NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 29, 2024.

Search: Author = T.A.Jose

Found 7 matches.

Back to query form



2023SA51      Int.J.Mod.Phys. E32, 2350047 (2023)

K.P.Santhosh, D.T.Akrawy, T.A.Jose, Ali H.Ahmed, H.Hassanabadi, S.S.Hosseini, V.Zanganah, L.Sihver

A systematic study of α-decay half-lives for Ac, Th, Pa, U and Np isotopes with A = 205-245 using the modified generalized liquid drop model

RADIOACTIVITY 205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237Ac, 208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239Th, 211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241Pa, 214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243U, 219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245Np(α); calculated T1/2. Comparison with available data.

doi: 10.1142/S0218301323500477
Citations: PlumX Metrics


2022SA26      Phys.Rev. C 105, 054605 (2022)

K.P.Santhosh, T.A.Jose, N.K.Deepak

Probable chances of radioactive decays from superheavy nuclei 290-304120 within a modified generalized liquid drop model with a Q-value-dependent preformation factor

RADIOACTIVITY 290120(α), (74Ge), (75Ga), (76Ge), (77Ge), (78Se), (79Se), (80Se), (81Se), (82Se), (83Br), (84Kr), (85Kr), (86Kr), (87Rb), (88Sr), (89Sr), (90Sr), (91Y), (93Zr), (94Zr), (95Nb), (96Zr), (97Nb), (98Mo), (99Mo), (100Mo), (101Tc), (102Ru), (104Ru), (107Rh), (108Pd), (110Pd), (111Ag), (112Pd), (113Cd), (114Cd), (115Cd), (116Cd), (117In), (119Sn), (120Sn), (121Sn), (122Sn), (123Sb), (124Te), (125Te), (126Te), (127I), (128Xe), (130Xe), (131Xe), (132Xe), (133Cs), (134Ba), (135Cs), (136Ba), (137Ba), (138Ba), (139Ba), (140Ba); 292120(α), (8Be), (77Ge), (78Ge), (79As), (80Se), (81Se), (82Se), (83Br), (84Kr), (85Kr), (86Kr), (87Rb), (88Sr), (89Sr), (90Sr), (91Sr), (93Y), (94Zr), (95Nb), (96Zr), (97Nb), (98Mo), (99Mo), (100Mo), (101Mo), (102Mo), (103Tc), (104Ru), (105Ru), (106Ru), (107Rh), (108Pd), (109Rh), (110Pd), (111Pd), (112Pd), (113Ag), (114Cd), (115Cd), (116Cd), (117In), (118Sn), (119Sn), (120Sn), (121Sn), (122Sn), (123Sb), (124Sn), (125Sb), (126Te), (127Te), (128Te), (129I), (130Xe), (131Xe), (132Xe), (133Xe), (134Xe), (135Cs); 294120(α), (77Ge), (78Ge), (79Ge), (80Ge), (81As), (82Se), (83Br), (84Kr), (85Kr), (86Kr), (87Rb), (88Sr), (89Sr), (90Sr), (91Sr), (92Sr), (93Y), (94Zr), (95Nb), (96Zr), (97Zr), (98Zr), (99Nb), (100Mo), (101Mo), (102Mo), (103Tc), (104Ru), (105Ru), (106Ru), (107Ru), (108Ru), (109Rh), (110Pd), (111Pd), (112Pd), (113Ag), (114Cd), (115Cd), (116Cd), (117Cd), (118Cd), (119In), (120Sn), (121Sn), (122Sn), (123Sn), (124Sn), (125Sb), (126Te), (127Te), (128Te), (129I), (130Te), (131I), (132Xe), (133Xe), (134Xe), (135Cs), (136Ba), (137Ba), (138Ba); 296120(α), (78Ge), (79Ge), (80Ge), (81As), (82Se), (83Se), (84Se), (85Br), (86Kr), (87Rb), (88Sr), (89Sr), (90Sr), (91Sr), (92Sr), (93Sr), (94Sr), (95Nb), (96Zr), (97Zr), (98Zr), (99Nb), (100Mo), (101Mo), (102Mo), (103Mo), (104Mo), (103Tc), (106Ru), (107Ru), (108Ru), (109Rh), (110Pd), (111Rh), (112Pd), (113Pd), (114Pd), (115Ag), (116Cd), (117Cd), (118Cd), (119In), (120Sn), (121Sn), (122Sn), (123Sn), (124Sn), (125Sn), (126Sn), (127Sb), (128Te), (129Te), (130Te), (131I), (132Xe), (133Xe), (134Xe), (135Xe), (136Xe), (137Cs), (138Ba), (139La); calculated Q values, T1/2 for cluster decays modified generalized liquid drop model with a Q-value-dependent preformation factor; deduced probable heavy cluster emitted from each isotope of 290,292,294,296120 with half-life comparable to α-decay T1/2, and probable chances of heavy-cluster decay with minimum half-life.

RADIOACTIVITY 298120(α), (77Ga), (78Ge), (79Ge), (80Ge), (81As), (82Se), (83Se), (84Se), (85Br), (86Kr), (87Kr), (88Kr), (89Rb), (90Sr), (91Sr), (92Sr), (93Sr), (94Sr), (95Nb), (96Zr), (97Zr), (98Zr), (99Zr), (100Zr), (101Nb), (102Mo), (103Mo), (104Mo), (105Tc), (106Ru), (107Ru), (108Ru), (109Ru), (110Ru), (111Rh), (112Pd), (113Pd), (114Pd), (116Cd), (117Cd), (118Cd), (119Cd), (120Cd), (122Sn), (123Sn), (124Sn), (125Sn), (126Sn), (128Te), (129Sb), (130Te), (131Te), (132Te), (134Xe), (135Xe), (136Xe), (137Cs), (138Ba), (140Ba), (141La); 300120(α), (80Ge), (81As), (82Se), (83As), (84Se), (85Se), (86Kr), (87Kr), (88Kr), (89Kr), (90Kr), (91Rb), (92Sr), (93Sr), (94Sr), (95Rb), (96Zr), (97Zr), (98Zr), (99Zr), (100Zr), (101Nb), (102Mo), (103Mo), (104Mo), (105Mo), (106Mo), (107Tc), (108Ru), (109Ru), (110Ru), (111Rh), (112Pd), (113Pd), (114Pd), (115Pd), (116Pd), (117Ag), (118Cd), (119Cd), (120Cd), (121In), (123Sn), (124Sn), (125Sn), (126Sn), (127Sn), (128Sn), (129Sb), (130Te), (131Te), (132Te), (133I), (135I), (136Cs), (137Cs), (138Ba), (139Ba), (140Ba), (141Ba); 302120(α), (80Ge), (82Ge), (83As), (84Se), (85Se), (86Se), (87Kr), (88Kr), (89Kr), (90Kr), (91Rb), (92Sr), (93Sr), (94Sr), (95Rb), (96Sr), (97Zr), (98Zr), (99Zr), (100Zr), (101Zr), (102Zr), (103Nb), (104Mo), (105Mo), (106Mo), (107Tc), (108Ru), (109Ru), (110Ru), (111Ru), (112Ru), (113Rh), (114Pd), (115Pd), (116Pd), (117Ag), (118Cd), (119Cd), (120Cd), (121Cd), (122Cd), (123In), (124Sn), (125Sn), (126Sn), (127Sn), (128Sn), (129Sb), (130Te), (131Sb), (132Te), (133Te), (134Xe), (135I), (136I), (137Xe), (138Xe), (139Cs), (140Ba), (141Ba), (142Ba), (143La); 304120(α), (80Ge), (82Ge), (83As), (84Se), (85Se), (86Se), (87Br), (88Kr), (89Kr), (90Kr), (91Kr), (92Sr), (93Sr), (94Sr), (95Rb), (96Sr), (97Y), (98Zr), (99Zr), (100Zr), (101Zr), (102Zr), (103Nb), (104Nb), (105Mo), (106Mo), (107Mo), (108Ru), (109Ru), (110Ru), (111Ru), (112Ru), (113Rh), (114Pd), (115Pd), (116Pd), (117Pd), (118Pd), (119Ag), (120Cd), (121Cd), (122Cd), (123In), (124Sn), (125Sn), (126Sn), (127Sn), (128Sn), (129Sn), (130Sn), (131Sb), (132Sn), (133Te), (134I), (135I), (136I), (137Xe), (138Xe), (139Cs), (140Ba), (141Ba), (142Ba), (143Ba); calculated Q values, T1/2 for cluster decays modified generalized liquid drop model with a Q-value-dependent preformation factor; deduced probable heavy cluster emitted from each isotope of 298,300,302,304120 with half-life comparable to α-decay T1/2, and probable chances of heavy-cluster decay with minimum half-life. 290,292,294,296,298,300,302,304120(2α), (8Be); calculated Q values and T1/2 for cluster decays. 290,292,294,296,298,300,302,304120(α), (SF); 286,288,290,292,294,296,298,300Og(α), (SF); 282,284,286,288,290,292,294,296Lv(α), (SF); 278,280,282,284,286,288,290,292Fl(α), (SF); 274,276,278,280,282,284,286,288Cn(α), (SF); 270,272Ds(α), (SF); 268,270Hs(α), (SF); calculated T1/2 and compared to available experimental values.

doi: 10.1103/PhysRevC.105.054605
Citations: PlumX Metrics


2021SA26      Phys.Rev. C 103, 064612 (2021)

K.P.Santhosh, T.A.Jose, N.K.Deepak

Radioactive decay of 288-296Og via heavy cluster emission within a modified generalized liquid drop model with a Q-value-dependent preformation factor

RADIOACTIVITY 288Og(α), (109Rh), (111Pd), (112Pd), (113Ag), (114Cd), (115Cd), (116Cd), (117Cd), (118Cd), (119In), (120Sn), (121Sn), (122Sn), (123Sn), (124Sn), (131I), (138Ba); 289Og(α), (110Pd), (111Pd), (113Pd), (114Cd), (115Cd), (116Cd), (117Cd), (118Cd), (119Sn), (120Sn), (121Sn), (122Sn), (123Sn), (124Sn), (125Sn), (138Ba); 290Og(α), (110Pd), (112Pd), (114Pd), (115Ag), (116Cd), (117Cd), (118Cd), (119In), (120Sn), (121Sn), (122Sn), (123Sn), (124Sn), (131I), (138Ba); 291Og(α), (86Kr), (112Pd), (113Pd), (114Pd), (115Ag), (116Cd), (117Cd), (118Cd), (119Cd), (120Sn), (121Sn), (122Sn), (123Sn), (124Sn), (125Sn), (126Sn), (127Te), (138Ba); 292Og(α), (86Kr), (112Pd), (114Pd), (116Pd), (117Cd), (118Cd), (119Cd), (120Cd), (121In), (122Sn), (123Sn), (124Sn), (125Sn), (126Sn), (129Te), (131I), (136Xe), (138Ba); 293Og(α), (86Kr), (87Kr), (112Pd), (113Pd), (114Pd), (116Cd), (117Cd), (118Cd), (119Cd), (120Cd), (121Sn), (122Sn), (123Sn), (125Sn), (127Sn), (136Xe); 294Og(α), (86Kr), (88Kr), (114Pd), (116Cd), (117Cd), (118Cd), (119Cd), (120Cd), (121In), (122Sn), (123Sn), (125Sn), (127Sn), (136Xe), (138Ba); 295Og(α), (87Kr), (88Kr), (114Pd), (115Pd), (116Pd), (117Cd), (118Cd), (119Cd), (120Cd), (121Cd), (122Sn), (123Sn), (135Xe); 296Og(α), (88Kr), (116Pd), (118Cd), (119Cd), (120Cd), (121Cd), (122Cd), (123In), (124Sn), (125Sn), (126Sn), (127Sn), (129Sb), (131Te), (136Xe), (139Ba), (140Ba), (141Ba), (142Ba); calculated Q values, T1/2 for clusters and α decays, branching ratios, comparable half-lives for some of the cluster and α decays in Table II, comparison of alpha decay half-life from parent nuclei calculated with present model with various theoretical models and with available experimental data for 294Og α decay. 288,289,290,291,292,294Og(138Ba); 292,293,296Og(136Ba); 295Og(135Xe); 292,293,294,296Og(136Xe); deduced as most probable heavy cluster decays with least half-life among all splitting. Modified generalized liquid drop model with the Q value dependent preformation factor.

doi: 10.1103/PhysRevC.103.064612
Citations: PlumX Metrics


2021SA34      Phys.Rev. C 104, 024617 (2021)

K.P.Santhosh, C.Nithya, T.A.Jose

Decay modes of superheavy nuclei using a modified generalized liquid drop model and a mass-inertia-dependent approach for spontaneous fission

RADIOACTIVITY 253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268Rf, 258,259,260,261,262,263,264,265,266,267,268,269,270,271,272Sg, 263,264,265,266,267,268,269,270,271,272,273,274,275,276,277Hs, 267,268,269,270,271,272,273,274,275,276,277,278,279,280,281Ds, 276,277,278,279,280,281,282,283,284,285Cn, 284,285,286,287,288,289Fl, 289,290,291,292,293Lv, 293,294,295Og(α), (SF); 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270Db, 260,261,262,263,264,265,266,267,268,269,270,271,272,273,274Bh, 265,266,267,268,269,270,271,272,273,274,275,276,277,278,279Mt, 272,273,274,275,276,277,278,279,280,281,282,283Rg, 278,279,280,281,282,283,284,285,286,287Nh, 287,288,289,290,291Mc, 291,292,293,294Ts(α), (SF); calculated α decay and SF decay T1/2 of superheavy nuclei using modified generalized liquid drop model (MGLDM) with the proximity 77 parametrization for α decay, and a mass-inertia-dependent approach for spontaneous fission. Comparison with available experimental T1/2.

doi: 10.1103/PhysRevC.104.024617
Citations: PlumX Metrics


2020SA23      Phys.Rev. C 101, 064610 (2020)

K.P.Santhosh, D..Akrawy, H.Hassanabadi, Al.H.Ahmed, T.A.Jose

α-decay half-lives of lead isotopes within a modified generalized liquid drop model

RADIOACTIVITY 178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220Pb(α); calculated half-lives using modified generalized liquid drop model (MGLDM) with Akrawy, Royer, AKRE, and modified RenB formulas, and experimental Q(α) values. Comparison with available experimental half-lives, and with predicted half-lives in Coulomb and proximity potential model.

doi: 10.1103/PhysRevC.101.064610
Citations: PlumX Metrics


2019SA33      Phys.Rev. C 99, 064604 (2019)

K.P.Santhosh, T.A.Jose

Half-lives of cluster radioactivity using the modified generalized liquid drop model with a new preformation factor

RADIOACTIVITY 220Ra, 225Np(12C); 221Fr, 221,222,223,224,226Ra, 225Ac, 225,227Np, 224,226,228,229Th, 230U(14C); 221,222,223Ra, 224,226Th(15N); 220Ra, 224Th, 225,227Np(16O); 225Ac(17N); 227Np(17O); 222,223Ra, 225Ac, 226Th, 227,229Np(18O); 224,226Ra, 230U, 228Th, 231Np(20O); 229Th(21O); 230U(21F); 231Pa(22O); 230U, 231,233Np(22Ne); 229Th, 231Pa, 232U(23F); 224,226,228,229,230,232Th, 231Pa, 230,232,233,234,235U, 233Np, 234,236Pu(24Ne); 232Pa, 233,234Np(25Ne); 232Th, 234,236U(26Ne); 231,232Pa, 233,234U, 234,236Pu(27Na); 231,232Pa, 230,232,233,234,235,236U, 234,235,236Np, 234,236,238Pu, 237,238Am, 238Cm(28Mg); 235U, 235,236Np, 237Pu, 237,238Am(29Mg); 234,236Pu(29Al); 236,237Np, 236U, 238Pu, 239Am, 240Cm(30Mg); 237Pu(30Al); 238Pu(31Al); 230,232U, 237Np, 234,236,237Pu, 237,238,239Am, 238,239,240,241,242Cm, 242Cf(32Si); 238,239,240,241Am, 242Cf(33Si); 240Pu, 239,240,241Am, 240,242,243,244Cm, 242,244Cf(34Si); 242Cf(36S); 246Cf(38S); 249Cf(42S); 249,251Cf(46Ar); 249Cf(48Ca), (50Ca); calculated cluster decay half-lives using modified generalized liquid drop model. Comparison with available experimental values, and with other theoretical model predictions.

doi: 10.1103/PhysRevC.99.064604
Citations: PlumX Metrics


2019SA53      Nucl.Phys. A992, 121626 (2019)

K.P.Santhosh, T.A.Jose

Alpha and cluster decay using Modified Generalized Liquid Drop Model with iso-spin dependent pre-formation factor

doi: 10.1016/j.nuclphysa.2019.121626
Citations: PlumX Metrics


Back to query form