NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = K.X.Jing Found 10 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
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
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
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
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
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