NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = Ganesh Found 11 matches. 2022DA17 Phys.Rev. C 106, 064603 (2022) P.S.Damodara Gupta, N.Sowmya, H.C.Manjunatha, L.Seenappa, T.Ganesh Quasifission barrier of heavy ion fusion reactions leading to the formation of the superheavy nucleus 302120 NUCLEAR REACTIONS 251Cf(56Ti, 3n)304120, E*=36 MeV; 251Cf(57Ti, 4n)304120, E*=47 MeV; 251Cf(58Ti, 5n)304120, E*=60 MeV; 249Bk(58V, 3n)304120, E*=37 MeV; 249Bk(59V, 4n)304120, E*=47 MeV; 249Bk(60V, 5n)304120, E*=59 MeV; 248Cm(59Cr, 3n)304120, E *=36 MeV; 248Cm(60Cr, 4n)304120, E*=46 MeV; 248Cm(61Cr, 5n)304120, E*=57 MeV; 248Cf(45Sc, 3n)290119, E*=39 MeV; 247Bk(50Ti, 3n)294119, E*=36 MeV; 242Cm(51V, 3n)290119, E*=38 MeV; 242Am(54Cr, 3n)293119, E*=37 MeV; calculated evaporation residue σ. 237Th(65Zn, X), 218Po(84Kr, X), E not given; calculated nucleus-nucleus interaction potential from the fusion which leads to 302120 production. 252Cf(50Ti, X), E(cm)=223 MeV; 249Bk(53V, X), E(cm)=229 MeV; 248Cm(54Cr, X), E(cm)=236 MeV; 244Pu(58Fe, X), E(cm)=249 MeV; 239Pa(63Cu, X), E(cm)=260 MeV; 232Th(70Zn, X), E(cm)=281 MeV; 222Rn(80Se, X), E(cm)=309 MeV; 228Ra(74Ge, X), E(cm)=240 MeV; 238U(64Ni, X), E(cm)=267 MeV; calculated quasifission barrier, evaporation residue σ, entrance channel parameters. Investigated the influence of the projectile-target orientation and angular momentum on quasifission barriers. Dinuclear system (DNS) model. Comparison to other theoretical estimations.
doi: 10.1103/PhysRevC.106.064603
2021HA37 Phys.Rev. C 104, 034905 (2021) N.Hatwar, C.R.Singh, S.Ganesh, M.Mishra Bottomonium suppression in PbPb collisions at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.104.034905
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
2016GA01 Nucl.Phys. A947, 38 (2016) pQCD approach to charmonium regeneration in QGP at the LHC
doi: 10.1016/j.nuclphysa.2015.12.004
2015GA08 Phys.Rev. C 91, 034901 (2015) Temperature-dependent formation-time approach for Υ suppression at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.91.034901
2015SI16 Phys.Rev. C 92, 034916 (2015) C.R.Singh, P.K.Srivastava, S.Ganesh, M.Mishra Unified description of charmonium suppression in a quark-gluon plasma medium at RHIC and LHC energies
doi: 10.1103/PhysRevC.92.034916
2014CR04 Nucl.Sci.Eng. 178, 66 (2014) R.Crasta, S.Ganesh, H.Naik, A.Goswami, S.V.Suryanarayana, S.C.Sharma, P.V.Bhagwat, B.S.Shivashankar, V.K.Mulik, P.M.Prajapati Measurement of the 238U(n, γ)239U and 238U(n, 2n)237U Reaction Cross Sections Using a Neutron Activation Technique at Neutron Energies of 8.04 and 11.90 MeV NUCLEAR REACTIONS 238U(n, γ), (n, 2n), E=8.04-11.90 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VII.0, JENDL-4.0, JEFF-3.1/A, CENDL-3.1 libraries.
doi: 10.13182/NSE11-90
2013CR03 Radiochim.Acta 101, 541 (2013) R.Crasta, H.Naik, S.V.Suryanarayana, S.Ganesh, P.M.Prajapati, M.Kumar, T.N.Nathaniel, V.T.Nimje, K.C.Mittal, A.Goswa Measurement of bremsstrahlung-induced reaction cross-section for 93Nb using electron Linac NUCLEAR REACTIONS 93Nb(γ, n), E<10 MeV; 197Au(γ, n), E<12.5 MeV;measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS nuclear model code calculations, available data.
doi: 10.1524/ract.2013.2051
2013GA44 Phys.Rev. C 88, 044908 (2013) Bottomonium suppression at √ SNN=276 TeV using a model based on color screening and gluonic dissociation with collisional damping
doi: 10.1103/PhysRevC.88.044908
2005ES04 Nucl.Instrum.Methods Phys.Res. A540, 412 (2005) K.M.Eshwarappa, Ganesh, K.Siddappa, Y.Kashyap, A.Sinha, P.S.Sarkar, B.K.Godwal Estimation of photoneutron yield from beryllium target irradiated by variable energy microtron-based bremsstrahlung radiation NUCLEAR REACTIONS 9Be(γ, nX), E=8.7 MeV bremsstrahlung; measured thick-target neutron yields. 9Be(γ, nX), E=8-12 MeV bremsstrahlung; calculated thick-target neutron yields.
doi: 10.1016/j.nima.2004.12.001
2004MB15 Nucl.Instrum.Methods Phys.Res. B215, 4 (2004) M.L.Mallikarjuna, S.B.Appaji Gowda, K.E.Ganesh, R.Gowda, T.K.Umesh A method to determine the K-shell photoeffect cross sections of some rare earth elements NUCLEAR REACTIONS La, Ce, Pr, Nd, Sm, Gd, Dy, Ho, Er(γ, E), E<84.3 keV; measured reaction products; deduced K-shell photoeffect σ.
doi: 10.1016/s0168-583x(03)01717-8
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