NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.M.Sharma Found 39 matches. 2015RO13 Eur.Phys.J. A 51, 73 (2015) R.Rodriguez-Guzman, L.M.Robledo, M.M.Sharma Microscopic description of quadrupole collectivity in neutron-rich nuclei across the N = 126 shell closure NUCLEAR STRUCTURE 182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216Nd, 184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Sm, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220Gd, 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Dy, 190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224Er, 192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226Yb, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228Hf, 196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230W; calculated gs quadrupole deformation, intrinsic deformation, energy potential surfaces, 2n separation energy, mass excess, neutron, proton single-particle energy, J, π using mean field and beyond with Gogny energy density functionals.
doi: 10.1140/epja/i2015-15073-4
2009SA34 J.Phys.(London) G36, 115103 (2009) A.A.Saldanha, A.R.Farhan, M.M.Sharma Superheavy nuclei with the vector self-coupling of the ω-meson in relativistic mean-field theory
doi: 10.1088/0954-3899/36/11/115103
2009SH01 Nucl.Phys. A816, 65 (2009) The breathing-mode giant monopole resonance and the surface compressibility in the relativistic mean-field theory NUCLEAR STRUCTURE 40,48Ca, 90Zr, 120Sn, 208Pb; calculated isoscalar giant monopole resonance energy using relativistic mean-field theory.
doi: 10.1016/j.nuclphysa.2008.11.006
2008HA13 Nucl.Phys. A803, 159 (2008) Sigma-omega meson coupling and properties of nuclei and nuclear matter NUCLEAR STRUCTURE 16O, 40,48Ca, 76Ni, 90Zr, 100,116,124,132Sn, 202,208,214Pb; calculated binding energies and charge radii of spherical nuclei. 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; calculated binding energies. 202,208,214Pb; calculated charge radii and isotopic shifts. 36,38,40,42Si, 80,86,88Sr, 108,110Mo, 120Xe, 174Yb; calculated binding energies and quadrupole deformation. 90Zr, 120Sn, 208Pb; calculated GMR energies. Lagrangian model using relativistic mean field theory meson coupling.
doi: 10.1016/j.nuclphysa.2008.02.296
2006FA04 Phys.Rev. C 73, 045803 (2006) Strength of nuclear shell effects at N = 126 in the r-process region NUCLEAR STRUCTURE Z=36-72; calculated two-neutron separation energies for even-even nuclides near neutron shell closures; deduced shell effects. Relativistic mean-field approach, astrophysical implications discussed.
doi: 10.1103/PhysRevC.73.045803
2005SH19 Phys.Rev. C 71, 054310 (2005) M.M.Sharma, A.R.Farhan, G.Munzenberg α-decay properties of superheavy elements Z = 113-125 in the relativistic mean-field theory with vector self-coupling of ω meson RADIOACTIVITY 307,308125, 303,304123, 299,300121, 295,296119, 291,292Ts, 287,288Mc, 283,284Nh, 279,280Rg, 275,276Mt, 272Bh(α); calculated Qα, β2, T1/2. Relativistic mean-field theory with vector self-coupling of ω meson.
doi: 10.1103/PhysRevC.71.054310
2003FA13 Nucl.Phys. A719, 221c (2003) Current status of nuclear shell effects near the r-process path
doi: 10.1016/S0375-9474(03)00922-9
2003OB04 Nucl.Phys. A719, 283c (2003) H.Oberhummer, A.Csoto, M.Fairbairn, H.Schlattl, M.M.Sharma Temporal variation of coupling constants and nucleosynthesis
doi: 10.1016/S0375-9474(03)00933-3
2002SH11 Phys.Rev. C65, 044301 (2002) Nuclear Shell Effects Near the r-Process Path in the Relativistic Hartree-Bogoliubov Theory NUCLEAR STRUCTURE Zn, Pd, Ru, Mo, Zr, Sr, Kr; calculated two-neutron separation energies, single-particle levels; deduced shell effects. 124Zr; calculated neutron single-particle levels. 120Zr; calculated spin-orbit potential. Relativistic Hartree-Bogoliubov theory.
doi: 10.1103/PhysRevC.65.044301
2001SH29 Nucl.Phys. A688, 353c (2001) Nuclear Shell Effects Near the r-Process Path NUCLEAR STRUCTURE Zn, Mo, Zr, Sr, Kr; calculated mass, 2-neutron separation energy. Comparison with data, effects of nuclear potential discussed.
doi: 10.1016/S0375-9474(01)00726-6
2000SH16 Phys.Rev. C61, 054306 (2000) M.M.Sharma, A.R.Farhan, S.Mythili Shell Effects in Nuclei with Vector Self-Coupling of the ω Meson in the Relativistic Hartree-Bogoliubov Theory NUCLEAR STRUCTURE Ni, Sn; calculated binding energies, two-neutron separation energies; deduced shell effects. 58,80Ni, 102,134Sn; calculated neutron single-particle level energies. Relativistic mean-field approach, several models compared.
doi: 10.1103/PhysRevC.61.054306
1999SH16 Phys.Rev. C59, 1379 (1999) M.M.Sharma, S.Mythili, A.R.Farhan Carbon Isotopes Near Drip Lines in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 10,12,14,16,18,22,24C; calculated binding energies, deformations, radii, single-particle levels. Relativisitic mean-field theory, meson scalar, vector self-coupling.
doi: 10.1103/PhysRevC.59.1379
1998LA02 Nucl.Phys. A628, 221 (1998) G.A.Lalazissis, A.R.Farhan, M.M.Sharma Light Nuclei Near Neutron and Proton Drip Lines in Relativistic Mean-Field Theory NUCLEAR STRUCTURE 18,20,22,24,26,28,30,32,34,36,38Ne, 20,22,24,26,28,30,32,34,36,38,40,42,44Mg, 22,24,26,28,30,32,34,36,38,40,42,44,46Si, 26,28,30,32,34,36,38,40,42,44,46,48,50,52,54,56S, 34,36,38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74Ti, 38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80Cr, 28,30,32,34,36,38,40,42,44,46,48,50,52,54,56,58,60Ar; calculated binding energies, radii, densities, deformation, other ground-state properties. Relativistic mean-field theory.
doi: 10.1016/S0375-9474(97)00630-1
1998RA08 Phys.Rev. C57, 2031 (1998) T.Rauscher, R.Bieber, H.Oberhummer, K.-L.Kratz, J.Dobaczewski, P.Moller, M.M.Sharma Dependence of Direct Neutron Capture on Nuclear-Structure Models NUCLEAR STRUCTURE 124,126,128,130,132,134,136,138,140,142,144Sn, 208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238Pb; calculated neutron capture σ. Several structure models compared.
doi: 10.1103/PhysRevC.57.2031
1996LA03 Nucl.Phys. A597, 35 (1996) G.A.Lalazissis, M.M.Sharma, P.Ring Rare-Earth Nuclei: Radii, isotope-shifts and deformation properties in the relativistic mean-field theory NUCLEAR STRUCTURE 130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164Sm, 138,140,142,144,146,148,150,152,154,156,158,160,162,164,166Gd, 142,144,146,148,150,152,154,156,158,160,162,164,166,168Dy, 142,144,146,148,150,152,154,156,158,160,162,164,166,168,170Er, 154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Yb; calculated binding energy, charge, neutron radii, isotope shifts, deformation related features. Relativistic mean field theory.
doi: 10.1016/0375-9474(95)00436-X
1996LA24 Nucl.Phys. A608, 202 (1996) G.A.Lalazissis, M.M.Sharma, P.Ring, Y.K.Gambhir Superheavy Nuclei in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE Z=102-118; calculated two-nucleon separation energies, α-decay T1/2, β2, β4 deformations. Binding, nucleon single particle-energies, shell corrections calculated for some cases, relativistic mean field theory.
doi: 10.1016/S0375-9474(96)00273-4
1995LA07 Nucl.Phys. A586, 201 (1995) Ground-State Properties of Exotic Nuclei Near Z = 40 in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110Sr, 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110Zr, 70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100Kr; calculated binding energy, rms charge, neutron radii, isotope shifts, neutron skin thickness, shape coexistence (in some cases), quadrupole deformations. Relativistic mean field theory.
doi: 10.1016/0375-9474(94)00519-S
1995SH13 Phys.Rev.Lett. 74, 3744 (1995) M.M.Sharma, G.Lalazissis, J.Konig, P.Ring Isospin Dependence of the Spin-Orbit Force and Effective Nuclear Potentials NUCLEAR MOMENTS 200,202,204,206,208,210,212Pb; analyzed charge radii isotope shifts. Effective nuclear potentials, density dependent Hartree-Fock approach, effective Skyrme-like energy functional, spin-orbit potential iso-spin dependence.
doi: 10.1103/PhysRevLett.74.3744
1994SH09 Phys.Rev.Lett. 72, 1431 (1994) M.M.Sharma, G.A.Lalazissis, W.Hillebrandt, P.Ring Shell Effects in Nuclei Near the Neutron-Drip Line NUCLEAR STRUCTURE 110,112,114,116,118,120,122,124,128,132,134,136Zr; calculated binding energy, quadrupole deformation, single particle levels. Relativistic mean field theory.
doi: 10.1103/PhysRevLett.72.1431
1994SH25 Phys.Rev.Lett. 73, 1870 (1994) M.M.Sharma, G.A.Lalazissis, W.Hillebrandt, P.Ring Sharma et al. Reply: NUCLEAR STRUCTURE A=116-136; analyzed structure calculation. Skyrme approach, relativistic mean field approach comparison.
doi: 10.1103/PhysRevLett.73.1870
1994SH36 Ann.Phys.(New York) 231, 110 (1994) M.M.Sharma, M.A.Nagarajan, P.Ring The Relativistic Mean-Field, Effective Mass and the Compression Properties of Nuclei NUCLEAR STRUCTURE 16O; calculated p-shell spin-orbit splitting vs m(σ). Relativistic mean field, effective mass, compression properties.
doi: 10.1006/aphy.1994.1035
1994ST14 Phys.Rev. C50, 1445 (1994) M.V.Stoitsov, P.Ring, M.M.Sharma Generator Coordinate Calculations for Breathing-Mode Giant Monopole Resonance in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated giant monopole resonance, ground state energy, mass rms radii. Relativistic mean field theory, generator coordinate method.
doi: 10.1103/PhysRevC.50.1445
1994ST22 J.Phys.(London) G20, L149 (1994) M.V.Stoitsov, M.L.Cescato, P.Ring, M.M.Sharma Nuclear Breathing Mode in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 208Pb, 90Zr, 40Ca, 16O; calculated breathing mode collective mass incompressibility. Relativistic mean field theory.
doi: 10.1088/0954-3899/20/12/003
1993SH13 Phys.Lett. 312B, 377 (1993) M.M.Sharma, M.A.Nagarajan, P.Ring Rho Meson Coupling in the Relativistic Mean Field Theory and Description of Exotic Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,124Sn, 208Pb; calculated binding energy, charge, neutron radii percentage deviations, neutron skin thickness. 112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142Xe; calculated binding energy, charge radii, deformations; deduced ρ-meson coupling role. Relativistic mean field theory.
doi: 10.1016/0370-2693(93)90970-S
1993SH24 Phys.Lett. 317B, 9 (1993) M.M.Sharma, G.A.Lalazissis, P.Ring Anomaly in the Charge Radii of Pb Isotopes NUCLEAR STRUCTURE 190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated binding energies, charge radii, isotope shifts; deduced anomalous behavior explanation. Relativistic mean field theory.
doi: 10.1016/0370-2693(93)91561-Z
1992SH10 Phys.Rev. C45, 2514 (1992) Neutron Skin of Spherical Nuclei in Relativistic and Nonrelativistic Mean-Field Approaches NUCLEAR STRUCTURE 112,114,116,118,120,122,124Sn; calculated charge radii. 40,48Ca, 58,64Ni, 90Zr, 116,124Sn, 140Ce, 208Pb; calculated neutron rms radii, neutron-proton radius ratio to matter radius; deduced neutron rms radius increase with isospin. Relativistic mean-field approach, Hartree approximation.
doi: 10.1103/PhysRevC.45.2514
1992SH18 Phys.Rev. C46, 1715 (1992) Relativistic Mean-Field Description of Neutron-Deficient Platinum Isotopes NUCLEAR STRUCTURE 184,186,188,190,192,194,196,198Pt; calculated binding energy per nucleon, deformation parameters, rms charge radii changes, neutron skin thickness. Relativistic mean field approach.
doi: 10.1103/PhysRevC.46.1715
1991CI04 Phys.Rev. C43, 2622 (1991) O.Civitarese, A.G.Dumrauf, M.Reboiro, P.Ring, M.M.Sharma Effect of Pairing on Breathing Mode and Nuclear Matter Compressibility NUCLEAR STRUCTURE 112,114,116,118,120,122,124Sn; calculated giant resonance strength distribution; deduced pairing effect role on breathing mode excitation. Quasiparticle RPA.
doi: 10.1103/PhysRevC.43.2622
1991KO23 Nucl.Phys. A533, 95 (1991) Scalar Coupling in Relativistic Mean Field Theory and Properties of Nuclei and Nuclear Matter NUCLEAR STRUCTURE 208Pb; calculated proton baryon density, effective mass, neutron, proton, charge, rms radii, binding energy per particle. 16O; calculated effective mass, neutron, proton, charge, rms radii, binding energy per particle. Relativistic mean field theory.
doi: 10.1016/0375-9474(91)90821-M
1991KO36 Z.Phys. A340, 119 (1991) W.Koepf, Y.K.Gambhir, P.Ring, M.M.Sharma Neutron Halo in Lithium Nuclei: A relativistic mean-field approach NUCLEAR STRUCTURE 6,7,8,9,10,11Li; calculated binding energy matter, charge radii, two-neutron separation energies, quadrupole, hexadecapole moments. Relativisitic mean field approach.
doi: 10.1007/BF01303823
1990BO25 Nucl.Phys. A515, 173 (1990) W.T.A.Borghols, S.Brandenburg, J.H.Meier, J.M.Schippers, M.M.Sharma, A.van der Woude, M.N.Harakeh, A.Lindholm, L.Nilsson, S.Crona, A.Hakansson, L.P.Ekstrom, N.Olsson, R.de Leo Neutron Decay of the Giant Resonance Region in 124Sn and Especially of the Giant Monopole Resonance NUCLEAR REACTIONS 124Sn(α, α'), E=120 MeV; measured σ(θα, θn) vs excitation energy. 124Sn deduced giant resonance, neutron decay characteristics. Statistical model calculations. 124Sn(d, t), E=50 MeV; measured σ(Et). 123Sn deduced level structure, low lying hole states.
doi: 10.1016/0375-9474(90)90365-S
1989BO34 Nucl.Phys. A504, 231 (1989) W.T.A.Borghols, S.Brandenburg, J.H.Meier, J.M.Schippers, M.M.Sharma, A.van der Woude, M.N.Harakeh, A.Lindholm, L.Nilsson, S.Crona, A.Hakansson, L.P.Ekstrom, N.Olsson, R.De Leo Particle Decay of the Giant Resonance Region in 90Zr and Especially of the Giant Monopole Resonance NUCLEAR REACTIONS 90Zr(α, α'n), (α, α'p), E=120 MeV; measured α'p-, α'n-coin. 90Zr deduced giant resonance neutron, proton decay characteristics. Statistical model calculation.
doi: 10.1016/0375-9474(89)90344-8
1989SH29 Nucl.Phys. A504, 337 (1989) M.M.Sharma, W.Stocker, P.Gleissl, M.Brack Nuclear Matter Incompressibility from a Semi-Empirical Analysis of Breathing-Mode Energies NUCLEAR STRUCTURE A=20-200; analyzed breathing mode energies, incompressibilities; deduced liquid drop model parameters.
doi: 10.1016/0375-9474(89)90349-7
1988SH38 Phys.Rev. C38, 2562 (1988) M.M.Sharma, W.T.A.Borghols, S.Brandenburg, S.Crona, A.van der Woude, M.N.Harakeh Giant Monopole Resonance in Sn and Sm Nuclei and the Compressibility of Nuclear Matter NUCLEAR REACTIONS 112,114,116,120,124Sn, 144,148,150,152Sm(α, α'), E=120 MeV; measured σ(E, θ); deduced compressibility of nuclear matter. 112,114,116,120,124Sn, 144,148,150,152Sm deduced GQR, GMR, Γ, sum rule strength. DWBA analysis.
doi: 10.1103/PhysRevC.38.2562
1987BO37 Phys.Lett. 197B, 37 (1987) W.T.A.Borghols, S.Brandenburg, S.Crona, R.De Leo, L.P.Ekstrom, A.Hakansson, M.N.Harakeh, A.Lindholm, J.H.Meier, L.Nilsson, N.Olsson, J.M.Schippers, M.M.Sharma, A.van der Woude Neutron Decay of the Giant Monopole Resonance in 124Sn NUCLEAR REACTIONS 124Sn(α, α'n), E=120 MeV; measured σ(θα', θn). 124Sn deduced isoscalar giant monopole resonance neutron decay. 123Sn deduced hole state J, π, spectroscopic strength.
doi: 10.1016/0370-2693(87)90337-6
1987VA10 Phys.Rev.Lett. 58, 2383 (1987) A.van der Woude, W.T.A.Borghols, S.Brandenburg, M.M.Sharma Comment on ' Compression Modulus of Nuclear Matter and Charge-Distribution Differences ' NUCLEAR STRUCTURE 28Si, 64,66Zn, 112,116,118,120,124Sn, 142Nd, 144Sm, 197Au, 208Pb; analyzed giant monople resonance data, E0 transition EWSR; deduced nuclear matter compression modulus parameters.
doi: 10.1103/PhysRevLett.58.2383
1986SH17 Radiat.Eff. 93, 53 (1986) Angular Distribution of Polar Light Particles in the Fission of 235-U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured σ(θα), σ(θt) following fission.
doi: 10.1080/00337578608207428
1985SH10 Pramana 24, 131 (1985) Angular Distribution in Ternary Fission NUCLEAR REACTIONS 235U(n, F), E=0.1-1 MeV; measured σ(θα), anisotropy following fission. Particle telescope.
doi: 10.1007/BF02894824
1982SI08 J.Phys.(London) G8, L85 (1982) A.K.Sinha, M.M.Sharma, S.C.L.Sharma, G.K.Mehta, D.M.Nadkarni Polar and Equatorial Emission of Light Charged Particles in keV Neutron-Induced Fission NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal, 600 keV; measured proton, triton, α yields, polar, equatorial emission; deduced polar emission mechanism. E-ΔE telescope.
doi: 10.1088/0305-4616/8/6/006
Back to query form |