NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = G.Shanmugam Found 19 matches. 2005SH42 Phys.Rev. C 72, 034310 (2005) G.Shanmugam, S.Sudhakar, S.Niranjani Role of shapes in the identification of superheavy nuclei RADIOACTIVITY 198,200,202,204,206Po, 204,206,208,210,212Rn, 222,224,226Ra, 226,228,230,232Th, 230,232,234,236,238U, 236,238,240,242,244Pu, 240,242,244,246,248Cm, 250,252Cf, 254,256Fm, 271Sg, 272Bh, 275Hs, 275,276Mt, 279Ds, 279,280Rg, 282,283,285Cn, 283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og(α); calculated Qα, T1/2, deformation parameters.
doi: 10.1103/PhysRevC.72.034310
2004AR11 Phys.Rev. C 69, 054313 (2004) P.Arumugam, G.Shanmugam, S.K.Patra Giant dipole resonance and Jacobi transition with exact treatment of fluctuations NUCLEAR STRUCTURE 45Sc, 90Zr, 92Mo, 120Sn, 184Hg, 208Pb; calculated GDR energies, widths at finite temperature and spin, role of Jacobi transition. Nilsson-Strutinsky approach, Landau theory, comparison with data.
doi: 10.1103/PhysRevC.69.054313
2001SH24 Phys.Rev. C63, 064311 (2001) G.Shanmugam, V.Ramasubramanian, S.N.Chintalapudi Jacobi Shape Transition in fp Shell Nuclei NUCLEAR STRUCTURE 44Ti, 48Cr, 52Fe, 56Ni; calculated deformation vs spin; deduced Jacobi shape transition features. Cranked Nilsson-Strutinsky method.
doi: 10.1103/PhysRevC.63.064311
2001SH43 Pramana 57, 223 (2001) Inclusion of Temperature Dependent Shell Corrections in Landau Theory for Hot Rotating Nuclei NUCLEAR STRUCTURE 80Zr; calculated deformation vs temperature, spin. Temperature-dependent shell corrections, Landau theory.
doi: 10.1007/s12043-001-0180-z
2000SH22 Phys.Rev. C62, 014302 (2000) Shape Transitions in Hot Rotating Strontium and Zirconium Isotopes NUCLEAR STRUCTURE 84Zr; calculated pairing gap parameter vs temperature and spin. 84Sr; calculated moment of inertia vs temperature and spin. 76Sr, 80Zr; calculated deformation vs temperature and spin. Landau theory of phase transitions.
doi: 10.1103/PhysRevC.62.014302
1999SH44 Pramana 53, 443 (1999) Distinction between Pre-Formed Cluster Emission and Heavy Ion Decay by Fission
doi: 10.1007/s12043-999-0012-0
1999SH45 Pramana 53, 457 (1999) G.Shanmugam, V.Ramasubramanian, P.Arumugam Rotational Co-Existence in Selenium Isotopes NUCLEAR STRUCTURE 72,73,74Se; calculated rotational bands energies; deduced shape coexistence features. Cranked Nilsson-Strutinsky approach.
doi: 10.1007/s12043-999-0015-x
1999SH48 Pramana 53, 635 (1999) Cubic Potential Models for Cluster Radioactivity
doi: 10.1007/s12043-999-0042-7
1995SH16 Phys.Rev. C51, 2616 (1995) G.Shanmugam, G.M.C.Vigila Bai, B.Kamalaharan Cluster Radioactivities from an Island of Cluster Emitters RADIOACTIVITY 114,115,116,117,118,119,120Ba, 120,121La(α), (12C); 118,120,121,122,123,124Ce(α)(16O); 122,123Nd(α), (16O); 125Nd, 127,128Sm(α), (28Si); calculated α-, cluster-decay T1/2. Cube potential in overlapping region.
doi: 10.1103/PhysRevC.51.2616
1995SH26 Phys.Rev. C52, 1443 (1995) G.Shanmugam, K.Sankar, K.Ramamurthi Structure of Hot Rotating s-d Shell Nuclei NUCLEAR STRUCTURE 20Ne, 28Si, 24Mg, 40Ca; calculated shape evolution vs temperature with, without thermal fluctuations. Hot rotating nuclei, Landau phase transition theory.
doi: 10.1103/PhysRevC.52.1443
1990SH01 Phys.Rev. C41, 1184 (1990) Role of Deformation in Exotic Decay Studies RADIOACTIVITY 221Fr, 221,222,223,224,226Ra(14C); 230Th, 231Pa, 232,233,234U(24Ne); 222Th, 234U(26Ne); 234U, 238Pu(28Mg); 237Np, 238Pu(30Mg); 238Pu(32Si); 241Am(34Si); calculated T1/2 relative to α-decay; deduced deformation role. Yukawa-plus-exponential potential.
doi: 10.1103/PhysRevC.41.1184
1990SH06 Phys.Rev. C41, 1742 (1990) Exotic Decay Model and Alpha Decay Studies NUCLEAR STRUCTURE A=152-242; calculated exotic decay characteristics, T1/2, charge to mass ratio.
doi: 10.1103/PhysRevC.41.1742
1989SH12 Phys.Rev. C39, 1623 (1989) Isovector Giant Dipole Resonance in Hot Rotating Light Nuclei in the Calcium Region NUCLEAR STRUCTURE 40,42Ca, 46Ti; calculated isovector GDR energy vs temperature. Hot rotating nuclei.
doi: 10.1103/PhysRevC.39.1623
1989SH22 Phys.Rev. C40, 1273 (1989) Nuclear Molecular Configurations in Heavy Ion Collisions NUCLEAR REACTIONS 12C(12C, X), 28Si(28Si, X), 24Mg(24Mg, X), 40Ca(40Ca, X), 4He(24Mg, X), (14C, X), 16O(12C, X), E not given; calculated molecular configuration energy vs neck diameter. Compound nuclei, rotating liquid drop, model parametrization.
doi: 10.1103/PhysRevC.40.1273
1988SH04 Phys.Rev. C37, 853 (1988) Effect of Rotation on the Isovector Giant Dipole Resonance in Certain Calcium Isotopes NUCLEAR STRUCTURE 40,42,43,44Ca; calculated isovector GDR properties; deduced rotation effects. NUCLEAR REACTIONS 40,42,43,44Ca(γ, X), E=15-35 MeV; calculated photoabsorption σ(E); deduced rotation effects.
doi: 10.1103/PhysRevC.37.853
1988SH29 Phys.Rev. C38, 1377 (1988) Application of a Cubic Barrier in Exotic Decay Studies RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 231Pa, 232,233U(24Ne); calculated T1/2 relative to α-decay. Cubic barrier method.
doi: 10.1103/PhysRevC.38.1377
1986SH19 Phys.Rev. C34, 317 (1986) G.Shanmugam, K.Ramamurthi, B.Kamalaharan Giant Quadrupole Resonance in Rotating Light Nuclei in the Calcium Region NUCLEAR STRUCTURE 43,40Ca, 36S, 40Ar; calculated vibrational spectrum parameter dependence. Fermi liquid drop model.
doi: 10.1103/PhysRevC.34.317
1982SH09 Phys.Scr. 25, 607 (1982) Yrast Lines and Fusion Bands of 40,42Ca and 46Ti NUCLEAR STRUCTURE 40,42Ca, 46Ti; calculated yrast lines; deduced relative position to fusion bands. Microscopic Mottelson-Nilsson method.
doi: 10.1088/0031-8949/25/5/005
1981SH14 Phys.Scr. 24, 17 (1981) Application of the Mottelson-Nilsson Method for the Study of Yrast Traps in Light Nuclei NUCLEAR STRUCTURE 36S, 40Ar, 44Ca; calculated ground state energy vs deformation parameters, yrast lines; deduced equilibrium shapes. Microscopic Mottelson-Nilsson model, cranked triaxial Hamiltonian.
doi: 10.1088/0031-8949/24/1A/003
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