NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.K.Jain Found 13 matches. 2023JA02 Nucl.Phys. A1031, 122597 (2023) A.Jain, P.K.Sharma, S.K.Jain, J.K.Deegwal, G.Saxena Cluster radioactivity in trans-lead region: A systematic study with modified empirical formulas RADIOACTIVITY 221Fr, 221,222,223Ra, 223Ac(14C), 223Ac(15N), 224Ra, 225Ac, 226Ra, 226Th(14C), 228Th(20O), 230Th(24Ne), 230U(22Ne), 231Pa(24Ne), 232Th(24Ne), (26Ne), 232U(24Ne), (28Mg), 233U(24Ne), (25Ne), (28Mg), 234U(24Ne), (26Ne), (28Mg), 235U(24Ne), (25Ne), (28Mg), (29Mg), 236U(24Ne), (26Ne), (28Mg), (30Mg), 236Pu(28Mg), 237Np(30Mg), 238Pu(28Mg), (30Mg), (32Si), 240Pu, 241Am, 242Cm(34Si), 216Rn(8Be), 222Fr(14B), 221Ra(13C), 223Ra(15C), 222Ac(14N), (15N), (16N), (17N), 224Th(16O), 225Th(17O), 226Th(18O), 227Th(19O), 228Th(20O), 229Th(21O), 230Th(22O), 231Th(23O), 228Pa(20F), 229Pa(21F), 231Pa(23F), 231U(23Ne), (25Ne); calculated T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2022.122597
2022SH29 Phys.Scr. 97, 045307 (2022) R.Sharma, A.Jain, P.K.Sharma, S.K.Jain, G.Saxena A comprehensive study of decay modes associated with Pb isotopes RADIOACTIVITY 176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,205Pb(β+), (EC), 209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266Pb(β-), 178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193Pb(α); calculated T1/2. Comparison with available data.
doi: 10.1088/1402-4896/ac607c
2021JA09 Hyperfine Interactions 242, 60 (2021) A.Jain, R.Sharma, S.K.Jain, P.K.Sharma, G.Saxena Cluster radioactivity in 294, 296Og RADIOACTIVITY 294,296Og(α), (8Be), (12C), (14C), (16O), (18O), (20O), (22Ne), (24Ne), (26Mg), (28Mg), (30Si), (32Si), (34Si), (36S), (38S), (40Ar), (42Ar), (44Ar), (46Ca), (48Ca), (50Ca), (52Ti), (54Ti), (56Cr), (58Cr), (60Cr), (62Fe), (64Fe), (66Ni), (68Ni), (70Ni), (72Zn), (74Ge), (76Zn), (78Ge), (80Ge), (82Ge), (84Se), (86Kr), (88Kr), (90Sr), (92Kr), (94Sr), (96Zr), (98Zr), (100Mo), (102Mo); calculated T1/2. Comparison with available data.
doi: 10.1007/s10751-021-01748-0
2021SH29 Int.J.Mod.Phys. E30, 2150070 (2021) R.Sharma, A.Jain, M.Kaushik, S.K.Jain, G.Saxena Structural properties of nuclei with semi-magic number N(Z)=40 NUCLEAR STRUCTURE 56S, 58Ar, 60Ca, 62Ti, 64Cr, 66Fe, 68Ni, 70Zn, 72Ge, 74Se, 76Kr, 78Sr, 80Zr, 82Mo, 84Ru, 86Pd, 78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124Zr; calculated binding energies, deformation parameters.
doi: 10.1142/S0218301321500701
2021SH43 Hyperfine Interactions 242, 35 (2021) R.Sharma, A.Jain, S.K.Jain, G.Saxena Magicity in the nuclei with N = 32 and 34 NUCLEAR STRUCTURE 46,48Si, 48,50S, 50,52Ar, 52,54Ca, 54,56Ti, 56,58Cr, 58,60Fe, 60,62Ni, 62,64Zn, 64,66Ge, 66,68Se, 68,70Kr; analyzed available data; calculated potential energy surfaces, quadrupole deformation parameters, two proton shell gap, isotopic shift using relativistic mean-field (RMF) approach with density-dependent meson-nucleon couplings using DD-ME2 parameter.
doi: 10.1007/s10751-021-01751-5
2021SI02 Nucl.Phys. A1006, 122066 (2021) U.K.Singh, R.Sharma, P.K.Sharma, M.Kaushik, S.K.Jain, G.Saxena Structural properties and α-decay chains of transfermium nuclei (101 ≤ Z ≤ 110) RADIOACTIVITY 235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287Md, 238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288No, 241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289Lr, 243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290Rf, 245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291Db, 248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292Sg, 250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293Bh, 253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294Hs, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295Mt, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296Ds(α), (SF); calculated potential energy surfaces (PESs), occupancies of neutron single particle states, rms α-decay T1/2, T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.122066
2020KU26 Int.J.Mod.Phys. E29, 2050068 (2020) M.Kumawat, G.Saxena, M.Kaushik, S.K.Jain, J.K.Deegwal, M.Aggarwal Novel feature of doubly bubble nuclei in 50 ≤ Z(N) ≤ 82 region along with magicity and weakly bound structure NUCLEAR STRUCTURE Z=50-82; calculated the separation energies, s.p. energies, pairing energies, proton and neutron density profiles along with deformations of even-even nuclei using the Relativistic Mean-Field (RMF) approach; deduced central density depletion in both proton and neutron named as doubly bubble nuclei.
doi: 10.1142/S0218301320500688
2020SI27 Nucl.Phys. A1004, 122035 (2020) U.K.Singh, P.K.Sharma, M.Kaushik, S.K.Jain, D.T.Akrawy, G.Saxena Study of decay modes in transfermium isotopes RADIOACTIVITY 245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260Md, 250,251,252,253,254,255,256,257,258,259,260,261,262No, 252,253,254,255,256,257,258,259,260,261,262,263,264,265,266Lr, 253,254,255,256,257,258,259,260,261,262,263,264,265Rf, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270Db, 258,259,260,261,262,263,264,265,266,267,268,269,270,271Sg, 260,261,262,263,264,265,266,267,268,269,270,271,272,273,274Bh, 263,264,265,266,267,268,269,270,271,272,273,274,275,276,277Hs, 266,267,268,269,270,271,272,273,274,275,276,277,278Mt(EC), (β-), (α), (SF); calculated T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.122035
2019SA02 Phys.Lett. B 788, 1 (2019) G.Saxena, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Bubble structure in magic nuclei NUCLEAR STRUCTURE 12,13,14,15,16,17,18,19,20,21,22,23,24O, 34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70Ca, 48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98Ni, 80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150Zr, 78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126Sn, 178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262Pb, 251Fr, 299Mc, 302Og, 22Si, 34Si, 46Ar, 56S, 58Ar, 184Ce, 347119, 292120, 341Nh; calculated charge and matter densities, single particle levels and depletion fraction (DF) across the periodic chart; deduced that the central depletion is correlated to shell structure and occurs due to unoccupancy in s-orbit (2s, 3s, 4s) and inversion of (2s, 1d) and (3s, 1h) states in nuclei upto Z less or equal to 82. Bubble effect in superheavy region is a signature of the interplay between the Coulomb and nn-interaction where the depletion fraction is found to increase with Z (Coulomb repulsion) and decrease with isospin.
doi: 10.1016/j.physletb.2018.08.076
2018KU17 Can.J.Phys. 96, 1413 (2018) M.Kumawat, G.Saxena, M.Kaushik, R.Sharma, S.K.Jain Description of nuclei with magic number Z (N) = 6 NUCLEAR STRUCTURE Z=6, N=6; calculated ground state properties of entire chains of isotopes (isotones) with Z (N) = 6 including even and odd mass nuclei using relativistic mean-field plus BCS, including quadrupole deformation, binding energy, separation energy, single particle energy, root mean squared radii, along with charge and neutron density profile. Comparison with available data.
doi: 10.1139/cjp-2017-1013
2018SA44 Int.J.Mod.Phys. E27, 1850074 (2018) G.Saxena, U.K.Singh, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Distinct ground state features and the decay chains of Z=121 superheavy nuclei NUCLEAR STRUCTURE Z=121; calculated separation energies, shell corrections, deformation parameters, radial variation of charge density and neutron density using RMF+BCS approach. RADIOACTIVITY 293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312121(α); calculated Q-values, T1/2. Comparison with available data.
doi: 10.1142/S021830131850074X
2017SA69 Int.J.Mod.Phys. E26, 1750072 (2017) G.Saxena, M.Kumawat, M.Kaushik, U.K.Singh, S.K.Jain, S.Somorendro Singh, M.Aggarwal Implications of occupancy of 2s1/2 state in sd-shell within RMF+BCS approach NUCLEAR STRUCTURE 22C, 22,24O, 34,36Ca, 26S, 36S, 56S, 22,34,48Si; calculated quadrupole deformation parameters, neutron single particle states, neutron density. Comparison with available data.
doi: 10.1142/S0218301317500720
2017SA70 Phys.Lett. B 775, 126 (2017) G.Saxena, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Two-proton radioactivity with 2p halo in light mass nuclei A = 18-34 NUCLEAR STRUCTURE 19Mg, 22Si, 26S, 30Ar, 34Ca; calculated variation of charge density, charge radii, RMF potential energy, centrifugal barrier energy for proton resonant states; deduced 2-proton halo.
doi: 10.1016/j.physletb.2017.10.055
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