152,153,154,155,156Er, 153,153m,154,154m,155,156Tm, 154,155,156,157,158Yb, 155,155m,156m,157mLu, 156,157,158,160,162Hf, 157m,158,158m,159,159mTa, 158,159,160,161,162,163,164,166,168,180W, 159m,160,161m,162,162m,163,163m,164m,165,165m,167m,169,169mRe, 161,162,163,165,166,167,168,169,170,172,174,186Os, 164m,165m,166,166m,167,167m,168,168m,169,169m,170,170m,171,171m,172,172m,173m,174,174m,175,177Ir, 166,167,168,171,172,173,174,175,176,177,178,179,180,181,182,183,184,190Pt, 170,170m,171m,173,173m,175,175m,176,177,177m,179,181,183,185,186Au, 171,172,173,174,176,177,178,179,180,181,182,183,184,185,186Hg, 177,177m,179,179m,180,181m,183,183m,186m,187mTl, 178,179,180,183m,184,185m,186,187,187m,188,189,190,191m,192Pb, 186,186m,187,187m,189,190,190m,191,191m,192,192m,193,193m,194,194m,195,195m,196,196m,209,211,212,213,214Bi, 186,187,189,190,194,195,195m,196,197,197m,198,199,199m,200,201,201m,202,203,203m,204,205,206,207,208,209,211m,212,213,214,215,216,218,219Po, 191,191m,192,192m,193,193m,194,194m,195,197,197m,199,199m,200,200m,201,202,202m,203,204,205,206,207,208,209,210,211,212,213,215,217,218,219,220At(α); calculated T1/2 and α-preformation factors using an analytical formula as a bridge between the α-decay energy and α-particle preformation factor for even-even, odd-A and odd-odd α emitters. Comparison with experimental half-lives. RADIOACTIVITY 193,194,195,195m,196,197,197m,200,202,203,203m,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223Rn, 197,199,199m,200m,201,201m,203,203m,205,207,209,211,212,213,214,215,218,218m,219,220,221,223Fr, 201,201m,202,203,203m,204,207,208,209,213,214,215,216,217,218,219,220,221,222,223,224,226Ra, 205,207,211,215,216,216m,217,217m,218,219,221,222,223,225,226,227Ac, 208,209m,212,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231Th, 213,215,217,220,221,223,224,227,228,229,230Pa, 216,218,219,221,222,224,225,226,227,229,230,231,232,233,234,236U, 227,229,231,235,237,239Np, 228,230,231,232,233,234,235,236,238,239,240,241,242,244Pu, 229,233,235,237,239,241,242m,243Am, 233,234,236,237,238,240,241,242,243,244,245,246,248Cm, 247Bk, 238,240,241,242,243,244,245,246,247,248,250,251,252,254Cf, 245,246,247,248,249,252,253,254m,255Es, 243,244,247,247m,248,252,253,254,256,257Fm, 247,247m,251,256m,258Md, 251,251m,253,254,255,256,258,259No, 253,253m,255,257,259Lr, 255,256,257m,258,259,260,261,263Rf, 259Db, 259,259m,260,261,263Sg, 261Bh, 264,265,268,269,270Hs, 267,269,270,271,271m,273,277Ds, 277,281Cn, 286,288,289Fl, 290,292Lv, 294Og(α); calculated T1/2 and α-preformation factors using an analytical formula as a bridge between the α-decay energy and α-particle preformation factor for even-even, odd-A and odd-odd α emitters. Comparison with experimental half-lives.
doi: 10.1103/PhysRevC.102.044314
2019CH27 Nucl.Phys. A987, 350 (2019) J.-H.Cheng, J.-L.Chen, J.G.Deng, X.-J.Wu, X.-H.Li, P.-C.Chu Systematic study of α decay half-lives based on Gamow-like model with a screened electrostatic barrier RADIOACTIVITY Z>51(α); calculated even-even nuclei T1/2 using modified Gamow-like model including centrifugal potential and electrostatic shielding with two parameters, radius constant r0 and a parameter for the screened electrostatic potential; Z=120; calculated T1/2 for 7 even-even nuclei and for some of their not yet synthesized α-decay chain. Halflives compared with those calculated using different approaches and with available data.
doi: 10.1016/j.nuclphysa.2019.05.002
2019CH41 J.Phys.(London) G46, 065107 (2019) J.-L.Chen, X.-H.Li, J.-H.Cheng, J.-G.Deng, X.-J.Wu Systematic study of proton radioactivity based on Gamow-like model with a screened electrostatic barrier RADIOACTIVITY 105Sb, 109I, 112,113Cs, 121Pr, 130,131Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171Au, 176,177Tl, 185Bi(p); calculated T1/2. Comparison with experimental data.
doi: 10.1088/1361-6471/ab1a56
2019CH45 Eur.Phys.J. A 55, 214 (2019) J.-L.Chen, J.-Y.Xu, J.-G.Deng, X.-H.Li, B.He, P.-C.Chu New Geiger-Nuttall law for proton radioactivity
doi: 10.1140/epja/i2019-12927-7
2019DE17 Eur.Phys.J. A 55, 58 (2019) J.-G.Deng, X.-H.Li, J.L.Chen, J.-H.Cheng, X.-J.Wu Systematic study of proton radioactivity of spherical proton emitters within various versions of proximity potential formalisms RADIOACTIVITY 145,146,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 165,166,167Ir, 170,171Au, 176,177Tl, 185Bi(p); calculated proton radioactivity T1/2; compared with published calculations using different proximity potentials and with data.
doi: 10.1140/epja/i2019-12728-0
2019LI58 Int.J.Mod.Phys. E28, 1950089 (2019) H.-M.Liu, J.-Y.Xu, J.-G.Deng, B.He, X.-H.Li Predictions of α decay half-lives for even-even superheavy nuclei with 104≤ Z ≤ 128 based on two-potential approach within cluster-formation model RADIOACTIVITY 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156,158Yb, 156,158,160,162,164,166,168,170,172,174Hf, 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, 172,174,176,178,180,182,184,186,188Hg, 180Pb, 184,186,188,190,192,194Pb, 210Pb, 190Po, 194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196Rn, 200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204Ra, 208Ra, 214,216,218,220,222,224,226Ra, 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, 234,236,238,240,242,244,246,248,250Cm, 238,240,242,244,246,248,250,252,254,256Cf, 244Fm, 248Fm, 252,254,256Fm, 254,256,258No, 256,258,260Rf, 260Sg, 264Hs, 268,270Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α); calculated T1/2. Comparison with available data.
doi: 10.1142/S0218301319500897
2018DE14 Chin.Phys.C 42, 044102 (2018) J.-G.Deng, J.-C.Zhao, J.-L.Chen, X.-J.Wu, X.-H.Li α decay properties of 296Og within the two-potential approach RADIOACTIVITY 250,252,254,256Cf, 254,256Fm, 256,258No, 258,260Rf, 260Sg, 264,268,270Hs, 270Ds, 294,296Og, 290,292Lv, 286,288Fl(α); calculated T1/2. Comparison with experimental data.
doi: 10.1088/1674-1137/42/4/044102
2018DE17 Phys.Rev. C 97, 044322 (2018) J.-G.Deng, J.-C.Zhao, P.-C.Chu, X.-H.Li Systematic study of α decay of nuclei around the Z=82, N=126 shell closures within the cluster-formation model and proximity potential 1977 formalism RADIOACTIVITY 189,190,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,210,212,213,214,215,216,218,219Po, 194,195,196,197,200,202,203,204,205,206,207,208,209,210,212,213,214,215,216,217,218,219,220,221,222Rn, 202,203,204,207,208,209,213,214,215,216,217,218,219,220Ra, 212,214,215,216,217,218,219,220,221Th, 216,217,218,221,222U, 186,188Hg, 187,188,189,190,191,192,194,210Pb, 190,192,194,209,210,212,213,214Bi, 192,197,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,223At, 199,200,201,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221Fr, 212,213,214,215,217,219,220,221,222Pa, 205,206,207,211,215,216,217,218,219,220Ac(α); calculated α-decay preformation factors using cluster-formation model (CFM) and T1/2 using proximity potential 1977 formalism (Prox.1977). Comparison with experimental data.
doi: 10.1103/PhysRevC.97.044322
2017DE21 Phys.Rev. C 96, 024318 (2017) J.-G.Deng, J.-C.Zhao, D.Xiang, X.-H.Li Systematic study of unfavored α-decay half-lives of closed-shell nuclei related to ground and isomeric states RADIOACTIVITY 154mHo, 161,163Hf, 165W, 168Re, 171Os, 170m,171m,172,173m,175Ir, 175,179Pt, 177,181Hg, 179,181Au, 180,181mTl, 187,189Pb, 190,192,192m,194m,209,212m,213,214Bi, 189,203,211,211mPo, 191m,193m,210,212At, 193,205,211,213,219,221Rn, 210,212,214,220Fr, 207,213,215,219Ra, 214,216,216mAc, 215,217Th, 224Pa(α), 219U(α); calculated Q(α), half-lives, α-preformation probabilities for unfavored α decays of closed-shell nuclei related to ground and isomeric states around Z=82, N=82 and 126 closed shells. Two-potential approach for the valence nucleon (hole) and isospin asymmetry of the parent nuclei; deduced linear dependence on NpNn or NpNnI. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.024318
2017DE37 Chin.Phys.C 41, 124109 (2017) J.-G.Deng, J.-H.Cheng, B.Zheng, X.-H.Li α decay properties of 297Og within the two-potential approach RADIOACTIVITY 251,253,255Cf, 253,255Es, 253,257Fm, 255,257,259Md, 255,259No, 257,259Lr, 257,259,261,263Rf, 259Db, 259,261,263,265,271Sg, 261,271Bh, 265,267,269,273,275Hs, 275Mt, 267,269,271,273,277,279,281Ds, 279Rg, 277,281,285Cn, 283,285Nh, 285,287,289Fl, 287,289Mc, 291,293Lv, 293Ts, 293,295,297Og(α); calculated T1/2, transitions J, π, preformation probabilities. Comparison with available data.
doi: 10.1088/1674-1137/41/12/124109
2017SU06 Phys.Rev. C 95, 014319 (2017) X.-D.Sun, C.Duan, J.-G.Deng, P.Guo, X.-H.Li Systematic study of α decay for odd-A nuclei within a two-potential approach RADIOACTIVITY 145Pm, 147Sm, 147Eu, 149Gd, 149,149m,151Tb, 151,153Dy, 151,151m,153,153mHo, 153,155Er, 153,153m,155Tm, 155,157Yb, 155,155m,157mLu, 157Hf, 159,159mTa, 159,161,163W, 159m,161m,163,163m,165m,167m,169mRe, 161,163,165,167,169Os, 165m,167,167m,169,169m,171m,173m,175,177Ir, 167,171,173,175,177,179,181,183Pt, 173,175,177,179,181,183,185Au, 173,177,179,183,185Hg, 177,183,187mTl, 179,185,185m,187,187m,189,191mPb, 185m,187m,189m,191m,193m,195m,209,211,213Bi, 187,189,195,195m,197,199,201,203,205,207,211,213,215,217Po, 191m,193m,197,199,201,203,205,207,209,211,213,215,217At, 193,195,195m,197,203,205,207,209,213,215,217,219,221,223Rn, 199,201,203,205,207,209,211,213,215,219,221,223Fr, 203,207,209,211,213,215,217,219,221,223Ra, 207,211,215,217,219,221,223,225,227Ac, 215,217,219,221,223,225,227,229,231Th, 213,215,217,217m,219,221,223,227,229,231Pa, 219,225,227,229,231,235U, 225,227,229,231,235,237,239Np, 229,231,233,235,237,241Pu, 233,235,237,239,241,243Am, 233,237,239,243,245,247Cm, 243,245,247,249Bk, 247,249,255Cf, 243,251,253Es, 243,247,247m,251,255,257Fm, 247,247m,251,253,255,257Md, 251No, 253,255mLr, 255m,257m,261,263Rf, 257Db, 259m,261,263,265Sg, 265,267Hs, 267,269,271,271m,273,273m,277,281Ds, 281,285Cn, 289Fl(α); calculated α-decay half-lives for odd-A nuclei, preformation probabilities, and compared with experimental values. Two-potential approach based on isospin dependent nuclear potential.
doi: 10.1103/PhysRevC.95.014319
2017SU11 Phys.Rev. C 95, 044303 (2017) X.-D.Sun, J.-G.Deng, D.Xiang, P.Guo, X.-H.Li Systematic study of α decay half-lives of doubly odd nuclei within the two-potential approach RADIOACTIVITY 105,106,107,108,109,110Te, 108,109,110,111,112,113I, 109,110,111,112,113,115Xe, 112,114Cs, 114Ba, 148Eu, 152,154Ho, 154,156Tm, 156Lu, 158Ta, 160,162,164,166Re, 166,168,170,172,174Ir, 170,186Au, 180,186Tl, 190,192,194,196,212,214Bi, 192,194,198,200,202,204,206,208,210,212,214,216,218At, 202,204,208,210,212,214,216,218,220Fr, 212,220,224,228Pa, 214,216,218,220,222,226Ac, 232,236Np, 236,238,242Am, 246,248Bk, 244,246,248,252,254Es, 246,248,250,256,258,260Md, 254,258,260Lr, 272,274,278,280,282Rg, 258,260,262,268Db, 260,264,266,270,272,274Bh, 268,270,274,276,278Mt, 278,282,284,286Nh, 288,290Mc, 292,294Ts, 296119(α); calculated α-decay half-lives, and α preformation probabilities for odd-odd nuclei using a two-potential approach, and compared with experimental values.
doi: 10.1103/PhysRevC.95.044303
2013CH08 Phys.Rev. C 87, 024910 (2013) J.-W.Chen, J.Deng, H.Dong, Q.Wang Shear and bulk viscosities of a gluon plasma in perturbative QCD: Comparison of different treatments for the gg<->ggg process
doi: 10.1103/PhysRevC.87.024910
2005LI06 Radiat.Meas. 39, 401 (2005) Monte Carlo calculation of the cross-sections of single event upset induced by 14 MeV neutrons
doi: 10.1016/j.radmeas.2004.05.005
2005NO12 Nucl.Phys. A758, 263c (2005) K.Nomoto, N.Tominaga, H.Umeda, K.Maeda, T.Ohkubo, J.Deng Nucleosynthesis in Hypernovae and Population III Supernovae
doi: 10.1016/j.nuclphysa.2005.05.045
2005SC08 Nucl.Instrum.Methods Phys.Res. A545, 658 (2005) D.Schmidt, Z.Zhou, X.Ruan, H.Tang, B.Qi, H.Xia, J.Deng Application of non-monoenergetic sources in fast neutron scattering measurements NUCLEAR REACTIONS 51V(n, nX), E ≈ 10.2 MeV; measured neutron spectra, σ(E, θ). Two methods for separating scattering fractions discussed.
doi: 10.1016/j.nima.2005.02.031
2003DE28 Nucl.Phys. A718, 569c (2003) J.Deng, P.A.Mazzali, K.Maeda, K.Nomoto The Type Ic hypernova SN 2002ap
doi: 10.1016/S0375-9474(03)00855-8
2003NO05 Nucl.Phys. A718, 277c (2003) K.Nomoto, H.Umeda, K.Maeda, T.Ohkubo, J.Deng, P.Mazzali Nucleosynthesis in Hypernovae and Extremely Metal-Poor Stars
doi: 10.1016/S0375-9474(03)00728-0
2003NO08 Prog.Theor.Phys.(Kyoto), Suppl. 151, 44 (2003) K.Nomoto, K.Maeda, H.Umeda, T.Ohkubo, J.Deng, P.Mazzali Nucleosynthesis in Black-Hole-Forming Supernovae and Extremely Metal-Poor Stars
doi: 10.1143/PTPS.151.44
2002DE50 Phys.Rev. C66, 047001 (2002) New measurement of the neutron-proton scattering length anp via the n-d breakup reaction at 25 MeV NUCLEAR REACTIONS 2H(n, np), E=25 MeV; measured Ep, np-coin; deduced neutron-proton scattering length.
doi: 10.1103/PhysRevC.66.047001
2002SI06 Phys.Rev. C65, 034010 (2002) A.Siepe, J.Deng, V.Huhn, L.Watzold, Ch.Weber, W.von Witsch, H.Witala, W.Glockle Neutron-Proton and Neutron-Neutron Quasifree Scattering in the n-d Breakup Reaction at 26 MeV NUCLEAR REACTIONS 2H(n, 2n), (n, np), E=26 MeV; measured En, Ep, nn-, np-coin, σ(E1, E2); deduced neutron-neutron and neutron-proton quasifree scattering σ, related features.
doi: 10.1103/PhysRevC.65.034010
2002WA10 Phys.Lett. 536B, 203 (2002) M.Z.Wang, Q.Yue, J.R.Deng, W.P.Lai, H.B.Li, J.Li, Y.Liu, B.J.Qi, X.C.Ruan, C.H.Tang, H.Q.Tang, H.T.Wong, S.C.Wu, B.Xin, Z.Y.Zhou Nuclear Recoil Measurement in CsI(Tl) Crystal for Cold Dark Matter Detection NUCLEAR REACTIONS I, Cs(n, n), E ≈ 8 MeV; measured nuclear recoil spectra in scintillator crystal, σ(θ). Implications for dark matter search discussed. Comparison with optical model predictions.
doi: 10.1016/S0370-2693(02)01836-1
2001ZH09 Nucl.Phys. A684, 545c (2001) Z.Zhou, A.S.Crowell, J.Deng, W.Glockle, C.R.Howell, H.Kamada, B.Qi, R.A.Macri, X.Ruan, H.Tang, R.L.Walter, H.Witala The Space-Star Anomaly in nd Breakup at 25 MeV NUCLEAR REACTIONS 2H(n, np), E=25 MeV; measured nn-coin, σ(θ). Comparison with model predictions.
doi: 10.1016/S0375-9474(01)00389-X
2000ZH59 High Energy Phys. and Nucl.Phys. (China) 24, 418 (2000) S.-J.Zhu, M.-G.Wang, L.-Y.Zhu, M.Li, C.-Y.Gan, L.-M.Yang, M.Sakhaee, S.-L.Pau, J.-K.Deng, G.-L.Long, J.H.Hamilton, A.V.Ramayya, B.R.S.Babu, J.K.Hwang, W.C.Ma, J.Komicki, J.D.Cole, R.Aryaeinejad, M.W.Drigert, J.O.Rasmussen, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.G.Prussin, I.Y.Lee, Yu.Ts.Oganessian, G.M.Ter-Akopian, A.V.Daniel Octupole Deformation in Neutron Rich 145, 147La Nuclei
1999HA10 Acta Phys.Slovaca 49, 31 (1999) J.H.Hamilton, A.V.Ramayya, J.K.Hwang, W.Greiner, S.J.Zhu, A.Sandulescu, A.Florescu, J.Kormicki, G.Ter-Akopian, Y.Oganesyan, A.V.Daniel, G.S.Popeko, J.Kliman, M.Morhac, J.D.Cole, R.Aryaeinejad, M.W.Drigert, W.E.Collins, W.C.Ma, E.F.Jones, L.K.Peker, P.M.Gore, G.Drafta, B.R.S.Babu, G.Wang, J.K.Deng Cold Spontaneous Fission Processes of 252Cf and the Structure of Neutron Rich Ba and La Nuclei RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin; deduced cold binary, ternary fission yields. 143,144,146Ba, 145,147La deduced high-spin levels, J, π, stable octupole deformation. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13749. 1999MA54 Phys.Rev. C60, 027301 (1999) P.F.Mantica, M.R.Papantonakis, K.Butler-Moore, J.K.Deng, J.H.Hamilton, W.D.Hamilton, J.Kormicki, A.Lahamer, W.C.Ma, A.V.Ramayya Nuclear Orientation of 96Tc RADIOACTIVITY 96Tc(EC); measured Eγ, Iγ(θ) from oriented nuclei. 96Mo deduced transitions δ. Comparison with IBM-2 calculations.
doi: 10.1103/PhysRevC.60.027301
1999SA58 Phys.Rev. C60, 067303 (1999) M.Sakhaee, S.J.Zhu, J.H.Hamilton, A.V.Ramayya, J.K.Hwang, X.Q.Zhang, L.M.Yang, L.Y.Zhu, C.Y.Gan, E.F.Jones, P.M.Gore, T.N.Ginter, B.R.S.Babu, W.C.Ma, J.Kormicki, C.J.Beyer, G.L.Long, J.K.Deng, K.Li, J.D.Cole, R.Aryaeinejad, M.W.Drigert, J.O.Rasmussen, S.Asztalos, I.Y.Lee, A.O.Macchiavelli, S.Y.Chu, K.E.Gregorich, M.F.Mohar, M.A.Stoyer, R.W.Lougheed, K.J.Moody, J.F.Wild, S.G.Prussin, G.M.Ter-Akopian, A.V.Daniel, Yu.Ts.Oganessian Identification of Levels in Neutron-Rich 145Ce and 147Ce Nuclei RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 145,147Ce deduced high-spin levels, J, π, configurations. Gammasphere array. Comparison with particle-plus-rotor calculations.
doi: 10.1103/PhysRevC.60.067303
1999ZH05 Phys.Rev. C59, 1316 (1999) S.J.Zhu, J.H.Hamilton, A.V.Ramayya, M.G.Wang, J.K.Hwang, E.F.Jones, L.K.Peker, B.R.S.Babu, G.Drafta, W.C.Ma, G.L.Long, L.Y.Zhu, M.Li, C.Y.Gan, T.N.Ginter, J.Kormicki, J.K.Deng, D.T.Shi, W.E.Collins, J.D.Cole, R.Aryaeinejad, M.W.Drigert, J.O.Rasmussen, R.Donangelo, J.Gilat, S.Asztalos, I.Y.Lee, A.O.Macchiavelli, S.Y.Chu, K.E.Gregorich, M.F.Mohar, M.A.Stoyer, R.W.Lougheed, K.J.Moody, J.F.Wild, S.G.Prussin, G.M.Ter-Akopian, A.V.Daniel, Yu.Ts.Oganessian Octupole Correlations in Neutron-Rich 145, 147La Nuclei: Coriolis-limit-coupling bands with aligned h11/2 Proton RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 145,147La deduced high-spin levels, possible J, π, B(E1)/B(E2), octupole correlations. Cranked shell model analysis. Gammasphere array.
doi: 10.1103/PhysRevC.59.1316
1999ZH28 Chin.Phys.Lett. 16, 635 (1999) S.-J.Zhu, M.Li, L.-Y.Zhu, C.-Y.Gan, M.Sakhaee, L.-M.Yang, S.-L.Pau, G.-L.Long, J.-K.Deng, S.-X.Wen, X.-G.Wu, X.-A.Liu Identification of Collective Oblate Bands in 138Ce NUCLEAR REACTIONS 124Sn(18O, 4n), E=78 MeV; measured Eγ, Iγ, γγ-coin. 138Ce deduced high-spin levels, J, π, configurations, oblate deformation. Moments of inertia in neighboring nuclides discussed.
doi: 10.1088/0256-307X/16/9/005
1999ZH31 Phys.Rev. C60, 051304 (1999) S.J.Zhu, J.H.Hamilton, A.V.Ramayya, E.F.Jones, J.K.Hwang, M.G.Wang, X.Q.Zhang, P.M.Gore, L.K.Peker, G.Drafta, B.R.S.Babu, W.C.Ma, G.L.Long, L.Y.Zhu, C.Y.Gan, L.M.Yang, M.Sakhaee, M.Li, J.K.Deng, T.N.Ginter, C.J.Beyer, J.Kormicki, J.D.Cole, R.Aryaeinejad, M.W.Drigert, J.O.Rasmussen, S.Asztalos, I.Y.Lee, A.O.Macchiavelli, S.Y.Chu, K.E.Gregorich, M.F.Mohar, G.M.Ter-Akopian, A.V.Daniel, Yu.Ts.Oganessian, R.Donangelo, M.A.Stoyer, R.W.Lougheed, K.J.Moody, J.F.Wild, S.G.Prussin, J.Kliman, H.C.Griffin Octupole Correlations in Neutron-Rich 143, 145Ba and a Type of Superdeformed Band in 145Ba RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 143,145Ba deduced high-spin levels, J, π, B(E1)/B(E2), possible stable octupole deformation. Gammasphere array.
doi: 10.1103/PhysRevC.60.051304
1998ZH39 Chin.Phys.Lett. 15, 793 (1998) S.-J.Zhu, C.-Y.Gan, J.H.Hamilton, A.V.Ramayya, B.R.S.Babu, M.Sakhaee, W.C.Ma, G.-L.Long, J.-K.Deng, L.-Y.Zhu, M.Li, L.-M.Yang, J.Kormicki, J.D.Cole, R.Aryaeinejad, Y.K.Dardenne, M.W.Drigert, J.O.Rasmussen, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.G.Prussin, I.Y.Lee, N.R.Johnson, F.K.McGowan Collective Band Structures in the Neutron-Rich 107, 109Ru Nuclei RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 107,109Ru deduced high-spin levels, J, π, configurations. Particle-rotor model analysis. Gammasphere array.
doi: 10.1088/0256-307X/15/11/005
1997DO20 Nuovo Cim. 110A, 949 (1997) R.S.Dodder, E.F.Jones, J.H.Hamilton, A.V.Ramayya, P.Gore, C.J.Beyer, A.P.De Lima, J.K.Hwang, X.Q.Zhang, S.J.Zhu, Q.H.Lu, T.Ginter, B.R.S.Babu, M.G.Wang, J.Kormicki, J.K.Deng, D.Shi, J.D.Cole, R.Aryaeinejad, K.Butler-Moore, M.W.Drigert, W.C.Ma, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.V.Daniel, J.O.Rasmussen, S.J.Asztalos, I.Y.Lee, A.O.Machiavelli, M.A.Stoyer, R.W.Lougheed, Y.X.Dardenne, S.G.Prussin, R.Donangelo Identical and Shifted Identical Bands RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-, (X-ray)γ-coin. 156,158,160Sm, 160,162Gd deduced levels, J, π, identical bands features.
doi: 10.1007/BF03035931
1997HA64 Prog.Part.Nucl.Phys. 38, 273 (1997) J.H.Hamilton, A.V.Ramayya, J.K.Hwang, J.Kormicki, B.R.S.Babu, A.Sandulescu, A.Florescu, W.Greiner, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.V.Daniel, S.J.Zhu, M.G.Wang, T.Ginter, J.K.Deng, W.C.Ma, G.S.Popeko, Q.H.Lu, E.Jones, R.Dodder, P.Gore, W.Nazarewicz, J.O.Rasmussen, S.Asztalos, I.Y.Lee, S.Y.Chu, K.E.Gregorich, A.O.Macchiavelli, M.F.Mohar, S.Prussin, M.A.Stoyer, R.W.Lougheed, K.J.Moody, J.F.Wild, L.A.Bernstein, J.A.Becker, J.D.Cole, R.Aryaeinejad, Y.X.Dardenne, M.W.Drigert, K.Butler-Moore, R.Donangelo, H.C.Griffin New Cold and Ultra Hot Binary and Cold Ternary Spontaneous Fission Modes for 252Cf and New Band Structures with Gammasphere RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-, (X-ray)γ-coin, prompt neutron multiplicity following binary, ternary fission; deduced fragments isotopic yields. 142,143,144,145,146,148Ba, 140Xe, 144Ce, 99,100,102Zr, 98,100Sr, 112,114,116Pd, 156,158,160Sm deduced high-spin levels, J, π, rotational bands features. 108,110,112Ru, 148,150,152Ce, 146,148,150,152,154Nd, 140Ba, 98Sr, 104Zr deduced rotational bands features. Gammasphere array.
doi: 10.1016/S0146-6410(97)00037-9
1997TE03 Phys.Rev. C55, 1146 (1997) G.M.Ter-Akopian, J.H.Hamilton, Yu.Ts.Oganessian, A.V.Daniel, J.Kormicki, A.V.Ramayya, G.S.Popeko, B.R.S.Babu, Q.-H.Lu, K.Butler-Moore, W.-C.Ma, E.F.Jones, J.K.Deng, D.Shi, J.Kliman, M.Morhac, J.D.Cole, R.Aryaeinejad, N.R.Johnson, I.Y.Lee, F.K.McGowan Yields of Correlated Fragment Pairs in Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured correlated fragment pairs yields for Ru-Xe, Zr-Ce, Mo-Ba, Sr-Nd isotopes; deduced fission fragment yields vs mass, neutron multiplicities.
doi: 10.1103/PhysRevC.55.1146
1997ZH23 J.Phys.(London) G23, L77 (1997) S.J.Zhu, J.H.Hamilton, A.V.Ramayya, M.G.Wang, E.F.Jones, J.K.Hwang, B.R.S.Babu, W.C.Ma, G.L.Long, M.Li, L.Y.Zhu, J.K.Deng, T.N.Ginter, J.Kormicki, J.D.Cole, R.Aryaeinejad, Y.K.Dardenne, M.W.Drigert, G.Ter-Akopian, Yu.Ts.Oganessian, A.Daniel, J.O.Rasmussen, M.A.Stoyer, I.Y.Lee, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.G.Prussin, N.R.Johnson, F.K.McGowan High Spin Octupole Correlations in the N = 85, 139Xe and 141Ba Isotones RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγγ-coin. 139Xe, 141Ba deduced high-spin levels, J, π, B(E1)/B(E2) ratios, configurations, octupole bands. Gammasphere array. Band systematics from other data input.
1997ZH25 Chin.Phys.Lett. 14, 569 (1997) S.-J.Zhu, M.-G.Wang, J.H.Hamilton, A.V.Ramayya, B.R.S.Babu, W.C.Ma, G.-L.Long, J.-K.Deng, L.-Y.Zhu, M.Li, T.N.Ginter, J.Kormicki, J.D.Cole, R.Aryaeinejad, Y.K.Dardenne, M.W.Drigert, J.O.Rasmussen, Yu.Ts.Oganessian, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.G.Prussin, I.Y.Lee, N.R.Johnson, F.K.McGowan Reflection Asymmetric Shapes in the Neutron-Rich 140,143Ba Isotopes RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 140,143Ba deduced levels, J, π, B(E1)/B(E2), γ-multipolarity, octupole deformation, other shape related features.
1997ZH41 High Energy Phys. and Nucl.Phys. (China) 21, 104 (1997) S.Zhu, M.Wang, J.Deng, J.H.Hamilton, A.V.Ramayya, B.R.S.Babu, W.C.Ma, J.O.Rasmussen, M.A.Stoyer, I.Y.Lee, J.D.Cole Level Schemes in Neutron-Rich 141Xe, 152Ce, 153Nd and 160Sm Nuclei
1996BI06 Phys.Rev. C53, 3165 (1996) K.S.Bindra, P.F.Hua, B.R.S.Babu, C.Baktash, J.Barreto, D.M.Cullen, C.N.Davids, J.K.Deng, J.D.Garrett, M.L.Halbert, J.H.Hamilton, N.R.Johnson, A.Kirov, J.Kormicki, I.Y.Lee, W.C.Ma, F.K.McGowan, A.V.Ramayya, D.G.Sarantites, F.Soramel, D.Winchell Reply to ' Comment on ' Prolate-Oblate Band Mixing and New Bands in 182Hg ' ' NUCLEAR STRUCTURE 182Hg; analyzed band-mixing interpretations; deduced method's applicability limitations.
doi: 10.1103/PhysRevC.53.3165
1996HA27 Phys.Rep. 264, 215 (1996) J.H.Hamilton, G.M.Ter-Akopian, Yu.Ts.Oganessian, J.Kormicki, S.J.Zhu, M.G.Wang, Q.Lu, K.Butler-Moore, A.V.Ramayya, W.C.Ma, B.R.S.Babu, D.Shi, J.K.Deng, G.S.Popeko, A.V.Daniel, W.Greiner, A.Sandulescu, J.D.Cole, R.Aryaeinejad, J.Kliman, V.Polhorsky, M.Morhac, N.R.Johnson, I.Y.Lee, F.K.McGowan, L.K.Peker Structure of Neutron-Rich Nuclei and Neutron Multiplicities in Spontaneous Fission RADIOACTIVITY 252Cf(SF); compiled, reviewed γγ-, γγγ-coin data. 140,143,145,147Ba, 136Te, 138Xe deduced high-spin levels. Other nuclei included.
doi: 10.1016/0370-1573(95)00039-9
1996TE04 Phys.Rev.Lett. 77, 32 (1996) G.M.Ter-Akopian, J.H.Hamilton, Yu.Ts.Oganessian, A.V.Daniel, J.Kormicki, A.V.Ramayya, G.S.Popeko, B.R.S.Babu, Q.-H.Lu, K.Butler-Moore, W.-C.Ma, S.Cwiok, W.Nazarewicz, J.K.Deng, D.Shi, J.Kliman, M.Morhac, J.D.Cole, R.Aryaeinejad, N.R.Johnson, I.Y.Lee, F.K.McGowan, J.X.Saladin New Spontaneous Fission Mode for 252Cf: Indication of hyperdeformed 144,145,146Ba at scission RADIOACTIVITY 252Cf(SF); measured γγ-coin, prompt neutron multiplicities, Mo, Ba isotopes correlated fragment pairs yields; deduced new fission mode. 144,145,146Ba deduced hyperdeformed shape evidence at scission.
doi: 10.1103/PhysRevLett.77.32
1996TE07 Bull.Rus.Acad.Sci.Phys. 60, 129 (1996) G.M.Ter-Akopian, J.Hamilton, Yu.Ts.Oganessian, A.V.Daniel, J.Kormicki, G.S.Popeko, A.V.Ramayya, Q.Lu, K.Butler-Moore, W.-C.Ma, J.K.Deng, D.Shi, J.Kliman, M.Morhac, J.D.Cole, R.Aryaeinejad, S.J.Zhu, B.R.S.Babu, N.P.Johnson, I.J.Lee, F.K.McGowan Yields of Correlated Fragment Pairs from Spontaneous Fission of the 252Cf Nuclei RADIOACTIVITY 252Cf(SF); measured γ spectra, γγ-coin; deduced correlated fragment pairs yields for Xe-Ru, Ba-Mo, Ce-Zr isotopes. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13648. 1995BI02 Phys.Rev. C51, 401 (1995) K.S.Bindra, P.F.Hua, B.R.S.Babu, C.Baktash, J.Barreto, D.M.Cullen, C.N.Davids, J.K.Deng, J.D.Garrett, M.L.Halbert, J.H.Hamilton, N.R.Johnson, A.Kirov, J.Kormicki, I.Y.Lee, W.C.Ma, F.K.McGowan, A.V.Ramayya, D.G.Sarantites, F.Soramel, D.Winchell Prolate-Oblate Band Mixing and New Bands in 182Hg NUCLEAR REACTIONS 154Gd(32S, 4n), E=160-165 MeV; measured Eγ, Iγ, γγ(θ). 182Hg deduced high-spin levels, J, π, shape features. Compton suppressed Ge detectors, fragment mass analyzer, high spin states.
doi: 10.1103/PhysRevC.51.401
1995DE30 Phys.Rev. C52, 595 (1995) J.K.Deng, W.C.Ma, J.H.Hamilton, A.V.Ramayya, J.Kormicki, W.B.Gao, X.Zhao, D.T.Shi, I.Y.Lee, J.D.Garrett, N.R.Johnson, D.Winchell, M.Halbert, C.Baktash New High-Spin Band Structures in 184Hg NUCLEAR REACTIONS 156Gd(32S, 4n), E=160 MeV; measured Eγ, Iγ, γγ(θ), DCO ratios. 184Hg deduced high-spin levels, J, π, B(M1)/B(E2) ratios, configurations. Ge(Li) detectors array.
doi: 10.1103/PhysRevC.52.595
1995LU10 Phys.Rev. C52, 1348 (1995) Q.H.Lu, K.Butler-Moore, S.J.Zhu, J.H.Hamilton, A.V.Ramayya, V.E.Oberacker, W.C.Ma, B.R.S.Babu, J.K.Deng, J.Kormicki, J.D.Cole, R.Aryaeinejad, Y.X.Dardenne, M.Drigert, L.K.Peker, J.O.Rasmussen, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, I.Y.Lee, M.F.Mohar, J.M.Nitschke, N.R.Johnson, F.K.McGowan, G.M.Ter-Akopian, Yu.Ts.Oganessian, J.B.Gupta Structure of 108,110,112Ru: Identical bands in 108,110Ru RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-, γγγ-, (X-ray)γ-coin. 108,110,112Ru deduced levels, J, π, intraband B(E2) ratios. Rotation-vibration, rigid triaxial rotor calculation.
doi: 10.1103/PhysRevC.52.1348
1995ZH15 J.Phys.(London) G21, L57 (1995); Corrigendum J.Phys.(London) G21, 1555 (1995) S.J.Zhu, J.H.Hamilton, A.V.Ramayya, B.R.S.Babu, Q.H.Lu, W.C.Ma, T.N.Ginter, M.G.Wang, J.Kormicki, J.K.Deng, D.Shi, J.D.Cole, R.Aryaeinejad, J.Rasmussen, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.Prussin, G.M.Ter-Akopian, Yu.Ts.Oganessian, N.R.Johnson, I.Y.Lee, F.K.McGowan Identification of Levels in 160Sm and New High Spin States in 156,158Sm RADIOACTIVITY 252Cf(SF); measured γγ-, (X-ray)(X-ray)-, γ(X-ray)-, γγγ-coin. 156,158Sm deduced high-spin levels, J, π, configuration, band structure. 160Sm deduced levels.
doi: 10.1088/0954-3899/21/7/002
1995ZH34 Phys.Lett. 357B, 273 (1995) S.J.Zhu, Q.H.Lu, J.H.Hamilton, A.V.Ramayya, L.K.Peker, M.G.Wang, W.C.Ma, B.R.S.Babu, T.N.Ginter, J.Kormicki, D.Shi, J.K.Deng, W.Nazarewicz, J.O.Rasmussen, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.Asztalos, S.G.Prussin, J.D.Cole, R.Aryaeinejad, Y.K.Dardenne, M.Drigert, K.J.Moody, R.W.Lougheed, J.F.Wild, N.R.Johnson, I.Y.Lee, F.K.McGowan, G.M.Ter-Akopian, Yu.Ts.Oganessian Octupole Deformation in 142,143Ba and 144Ce: New band structures in neutron-rich Ba-isotopes RADIOACTIVITY 252Cf(SF); 242Pu(SF); measured γγ-, γγγ-coin following fission fragment decay. 142,143,144,145,146,147Ba, 144Ce deduced high-spin levels, J, π, band structure, shape features, B(λ) in some cases.
doi: 10.1016/0370-2693(95)00900-6
1995ZH39 J.Phys.(London) G21, L75 (1995) S.J.Zhu, J.H.Hamilton, Q.H.Lu, A.V.Ramayya, M.G.Wang, B.R.S.Babu, T.N.Ginter, W.C.Ma, J.K.Deng, D.Shi, J.Kormicki, J.D.Cole, R.Aryaeinejad, Y.X.Dardenne, M.W.Drigert, N.R.Johnson, I.Y.Lee, F.K.McGowan, G.M.Ter-Akopian, Yu.Ts.Oganessian, J.O.Rasmussen, M.A.Stoyer, S.Y.Chu, K.E.Gregorich, M.F.Mohar, S.Prussin Identification of 152Ce and Unexpected Variations in Moments of Inertia with Neutron Number and Spin in 142-148Ba, 144-152Ce and 146-156Nd RADIOACTIVITY 252Cf, 242Pu(SF); measured γ(X-ray)-, γγγ-, (X-ray)(X-ray)-coin. 142,144,146,148Ba, 144,146,148,150,152Ce, 146,148,150,152,154,156Nd deduced high-spin levels, band structure, moments of inertia.
doi: 10.1088/0954-3899/21/10/001
1994HA31 J.Phys.(London) G20, L85 (1994) J.H.Hamilton, A.V.Ramayya, J.Kormicki, W.-C.Ma, Q.Lu, D.Shi, J.K.Deng, S.J.Zhu, A.Sandulescu, W.Greiner, G.M.Ter-Akopian, Yu.Ts.Oganessian, G.S.Popeko, A.V.Daniel, J.Kliman, V.Polhorsky, M.Morhac, J.D.Cole, R.Aryaeinejad, I.Y.Lee, N.R.Johnson, F.K.McGowan Zero Neutron Emission in Spontaneous Fission of 252Cf: A form of cluster radioactivity RADIOACTIVITY 252Cf(SF); measured γγγ-coin; deduced neutronless spontaneous fission evidence, 106Mo+146Ba, 108Mo+144Ba, 104Zr+148Ce cluster production.
doi: 10.1088/0954-3899/20/8/003
1994KL10 Yad.Fiz. 57, No 7, 1174 (1994); Phys.Atomic Nuclei 57, 1108 (1994) J.Kliman, V.Polhorsky, M.Morhac, G.M.Ter-Akopian, Yu.Ts.Oganessian, G.S.Popeko, A.V.Daniel, J.H.Hamilton, K.Butler-Moore, A.V.Ramayya, W.-C.Ma, X.Zhao, Q.Lu, D.Shi, J.K.Deng, J.Kormicki, S.Zhu, J.D.Cole, R.Aryaeinejad, R.C.Greenwood, S.S.Harrill, N.D.Lohstreter, I.Y.Lee, N.R.Johnson, F.K.McGowan Correlated Yields and the Emission of Neutrons of Mo/Ba Fragments from 252Cf(SF) RADIOACTIVITY 252Cf(SF); analyzed fission data; deduced (Mo/Ba)fragment charge division evidence.
1994TE08 Phys.Rev.Lett. 73, 1477 (1994) G.M.Ter-Akopian, J.H.Hamilton, Yu.Ts.Oganessian, J.Kormicki, G.S.Popeko, A.V.Daniel, A.V.Ramayya, Q.Lu, K.Butler-Moore, W.C.Ma, J.K.Deng, D.Shi, J.Kliman, V.Polhorsky, M.Morhac, W.Greiner, A.Sandelescu, J.D.Cole, R.Aryaeinejad, N.R.Johnson, I.Y.Lee, F.K.McGowan Neutron Multiplicities and Yields of Correlated Zr-Ce and Mo-Ba Fragment Pairs in Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured γγ-, γγγ-coin; deduced Zr-Ce, Mo-Ba correlated fission fragment pair relative yields, neutron multiplicities.
doi: 10.1103/PhysRevLett.73.1477
1993AR05 Phys.Rev. C48, 566 (1993) R.Aryaeinejad, J.D.Cole, R.C.Greenwood, S.S.Harrill, N.P.Lohstreter, K.Butler-Moore, S.Zhu, J.H.Hamilton, A.V.Ramayya, X.Zhao, W.C.Ma, J.Kormicki, J.K.Deng, W.B.Gao, I.Y.Lee, N.R.Johnson, F.K.McGowan, G.Ter-Akopyan, Y.Oganesyan Band Crossing Observed in Neutron-Rich Pd Isotopes via Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured Iγ, γγ-, nγ-coin. 112,114,116Pd deduced levels, J, π, band crossing. Interacting boson and cranked shell models.
doi: 10.1103/PhysRevC.48.566
1993BU12 J.Phys.(London) G19, L121 (1993) K.Butler-Moore, J.H.Hamilton, A.V.Ramayya, S.Zhu, X.Zhao, W.C.Ma, J.Kormicki, J.K.Deng, W.B.Gao, J.D.Cole, R.Aryaeinejad, I.Y.Lee, N.R.Johnson, F.K.McGowan, G.Ter-Akopyan, Y.Oganesyan Levels in 136Te and New High-Spin States in Neutron-Rich N = 84 Isotones RADIOACTIVITY 252Cf(SF); measured γγ-, γγγ-coin. 140,138Xe, 140Ba, 136Te deduced levels, J, π, transition Iγ.
doi: 10.1088/0954-3899/19/7/004
1993DE42 Phys.Lett. 319B, 63 (1993) J.K.Deng, W.C.Ma, J.H.Hamilton, J.D.Garrett, C.Baktash, D.M.Cullen, N.R.Johnson, I.Y.Lee, F.K.McGowan, S.Pilotte, C.H.Yu, W.Nazarewicz High-Spin Single-Particle States in 193Hg NUCLEAR REACTIONS 150Nd(48Ca, 5n), E=210 MeV; measured γγγ-, higher fold-coin, DCO ratios. 193Hg deduced levels, J, π, band structure.
doi: 10.1016/0370-2693(93)90782-D
1993MA02 Phys.Rev. C47, R5 (1993) W.C.Ma, J.H.Hamilton, A.V.Ramayya, L.Chaturvedi, J.K.Deng, W.B.Gao, Y.R.Jiang, J.Kormicki, X.W.Zhao, N.R.Johnson, J.D.Garrett, I.Y.Lee, C.Baktash, F.K.McGowan, W.Nazarewicz, R.Wyss First Evidence for States in Hg Nuclei with Deformations between Normal and Super Deformation NUCLEAR REACTIONS 154Gd(36S, 4n), E=159-175 MeV; measured γγ-coin. 186Hg deduced levels, J, π, T1/2, deformation between normal and superdeformed, configuration, Iγ, quadrupole moments.
doi: 10.1103/PhysRevC.47.R5
1992DE50 Nucl.Instrum.Methods Phys.Res. A317, 242 (1992) J.K.Deng, W.C.Ma, J.H.Hamilton, A.V.Ramayya, J.Rikovska, N.J.Stone, W.L.Croft, R.B.Piercey, J.C.Morgan, P.F.Mantica, Jr. Test and Application of Symmetrical Four-Detector Compton Polarimeter for Low Temperature Nuclear Orientation and In-Beam Spectroscopy RADIOACTIVITY 192Ir(β-), (EC); 57Co(EC); 60Co(β-); 54Mn(EC); measured γ linear polarization, DCO, oriented nuclei; deduced polarization detection efficiency, other features. Symmetrical four-detector Compton polarimeter.
doi: 10.1016/0168-9002(92)90614-A
1992DE54 Hyperfine Interactions 75, 439 (1992) J.K.Deng, J.H.Hamilton, A.V.Ramayya, W.C.Ma, X.W.Zhao, J.Kormicki, N.Severijns, L.Vanneste, W.D.Hamilton, P.F.Mantica, Jr., H.K.Carter On-Line Nuclear Orientation of 70As RADIOACTIVITY 70As(β+), (EC); measured γ-anistropy. 70Ge deduced transitions δ, symmetry features. On-line nuclear orientation.
doi: 10.1007/BF02399001
1992DE55 Hyperfine Interactions 75, 519 (1992) J.K.Deng, J.H.Hamilton, A.V.Ramayya, J.Rikovska, N.J.Stone, W.L.Croft, R.B.Piercey, J.C.Morgan, P.F.Mantica, Jr. Test of a Symmetrical Four-Detector Compton Polarimeter Using Low Temperature Nuclear Orientation RADIOACTIVITY 57Co(EC); 54Mn(EC); 60Co(β-); 192Ir(EC), (β-); measured γ(θ), γ linear polarization, orientation by hyperfine interaction at low temperature; deduced polarization detector efficiency. Symmetrical four-detector Compton polarimeter.
doi: 10.1007/BF02399007
1992ZH42 Rev.Mex.Fis. 38, 53 (1992) S.Zhu, X.Zhao, J.H.Hamilton, A.V.Ramayya, Q.Lu, W.-C.Ma, L.K.Peker, J.Kormicki, H.Xie, W.B.Gao, J.K.Deng, I.Y.Lee, N.R.Johnson, F.K.McGowan, C.E.Bemis, J.D.Cole, R.Aryaeinejad, G.M.Ter-Akopian, Yu.Ts.Oganessian Higher Spin States in Neutron Rich Nuclei
1991QI01 Chin.J.Nucl.Phys. 13, No 4, 343 (1991) H.Qi, Q.Chen, Y.Chen, H.Chen, Z.Chen, J.Deng, Z.Chen, H.Tang, B.Qi Small Angle Scattering Cross Sections of 12 MeV Neutron from 238U and Fe NUCLEAR REACTIONS 238U, Fe(n, n), E=12, 14 MeV; measured σ(θ).
1986CH46 Chin.J.Nucl.Phys. 8, 298 (1986) Chen Zemin, Deng Jingkang, Xu Sida, Xu Xiangyuan Polarization Analyzing Power for Elastic Scattering of 2.7 MeV Polarized Neutrons on Pb NUCLEAR REACTIONS 208Pb(polarized n, n), E=2.7 MeV; measured σ(θ), analyzing power vs θ. Tof. Optical model analyses. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31651. 1986DE40 Chin.J.Nucl.Phys. 8, 207 (1986) Independent α-Particle Model and 16O(12C, 16O)12C Reaction NUCLEAR REACTIONS 16O(12C, 16O), E=76.8 MeV; calculated σ(θ). DWBA.
Back to query form Note: The following list of authors and aliases matches the search parameter J.Deng: , J.G.DENG, J.K.DENG, J.R.DENG, J.Y.DENG |