NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.Jing Found 20 matches. 2001JI05 Phys.Lett. 518B, 221 (2001) K.X.Jing, L.W.Phair, L.G.Moretto, Th.Rubehn, L.Beaulieu, T.S.Fan, G.J.Wozniak Fission Transient Times from Fission Probabilities of Neighboring Isotopes NUCLEAR REACTIONS 182,183,184,186W(3He, F), (α, F), E ≈ 30-140 MeV; measured fission excitation functions. 185,186,187,188,189Os deduced compound nucleus fission transient times.
doi: 10.1016/S0370-2693(01)00977-7
2000AS01 Phys.Rev. C61, 014602 (2000) S.J.Asztalos, I.Y.Lee, K.Vetter, B.Cederwall, R.M.Clark, M.A.Deleplanque, R.M.Diamond, P.Fallon, K.Jing, L.Phair, A.O.Macchiavelli, F.S.Stephens, G.J.Wozniak, L.A.Bernstein, D.P.McNabb, P.F.Hua, D.G.Sarantites, J.X.Saladin, C.-H.Yu, J.A.Cizewski Isotopic Yields of Neutron-Rich Nuclei from Deep-Inelastic Reactions NUCLEAR REACTIONS 176Yb(154Sm, X), E=949 MeV; 208Pb(154Sm, X), E=1 GeV; measured Eγ, Iγ, γγ-coin; deduced projectile-like-, target-like-fragments isotopic yields, neutron multiplicity. Gammasphere array. Comparison with previous results.
doi: 10.1103/PhysRevC.61.014602
2000FA21 Nucl.Phys. A679, 121 (2000) T.S.Fan, K.X.Jing, L.Phair, K.Tso, M.McMahan, K.Hanold, G.J.Wozniak, L.G.Moretto Excitation Functions and Mass Asymmetric Fission Barriers for Compound Nuclei 70, 76Se NUCLEAR REACTIONS 12C(58Ni, X), (64Ni, X), E=6-14 MeV/nucleon; measured fragment charge distributions, production σ. 70,76Se deduced mass asymmetric fission barriers, transition state fission rates.
doi: 10.1016/S0375-9474(00)00334-1
1999AS05 Phys.Rev. C60, 044307 (1999) S.J.Asztalos, I.Y.Lee, K.Vetter, B.Cederwall, R.M.Clark, M.A.Deleplanque, R.M.Diamond, P.Fallon, K.Jing, L.Phair, A.O.Macchiavelli, J.O.Rasmussen, F.S.Stephens, G.J.Wozniak, J.A.Becker, L.A.Bernstein, D.P.McNabb, P.F.Hua, D.G.Sarantites, J.X.Saladin, C.-H.Yu, J.A.Cizewski, R.Donangelo Spin Yields of Neutron-Rich Nuclei from Deep Inelastic Reactions NUCLEAR REACTIONS 176Yb(48Ca, X), 176Yb, 208Pb(154Sm, X), E ≈ 6 MeV/nucleon; measured Eγ, Iγ, γγ-, (fragment)γ-coin; deduced spin yield vs nucleon transfer, enhancement due to deep inelastic contributions. 172,173,174,175,176,177,178Yb, 173Tm, 152,153,154,155,156Sm deduced high-spin levels, J, π. Gammasphere, silicon strip detector.
doi: 10.1103/PhysRevC.60.044307
1999JI01 Nucl.Phys. A645, 203 (1999) K.X.Jing, L.G.Moretto, A.C.Veeck, N.Colonna, I.Lhenry, K.Tso, K.Hanold, W.Skulski, Q.Sui, G.J.Wozniak Transition State Rates and Mass Asymmetric Fission Barriers of Compound Nuclei 90, 94, 98Mo NUCLEAR REACTIONS 12C(78Kr, X), (82Kr, X), (86Kr, X), E=6-13 MeV/nucleon; measured fragments σ(Z) vs E. 90,94,98Mo deduced mass asymmetric fission barriers, transition state fission rates.
doi: 10.1016/S0375-9474(98)00606-X
1997MO28 Phys.Rev.Lett. 79, 4295 (1997) L.G.Moretto, K.X.Jing, R.Gatti, Th.Rubehn, G.J.Wozniak, R.P.Schmitt Moretto et al. Reply:
doi: 10.1103/PhysRevLett.79.4295
1997MO29 J.Phys.(London) G23, 1323 (1997) L.G.Moretto, K.X.Jing, L.Phair, G.J.Wozniak Particle Structure Function and Sub-Barrier Fusion in Hot Nuclei NUCLEAR REACTIONS Ag(3He, αX), E=55-110 MeV; analyzed α spectra; deduced shape, polarization effects.
doi: 10.1088/0954-3899/23/10/021
1996RU14 Phys.Rev. C54, 3062 (1996) Th.Rubehn, K.X.Jing, L.G.Moretto, L.Phair, K.Tso, G.J.Wozniak Scaling Laws in 3He Induced Nuclear Fission NUCLEAR REACTIONS, ICPND 197Au, 208Pb, 209Bi(3He, F), E=20-145 MeV; measured fission σ; deduced scaling laws, shell effects. 212At, 211Po, 200Tl deduced fission barriers. Transition state method.
doi: 10.1103/PhysRevC.54.3062
1995MO06 Nucl.Phys. A583, 513c (1995) L.G.Moretto, L.Phair, K.Tso, K.Jing, G.J.Wozniak Time-Scale and Branching Ratios in Sequential Multifragmentation NUCLEAR REACTIONS 197Au(36Ar, X), E=80, 110 MeV/nucleon; analyzed intermediate mass fragment multiplicity distributions; deduced thermal binary events sequence evidence.
doi: 10.1016/0375-9474(94)00712-V
1995MO09 Phys.Rev.Lett. 74, 1530 (1995) L.G.Moretto, L.Phair, K.Tso, K.Jing, G.J.Wozniak, R.T.de Souza, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, F.Zhu Are Multifragment Emission Probabilities Reducible to an Elementary Binary Emission Probability NUCLEAR REACTIONS 197Au(36Ar, X), E=80, 110 MeV/nucleon; measured intermediate mass fragment distribution multiplicity; deduced emission probability characteristics, consequences.
doi: 10.1103/PhysRevLett.74.1530
1995MO15 Phys.Rev.Lett. 74, 3557 (1995) L.G.Moretto, K.X.Jing, G.J.Wozniak Transition State Rates and Complex Fragment Decay Widths NUCLEAR REACTIONS 82Kr(12C, X), E ≈ 70-140 MeV; analyzed σ(fragment Z) vs E; deduced energy level parameter. NUCLEAR STRUCTURE 75Br, 90,94Mo, 110,112In; analyzed mass asymmetric fission rate vs square root of (intrinsic excitation energy)(1/2); deduced transitions state predictions validity.
doi: 10.1103/PhysRevLett.74.3557
1995MO33 Phys.Rev.Lett. 75, 4186 (1995) L.G.Moretto, K.X.Jing, R.Gatti, G.J.Wozniak, R.P.Schmitt Scaling Laws, Shell Effects, and Transient Times in Fission Probabilities NUCLEAR STRUCTURE 186,187,188Os, 201Tl, 203,204,205,206,208Pb, 208,210,211,212Po, 213At; analyzed (α, F) reaction fission σ(E) data; deduced effective barriers, shell effects, scaling laws related features.
doi: 10.1103/PhysRevLett.75.4186
1994LI48 Radiochim.Acta 64, 95 (1994) Z.Li, X.Wang, K.Jing, A.Cui, D.Liu, D.Li, Y.Liu, X.Li, C.Liu, S.Su, P.Tang, T.Chih, S.Zhang, S.Zhang, J.Guo Fission Product Yields from 11.3 MeV Neutron-Induced Fission of 238U NUCLEAR REACTIONS 238U(n, F), E=11.3 MeV; measured fission fragment yields vs mass. Double fission chamber, γ-ray spectrometer. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32658. 1991BO08 Nucl.Phys. A523, 386 (1991) D.R.Bowman, G.F.Peaslee, N.Colonna, R.J.Charity, M.A.McMahan, D.Delis, H.Han, K.Jing, G.J.Wozniak, L.G.Moretto, W.L.Kehoe, B.Libby, A.C.Mignerey, A.Moroni, S.Angius, I.Iori, A.Pantaleo, G.Guarino Equilibrium and Non-Equilibrium Complex Fragment Emission in 50-100 MeV/u 139La + 12C Reactions NUCLEAR REACTIONS 12C(139La, X), E=50-100 MeV/nucleon; measured (fragment)(fragment)-coin, charge, angle, mass distributions; deduced emission process.
doi: 10.1016/0375-9474(91)90010-4
1991DE22 Z.Phys. A339, 279 (1991) D.N.Delis, Y.Blumenfeld, D.R.Bowman, N.Colonna, K.Hanold, K.Jing, M.Justice, J.C.Meng, G.F.Peaslee, G.J.Wozniak, L.G.Moretto A Complete Ridge-Line Potential for Complex Fragment Emission NUCLEAR REACTIONS 12C(63Cu, X), E=5-12.7 MeV/nucleon; measured σ vs fragment Z. 75Br deduced emission barriers, mass asymmetric fission, level density parameter ratio.
doi: 10.1007/BF01284065
1991DE30 Nucl.Phys. A534, 403 (1991) D.N.Delis, Y.Blumenfeld, D.R.Bowman, N.Colonna, K.Hanold, K.Jing, M.Justice, J.C.Meng, G.F.Peaslee, G.J.Wozniak, L.G.Moretto Mass Asymmetric Fission Barriers for 75Br NUCLEAR REACTIONS 12C(63Cu, X), E=5-12.7 MeV/nucleon; measured σ(fragment θ) spectra; deduced source velocities, charge distributions, σ(Z) vs E. 75Br deduced mass asymmetric fission barriers.
doi: 10.1016/0375-9474(91)90509-5
1990CH17 Nucl.Phys. A511, 59 (1990) R.J.Charity, K.X.Jing, D.R.Bowman, M.A.McMahan, G.J.Wozniak, L.G.Moretto, N.Colonna, G.Guarino, A.Pantaleo, L.Fiore, A.Gobbi, K.D.Hildenbrand Sources of Complex Fragment Emission in Lanthanum-Induced Reactions at E/A = 14.7 and 18.0 MeV NUCLEAR REACTIONS 12C, 27Al(139La, X), E=14.7, 18.0 MeV/nucleon; measured σ(fragment E, θ), (fragment)(fragment)-coin. Statistical model calculations.
doi: 10.1016/0375-9474(90)90027-J
1989HA08 Nucl.Phys. A492, 138 (1989) H.Y.Han, K.X.Jing, E.Plagnol, D.R.Bowman, R.J.Charity, L.Vinet, G.J.Wozniak, L.G.Moretto Complex-Fragment Emission in 12.6 MeV/Nucleon 63Cu-Induced Reactions on 12C and 27Al Targets NUCLEAR REACTIONS 12C, 27Al(63Cu, X), E=12.6 MeV/nucleon; measured σ(fragment E, θ), (fragment)(fragment)-coin; deduced reaction mechanism. Statistical model.
doi: 10.1016/0375-9474(89)90513-7
1988JI01 Chin.J.Nucl.Phys. 10, 244 (1988) Jing Kexing, Li Ze, Liu Conggui, Liu Yonghui, Su Shuxin, Huang Shengnian Fission Yields in 7.64 MeV Gamma Induced Fission of 232Th NUCLEAR REACTIONS 232Th(γ, F), E=7.64 MeV; measured cumulative, mass chain fission yields from 87Kr to 143Ce. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0500. 1985LI23 Chin.J.Nucl.Phys. 7, 97 (1985) Li Ze, Zhang Chunhua, Liu Conggui, Wang Xiuzhi, Qi Linkun, Cui Anzhi, Lu Huijun, Zhang Sujing, Liu Yonghui, Ju Changxin, Liu Daming, Tang Peijia, Meng Jiangchen, Jing Kexing Mass Distribution in 8.3 MeV Neutron-Induced Fission of 238U NUCLEAR REACTIONS 238U(n, F)83Br/84Br/85Kr/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Nb/99Mo/101Tc/103Ru/104Tc/105Ru/106Ru/107Rh/109Pd/111Ag/113Ag/112Pd/115Cd/121Sb/125Sn/127Sb/128Sn/129Sb/130Sb/131I/132Te/133I/134I/135Xe/136Cs/137Cs/138Cs/139Ba/140Ba/141Ba/141Ce/142La/143Ce/144Ce/146Pr/147Nd/149Pm/149Nd/151Pm/153Sm/156Eu/161Tb, E=8.3 MeV; measured absolute fission yields. Radiochemical methods, Ge(Li) γ-detector. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30751. Back to query form Note: The following list of authors and aliases matches the search parameter K.Jing: , K.X.JING |