NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = N.Manjunatha Found 10 matches. 2023MA28 J.Phys.(London) G50, 035101 (2023) H.C.Manjunatha, P.S.Damodara Gupta, N.Sowmya, N.Manjunatha, K.N.Sridhar, L.Seenappa, T.Nandi Survival probability of compound nuclei in heavy-ion fusion reaction NUCLEAR REACTIONS 249Cf(48Ca, X)294Og, E(cm)=200-230 MeV; 208Pb(50Ti, X)258Rf, 209Bi(50Ti, X)259Db, 244Pu(48Ca, X)292Fl, 208Pb(58Fe, X)266Hs, 208Pb(54Cr, X)262Sg, E not given; analyzed available data; calculated the survival probability of superheavy nuclei; deduced an empirical formula.
doi: 10.1088/1361-6471/acb1cb
2023MA56 Chin.Phys.C 47, 104104 (2023) H.C.Manjunatha, N.Sowmya, L.Seenappa, P.S.Damodara Gupta, N.Manjunatha Heavy ion fusion of spherical nuclei NUCLEAR REACTIONS 238U, 237Np, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, X)Po/Th/No, E(cm)=180-230 MeV; analyzed available data; deduced σ with theoretical models such as the dinuclear system (DNS) and advanced statistical model (ASM).
doi: 10.1088/1674-1137/acea21
2022MA67 Phys.Part. and Nucl.Lett. 19, 597 (2022) H.C.Manjunatha, A.M.Nagaraja, P.S.Damodara Gupta, N.Manjunatha, N.Sowmya, S.A.Cecil Raj Heavy Particle Radioactivity of Superheavy Element Z = 122 RADIOACTIVITY 222,223,224,226Ra(14C), 231Pa, 232U(24Ne), 233U(25Ne), 294,295,296,297,298,299,300122(86Kr), 301,302,303,304,305122(94Zr), 306,307,308,309,310,311,312,313,314122(α); calculated T1/2 using Coulomb and proximity potential model (CPPM) and modified generalized liquid drop model (MGLDM).
doi: 10.1134/S1547477122050260
2022MA69 J.Phys.(London) G49, 125101 (2022) H.C.Manjunatha, Y.S.Vidya, P.S.Damodara Gupta, N.Manjunatha, N.Sowmya, L.Seenappa, T.Nandi Rules of thumb for synthesizing superheavy elements NUCLEAR REACTIONS 249Cf(45Sc, X)294119, 249Bk(50Ti, X)299119, 248Cm(51V, X)299119, 249Cf(50Ti, X)299120, 243Am(54Cr, X)297119, 237Np(58Fe, X)295119, 238U(59Co, X)297119, 248Cm(54Cr, X)302120, 243Am(55Mn, X)298120, 237Np(59Co, X)296120, 244Pu(58Fe, X)302120, 238U(64Ni, X)302120, 248Cm(54Cr, X)302120, 244Pu(58Fe, X)302120, 244Pu(55Mn, X)299119, E not given; analyzed available data; deduced evaporation residue σ, deformation effects using ASM calculations.
doi: 10.1088/1361-6471/ac929c
2022SR02 Int.J.Mod.Phys. E31, 2250043 (2022) M.G.Srinivas, N.Sowmya, H.C.Manjunatha, P.S.Damodara Gupta, R.Munirathnam, N.Manjunatha Radioactivity of Dysprosium RADIOACTIVITY 133,134,135Dy(β+), 133,134,135Tb(p), 132,133,134Gd, 132,133,134Eu, 132,133,134Sm, 132,133,134Pm, 132,133,134Nd, 132,133,134Pr, 132,133,134Ce, 132,133,134La, 132,133,134Ba(β+), 132,133Ba(2β+); analyzed available data; deduced the penetration probability, T1/2 for one proton radioactivity of all possible Dysprosium isotopes. The effective liquid drop model (ELDM).
doi: 10.1142/S0218301322500434
2021MA16 Phys.Rev. C 103, 024311 (2021) H.C.Manjunatha, L.Seenappa, P.S.Damodara Gupta, N.Manjunatha, K.N.Sridhar, N.Sowmya, T.Nandi Quasifission and fusion-fission lifetime studies for the superheavy element Z=120 NUCLEAR REACTIONS 252Cf(50Ti, X)302120*, E=299 MeV; 251Cf(50Ti, X)301120*, E=293 MeV; 250Cf(50Ti, X)300120*, E=300 MeV; 252Cf(49Ti, X)301120*, E=299 MeV; 249Cf(50Ti, X)299120*, E=295 MeV; 248Cm(54Cr, X)302120*, E=316 MeV; 244Pu(58Fe, X)302120*, E=347 MeV; 238U(64Ni, X)302120*, E=372 MeV; 64Ni(238U, X)302120*, E=1383 MeV; 60Ni(238U, X)298120*, E=1476 MeV; calculated fusion barriers, fusion σ, evaporation σ, fusion-fission σ, quasifission σ, quasifission lifetimes, and fusion-fission lifetimes for synthesis of Z=120 nuclei. 65Zn(238U, X)303122*, E(cm)=275.7 MeV; 40Ca(238U, X)278Cn*, E(cm)=184.9 MeV; 48Ca(238U, X)278Cn*, E(cm)=215.7 MeV; 35Cl(238U, X)273Mt*, E(cm)=204.4 MeV; 32S(238U, X)270Hs*, E(cm)=152.0 MeV; 184W(72Ge, X)256Sg*, E(cm)=178.1 MeV; 27Al(238U, X)265Db*, E(cm)=146.0 MeV; 184W(64Ni, X)248No*, E(cm)=341.0 MeV; 184W(58Ni, X)242No*, E(cm)=250.9, 266.1, 285.1 MeV; 186W(48Ti, X)234Cm*, E(cm)=245.0 MeV; 184W(48Ti, X)232Cm*, E(cm)=190.3, 194.3, 202.2 MeV; 208Pb(16O, X)224Th*, E(cm)=140.0 MeV; 186W(32S, X)218Th*, E(cm)=180.0 MeV; 184W(32S, X)216Th*, E(cm)=153.3 MeV; calculated quasifission and fusion-fission lifetimes, and compared with experimental data. 248Cm(54Cr, X)302120*, E=326 MeV; 244Pu(58Fe, X)302120*, E(cm)=325 MeV; 238U(64Ni, X)302120*, E(cm)=349 MeV; 249Cf(50Ti, X)299120*, E(cm)=273 MeV; 249Bk(50Ti, X)299119*, E(cm)=267 MeV; 248Cm(51V, X)299120*, E(cm)=277 MeV; 249Cf(48Ca, X)297Og*, E(cm)=235 MeV; 249Bk(48Ca, X)297Ts*, E(cm)=239 MeV; 248Cm(48Ca, X)296Lv*, E(cm)=241 MeV; 243Am(48Ca, X)291Mc*, E(cm)=248 MeV; 242Pu(48Ca, X)290Fl*, E(cm)=244 MeV; 209Bi(70Zn, X)279Nh*, E(cm)=349 MeV; 208Pb(70Zn, X)278Cn*, E(cm)=346 MeV; calculated quasifission and fusion-fission lifetimes for the first six failed experiments to find evidence for Z=119 and 120, and the next seven successful experiments. Statistical method within the framework of the dinuclear system (DNS) model.
doi: 10.1103/PhysRevC.103.024311
2021MA57 Phys.Rev. C 104, 024622 (2021) H.C.Manjunatha, P.S.Damodara Gupta, N.Sowmya, L.Seenappa, N.Manjunatha Systematics of heavy ion fusion with entrance channel and deformation parameters NUCLEAR REACTIONS 169Tm(13C, 5n)176Re, E*=59.3 MeV; 165Ho(16O, 5n)176Re, E*=63.3 MeV; 181Ta(9Be, 4n)186Ir, E*=48.5 MeV; 170Eu(30Si, 5n)195Ir, E*=96.5 MeV; 169Tm(16O, 3n)182Ir, E*=47.9 MeV; 187Re(α, n)190Ir, E*=11.7 MeV; 186W(9Be, 5n)190Pt, E*=56.7 MeV; 187Re(9Be, 5n)191Au, E*=50.8 MeV; 197Au(6He, 5n)198Tl, E*=55.2 MeV; 194Pt(6Li, 4n)196Tl, E*=47 MeV; 181Ta(16O, 5n)192Tl, E*=63.7 MeV; 181Ta(19F, 5n)195Pb, E*=63.4 MeV; 208Pb(α, 2n)210Po, E*=27.4 MeV; 198Pt(12C, 5n)205Po, E*=57 MeV; 164Dy(40Ar, 5n)199Po, E*=76.2 MeV; 154Gd(48Ca, 4n)198Po, E*=51.2 MeV; 209Bi(α, 3n)210At, E*=34 MeV; 208Pb(9Li, 5n)212At, E*=54.9 MeV; 197Au(12C, 5n)204At, E*=58.5 MeV; 192Os(19F, 6n)205At, E*=70.8 MeV; 205Tl(9Be, 4n)210At, E*=44.7 MeV; 159Tb(48Ca, 5n)202At, E*=53.6 MeV; 165Ho(40Ar, 4n)201At, E*=47.7 MeV; 209Bi(6Li, 5n)210Rn, E*=60 MeV; 208Pb(9Be, 5n)212Rn, E*=56.7 MeV; 190Os(22Ne, 7n)205Rn, E*=77 MeV; 162Dy(48Ca, 5n)205Rn, E*=48 MeV; 160Gd(50Ti, 5n)205Rn, E*=49.1 MeV; 209Bi(11Be, 4n)216Fr, E*=52.9 MeV; 169Tm(40Ar, 4n)205Fr, E*=47.6 MeV; 205Tl(12C, 4n)213Fr, E*=47.9 MeV; 197Au(18O, 5n)210Fr, E*=53.8 MeV; 165Ho(48Ca, 5n)208Fr, E*=55.8 MeV; 159Tb(50Ti, 4n)205Fr, E*=43.1 MeV; 209Bi(11B, 4n)216Ra, E*=44 MeV; 198Pt(22Ne, 6n)214Ra, E*=64.1 MeV; 174Yb(40Ar, 5n)209Ra, E*=20.9 MeV; 162Dy(50Ti, 3n)209Ra, E*=41.3 MeV; calculated Coulomb interaction parameter, mean fissility, charge and mass asymmetry, deformation parameter β2, and evaporation residue σ for synthesis of the pre-actinide nuclei using advanced statistical model (ASM) and dinuclear system model (DNS) models. Comparison with experimental data. NUCLEAR REACTIONS 209Bi(12C, 6n)215Ac, E*=53.1 MeV; 197Au(22Ne, 5n)214Ac, E*=62.8 MeV; 175Lu(40Ar, 6n)209Ac, E*=68.2 MeV; 208Pb(16O, 3n)221Th, E*=31.5 MeV; 173Yb(48Ca, 4n)217Th, E*=46.6 MeV; 172Yb(48Ca, 4n)216Th, E*=45.7 MeV; 180Hf(40Ar, 4n)216Th, E*=49.4 MeV; 96Zr(124Sn, 4n)216Th, E*=48 MeV; 179Hf(40Ar, 4n)215Th, E*=38.9 MeV; 178Hf(40Ar, 5n)213Th, E*=44.8 MeV; 94Zr(124Sn, 3n)215Th, E*=37.1 MeV; 177Hf(40Ar, 4n)213Th, E*=39.2 MeV; 92Zr(124Sn, 3n)213Th, E*=31.7 MeV; 90Zr(124Sn, 3n)211Th, E*=38.4 MeV; 92Zr(124Sn, n)215Th, E*=23.6 MeV; 182W(32S, 4n)210Th, E*=53.1 MeV; 90Zr(124Sn, n)213Th, E*=22.6 MeV; 181Ta(40Ar, 4n)217Pa, E*=39.8 MeV; 208Pb(22Ne, 4n)226U, E*=37.2 MeV; 180Hf(48Ca, 3n)225U, E*=36.8 MeV; 238U(α, n)241Pu, E*=39.9 MeV; 235U(α, 2n)237Pu, E*=19.8 MeV; 234U(α, 2n)236Pu, E*=19.5 MeV; 233U(α, 2n)235Pu, E*=22.7 MeV; 184W(48Ca, 3n)229Pu, E*=31.2 MeV; 237Np(α, 2n)239Am, E*=21.5 MeV; 207Pb(34S, 3n)238Cf, E*=35.7 MeV; 207Pb(36S, 3n)240Cf, E*=32.1 MeV; 197Au(48Ca, 2n)243Es, E*=32.2 MeV; 238U(16O, 5n)249Fm, E*=50.2 MeV; 208Pb(48Ca, 2n)254No, E*=23.1 MeV; 246Cm(12C, 4n)254No, E*=41.2 MeV; 207Pb(48Ca, 2n)253No, E*=23.6 MeV; 248Cm(13C, 4n)257No, E*=38.7 MeV; 248Cm(12C, 4n)256No, E*=41.8 MeV; 246Cm(13C, 4n)255No, E*=42.3 MeV; 206Pb(48Ca, 2n)252No, E*=24.3 MeV; 244Cm(13C, 4n)253No, E*=41.4 MeV; 204Pb(48Ca, 2n)250No, E*=24, 25.4 MeV; 207Pb(48Ca, 2n)253No, E*=24.2 MeV; 209Bi(48Ca, 2n)255Lr, E*=22.9 MeV; calculated Coulomb interaction parameter, mean fissility, charge and mass asymmetry, deformation parameter β2, and evaporation residue σ for synthesis of the actinide nuclei using advanced statistical model (ASM) and dinuclear system model (DNS) models. Comparison with experimental data. NUCLEAR REACTIONS 208Pb(50Ti, 2n)256Rf, E*=24.3 MeV; 248Cm(16O, 5n)259Rf, E*=53.58 MeV; 209Bi(50Ti, n)258Db, E*=15.8 MeV; 248Cm(19F, 5n)262Db, E*=55.4 MeV; 208Pb(54Cr, n)261Sg, E*=16.1 MeV; 248Cm(22Ne, 5n)265Sg, E*=54.9 MeV; 238U(30Si, 5n)263Sg, E*=40.5 MeV; 209Bi(54Cr, n)262Bh, E*=16.9 MeV; 208Pb(58Fe, n)265Hs, E*=16.1 MeV; 248Cm(26Mg, 5n)269Hs, E*=57 MeV; 238U(34S, 5n)267Hs, E*=57.6 MeV; 209Bi(58Fe, n)266Mt, E*=15.5 MeV; 208Pb(64Ni, n)271Ds, E*=18.1 MeV; 208Pb(62Ni, n)269Ds, E*=15.6 MeV; 209Bi(64Ni, n)272Rg, E*=13.1 MeV; 238U(48Ca, 3n)283Cn, E*=37.8 MeV; 208Pb(70Zn, n)277Cn, E*=10 MeV; 237Np(48Ca, 3n)282Nh, E*=46.9 MeV; 209Bi(70Zn, n)278Nh, E*=16.9 MeV; 244Pu(48Ca, 4n)288Fl, E*=41 MeV; 242Pu(48Ca, 4n)286Fl, E*=42.9 MeV; 240Pu(48Ca, 4n)284Fl, E*=49 MeV; 239Pu(48Ca, 3n)284Fl, E*=46.4 MeV; 243Am(48Ca, 3n)288Mc, E*=45 MeV; 248Cm(48Ca, 4n)292Lv, E*=46.9 MeV; 249Bk(48Ca, 4n)293Ts, E*=65.7 MeV; 249Cf(48Ca, 3n)294Og, E*=38.8 MeV; calculated Coulomb interaction parameter, mean fissility, charge and mass asymmetry, deformation parameter β2, and evaporation residue σ for synthesis of superheavy nuclei using advanced statistical model (ASM) and dinuclear system model (DNS) models. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.024622
2021NA21 Nucl.Phys. A1015, 122306 (2021) A.M.Nagaraja, H.C.Manjunatha, N.Sowmya, L.Seenappa, P.S.Damodara Gupta, N.Manjunatha, S.A.Cecil Raj Heavy particle radioactivity of superheavy element Z = 126 RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C), 228Th(20O), 230U(22Ne), 230Th, 231Pa, 232,233U(24Ne), 234U(26Ne), 234U, 236,238Pu(28Mg), 238Pu(30Mg), 238Pu(32Si), 242Cm(34Si), 306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326126(α), (β+), (SF); analyzed available data; calculated T1/2.
doi: 10.1016/j.nuclphysa.2021.122306
2020MA51 Int.J.Mod.Phys. E29, 2050061 (2020) H.C.Manjunatha, N.Manjunatha, L.Seenappa Investigations on the study of entrance channel effects in synthesis of superheavy elements using Cr-induced fusion reactions NUCLEAR STRUCTURE 232,234,236,238Lv, 235,236,237,238,239Ts, 238,239,240,241,242,243,244Og, 242,243119, 240,241,242,243,244,245,246,247,248,249,250120, 243,245,247,249,251121, 246,247,248,249,250,251,252,253,254122, 252,253,254,255123; calculated compound nucleus formation probability using Cr-induced fusion reactions.
doi: 10.1142/S0218301320500615
2020MA62 Phys.Rev. C 102, 064605 (2020) H.C.Manjunatha, N.Sowmya, N.Manjunatha, P.S.Damodara Gupta, L.Seenappa, K.N.Sridhar, Ganesh, T.Nandi Entrance channel dependent hot fusion reactions for superheavy element synthesis NUCLEAR REACTIONS 208Pb(62Ni, n)269Ds, 251Cf(25Mg, 4n)272Ds, 249,253Bk(26Al, 5n)270Ds/274Ds, 209Bi(64Ni, n)272Rg, 234Th(48Sc, 3n)279Rg, 248Cm(33P, 4n)277Rg, 242Pu(37Cl, 4n)275Rg, 238U(40K, 5n)273Rg, 208Pb(70Zn, n)277Cn, 242Pu(42Ar, 3n)281Cn, 238U(47Ca, 3n)282Cn, 249Bk(33P, 4n)278Cn, 209Bi(70Zn, n)278Nh, 254Cf(31P, 4n)281Nh, 250Cm(37Cl, 4n)283Nh, 252Cf(32P, 4n)280Nh, 253Cf(33P, 4n)282Nh, 249Bk(33S, 5n)277Nh, 244Pu(48Ca, 3n)289Fl, 240Pu(43Ca, 3n)280Fl, 246Cm(36Ar, 4n)278Fl, 243Am(48Ca, 3n)288Mc, 244Pu(46Sc, 3n)287Mc, 246Bk(38Ar, 3n)281Mc, 240Pu(48Sc, 3n)285Mc, 236U(51V, 3n)284Mc, 248Cm(48Ca, 4n)292Lv, 249Cf(36Ar, 3n)282Lv, 240Cm(41Ca, 3n)278Lv, 252Cf(36Ar, 4n)284Lv, 249Bk(48Ca, 4n)293Ts, (48Ca, 3n)294Ts, 243Bk(46Ca, 2n)287Ts, 248Bk(48Ca, 3n)293Ts, 249Cf(48Ca, 3n)294Og, 244Pu(52Cr, 3n)293Og, 252Cf(47Ca, 3n)296Og, 253Cf(40Ca, 5n)288Og, 250Cm(50V, 3n)297119, 239Pu(53Mn, 3n)289119, 249Cf(44Ti, n)292120, (47Ti, n)295120, (50Ti, n)298120, 239Np(64Ni, 2n)301121, 252Cf(48V, 3n)297121, 253Cf(49V, 3n)299121, 225Rn(85Kr, X)310122, 223At(86Rb, n)308122, 239Pa(76Ge, n)314123, 242Np(72Zn, n)313123, 240Np(64Zn, 2n)302123, 232Th(71As, 2n)301123, 242,244Pu(72Zn, n)313124/315124, 227Ac(85Kr, n)311125, 245Bk(58Ni, n)302125, 249Bk(66Ni, n)314125, 247Bk(60Ni, n)305125, 232Th(83Kr, X)315126, (82Kr, X)314126, E not given; Z=5-40, A=10-96 projectiles; Z=72-114, A=180-290 targets; calculated evaporation residue fusion cross sections in 6645 different projectile-target combinations for synthesis of Z=110-126 superheavy nuclei, and their dependence on entrance channel effects of mass asymmetry, charge asymmetry, isospin asymmetry, Coulomb charge, Coulomb interaction parameter, mean fissility, and Businaro-Gallone mass asymmetry; compared with available experimental data. 266,270,272,274,276,278,280Ds, 278,280,282,284,286Cn, 272,274,276,278,280,282Fl, 276,278,280,282,284,286,288,290,292,294Lv, 292,294,296,298,300Og, 286,288,290,292,294,296,298,300,302,304120, 308,310,312,314122, 314,316,318124, 318,320126; calculated evaporation residue cross sections in fusion reactions as function of the mass asymmetry parameter. NUCLEAR REACTIONS 231U(36Ar, X)267Ds, 208Pb(61Ni, X)269Ds, 232U(38Ar, X)270Ds, 249Bk(26Al, X)275Ds, 251Cf(25Mg, X)276Ds, 253Cf(24Mg, X)277Ds, 252Cf(26Mg, X)278Ds, 253,254Bk(26Al, X)279Ds/280Ds, 254Bk(27Al, X)281Ds, 248Cf(26Al, X)274Rg, 231Pa(44Ca, X)275Rg, 239Pu(37Cl, X)276Rg, 236U(41K, X)277Rg, 238U(40K, X)278Rg, 242Pu(37Cl, X)279Rg, 253Cf(27Al, X)280Rg, 248,250Cm(33P, X)281Rg/283Rg, 234Th(48Sc, X)282Rg, 239Np(39K, X)278Cn, 243Pu(36Ar, X)279Cn, 250Cf(30Si, X)280Cn, 248Cm(33S, X)281Cn, 249Bk(33P, X)282Cn, 253Cf(30Si, X)283Cn, 242Pu(42Ar, X)284Cn, 238U(37Ca, X)285Cn, 254Cf(32Si, X)286Cn, 212Bi(67Zn, X)279Nh, 226Ac(54Cr, X)280Nh, 249Bk(33S, X)282Nh, 235U(48Sc, X)283Nh, 252Cf(32P, X)284Nh, 254Cf(31P, X)285Nh, 253Cf(33P, X)286Nh, 250Cm(37Cl, X)287Nh, 219,220Rn(58Ni, X)277Fl/278Fl, 217At(63Cu, X)280Fl, 226Ac(55Mn, X)281Fl, 246Cm(36Ar, X)282Fl, 240Pu(43Ca, X)283Fl, 246Bk(38Ar, X)284Mc, 236U(51V, X)287Mc, 249Pu(48Sc, X)288Mc, 242,244Pu(47Sc, X)289Mc/291Mc, 244Pu(46Sc, X)290Mc, 240,242,243Cm(40Ca, X)280Lv/282Lv/283Lv, 240Cm(41Ca, X)281Lv, 248,249,250,252,253Cf(36Ar, X)284Lv/285Lv/286Lv/288Lv/289Lv, 250Cf(37Ar, X)287Lv, 243Bk(46Ca, X)289Mc, 242Am(49Ti, X)291Mc, 252Bk(42Ca, X)294Mc, 248Bk(48Ca, X)296Mc, 239Pu(53Cr, X)292Og, 253Cf(40Ca, X)293Og, 250Cf(44Ca, X)294Og, 230Ac(65Cu, X)295Og, 244Pu(52Cr, X)296Og, 238U(59Fe, X)297Og, 250Bk(48Sc, X)298Og, 252Cf, 254Bk(47Ca, X)299Og/301Og, 198Pt(91Nb, X)289119, 207Bi(83Kr, X)290119, 241Am(50Cr, X)291119, 248Bk(44Ti, X)292119, 227Ac(66Zn, X)293119, 229Th(65Cu, X)294119, 236U(59Co, X)295119, 243Am(53Cr, X)296119, 238U(60Co, X)298119, 250Cm(50V, X)300119, (51V, X)301119, 209Po(78Kr, 2n)285120, 202Pb(86Sr, 2n)286120, 232U(59Ni, 4n)287120, 209Po(81Kr, 2n)288120, 232Po(58Ni, n)289120, 204Pb(87Sr, n)290120, 228Pu(64Fe, n)291120, 249Cf(44Ti, n)292120, (47Ti, n)295120, (50Ti, n)298120, 244Cm(50Cr, n)293120, 242Am(53Mn, n)294120, 210Bi(87Rb, n)296120, 247Bk(51V, n)297120, 246Cm(54Cr, n)299120, 229Th(72Zn, n)300120, 226Ra(76Ge, n)301120, 250Cm(53Cr, n)302120, 246Bk(53Cr, X)299121, 252Cf(48V, X)300121, 228Ra(73As, X)301121, 250Cm(52Mn, X)302121, 239Np(64Ni, X)303121, 233Pa(71Zn, X)304121, 253Cf(54Cr, n)306122, 230Ra(78Se, n)307122, 223At(86Rb, n)308122, 228Rn(83Kr, 2n)309122, 225Rn(85Kr, X)310122, 226Ac(86As, n)311122, 234Ra(80Se, 2n)312122, 230Rn(84Kr, n)313122, 232Th(71As, n)302123, 240Pu(67Zn, 4n)303123, 214Bi(92Zr, n)305123, 213Pb(94Nb, n)306123, 241Pu(67Cu, n)307123, 214Bi(96Zr, 2n)308123, 228Ra(85Kr, n)312124, 242,244Pu(72Zn, n)313124/315124, 228,230Rn(87Sr, n)314124/316124, 245,246,247Bk(58Ni, X)303125/304125/305125, 247Bk(60Ni, X)307125, 239Np(69Ge, n)308125, 243Am(66Zn, X)309125, 242Am(68Zn, X)310125, 246Cm(65Cu, X)311125, 249Bk(66Ni, X)315125, 232Th(82Kr, X)314126, (83Kr, X)315126, (84Kr, X)316126, (86Kr, X)318126, E not given; calculated fusion evaporation residue σ for suitable projectile-target combinations to synthesize Z=110-126 superheavy nuclei. 208Pb(40Ca, X), (48Ti, X), (52Cr, X), (56Fe, X), (59Ni, X), (65Zn, X), 209Bi(45Ca, X), (51Ti, X), (52Cr, X), (59Ni, X), (65Zn, X), E not given; calculated evaporation residue σ for the synthesis of Z=102-113 elements in cold fusion reactions, and compared with experimental data. 208Pb, 226Ra, 238U, 237Np, 244Pu, 243Am, 247Cm, 247Bk, 251Cf(48Ca, X), E not given; calculated evaporation residue σ for the synthesis of Z=112-118 elements in hot fusion reactions, and compared with experimental data. 232Th(82Kr, X)314126; calculated large evaporation residue cross sections as high as 31 nb. RADIOACTIVITY 283Cn, 279Ds, 275Hs, 271Sg, 267Rf, 263No, 259Fm, 255Cf, 247,251Bk, 243Am, 239Pu, 235Np(α); 251Cm, 247Am, 239Np, 235U(β-); 291Lv, 287Fl, 283Cn, 279Ds, 275Hs, 271Sg, 267Rf, 263No, 259Fm, 255Cf, 247,251Bk, 243Am, 239Pu, 235Np(α); 251Cm, 247Am, 239Np, 235U(β-); 296119, 292Ts, 288Mc, 284Nh, 280Rg, 276Mt, 272Bh, 268Db, 264Lr, 260Md, 256Es, 252Cf, 248Bk, 244Cm, 240Pu, 236Pu(α); 252Bk, 248Cm, 244Am, 236U(β-); 295Og, 291Lv, 287Fl, 283Cn, 279Ds, 275Hs, 271Sg, 267Rf, 263No, 259Fm, 255Cf, 247,251Bk, 243Am, 239Pu, 235Np(α); 251Cm, 247Am, 239Np, 235U(β-); 299120, 295Og, 291Lv, 287Fl, 283Cn, 279Ds, 275Hs, 271Sg, 267Rf, 263No, 259Fm, 255Cf, 247,251Bk, 243Am, 239Pu, 235Np(α); 251Cm, 247Am, 239Np, 235U(β-); predicted decay chains of 283Cn (Z=112), 291Lv (Z=116), 295Og (Z=118), 296119 (Z=119), and 299120 (Z=120).
doi: 10.1103/PhysRevC.102.064605
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