NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.Sharma Found 83 matches. 2024SO04 Phys.Rev. C 109, 024905 (2024) S.Solanki, M.Lal, R.Sharma, V.K.Agotiya Dissociation and thermodynamical properties of heavy quarkonia in an anisotropic strongly coupled hot quark gluon plasma: Using a baryonic chemical potential
doi: 10.1103/PhysRevC.109.024905
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
2021GU03 Nucl.Phys. A1005, 121967 (2021) Warm Pions in Real Time
doi: 10.1016/j.nuclphysa.2020.121967
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
2021SA57 J.Phys.(London) G48, 125102 (2021) G.Saxena, M.Kumawat, R.Sharma, M.Aggarwal Collapse of N = 28 magicity in exotic 40Mg-probe of deformed halo and 2n-radioactivity at Mg neutron drip-line NUCLEAR STRUCTURE 40,42,44Mg; calculated neutron separation energies, single particle energies, neutron and proton pairing energy contributions, shell gaps, radial moments, radial density distributions, neutron skin thickness. 40Mg; deduced neutron halo, dineutron correlations.
doi: 10.1088/1361-6471/ac288b
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
2019AS01 Nucl.Instrum.Methods Phys.Res. A922, 287 (2019) J.Ashenfelter, A.B.Balantekin, C.Baldenegro, H.R.Band, C.D.Bass, D.E.Bergeron, D.Berish, L.J.Bignell, N.S.Bowden, J.Boyle, J.Bricco, J.P.Brodsky, C.D.Bryan, A.B.Telles, J.J.Cherwinka, T.Classen, K.Commeford, A.J.Conant, A.A.Cox, D.Davee, D.Dean, G.Deichert, M.V.Diwan, M.J.Dolinski, A.Erickson, M.Febbraro, B.T.Foust, J.K.Gaison, A.Galindo-Uribarri, C.E.Gilbert, K.E.Gilje, A.Glenn, B.W.Goddard, B.T.Hackett, K.Han, S.Hans, A.B.Hansell, K.M.Heeger, B.Heffron, J.Insler, D.E.Jaffe, X.Ji, D.C.Jones, K.Koehler, O.Kyzylova, C.E.Lane, T.J.Langford, J.LaRosa, B.R.Littlejohn, F.Lopez, X.Lu, D.A.Martinez Caicedo, J.T.Matta, R.D.McKeown, M.P.Mendenhall, H.J.Miller, J.M.Minock, P.E.Mueller, H.P.Mumm, J.Napolitano, R.Neilson, J.A.Nikkel, D.Norcini, S.Nour, D.A.Pushin, X.Qian, E.Romero-Romero, R.Rosero, D.Sarenac, B.S.Seilhan, R.Sharma, P.T.Surukuchi, C.Trinh, M.A.Tyra, R.L.Varner, B.Viren, J.M.Wagner, W.Wang, B.White, C.White, J.Wilhelmi, T.Wise, H.Yao, M.Yeh, Y.-R.Yen, A.Zhang, C.Zhang, X.Zhang, M.Zhao The PROSPECT reactor antineutrino experiment
doi: 10.1016/j.nima.2018.12.079
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
2017GU27 Nucl.Phys. A967, 716 (2017) Effective Field Theory Models for Thermal QCD
doi: 10.1016/j.nuclphysa.2017.04.036
2017SH08 Eur.Phys.J. A 53, 63 (2017) Landau damping of gluons in the two-flavor color superconducting Fulde-Ferrell phase
doi: 10.1140/epja/i2017-12249-x
2016SI10 At.Data Nucl.Data Tables 109-110, 339 (2016) A.K.Singh, A.Goyal, I.Khatri, S.Aggarwal, R.Sharma, M.Mohan Energy levels, lifetimes and radiative data of Ba XXVI ATOMIC PHYSICS Ba; calculated energy levels, radiative rates, T1/2. Comparison with available data.
doi: 10.1016/j.adt.2015.12.003
2015SH15 Phys.Rev. C 91, 042801 (2015) Neutrino-pair bremsstrahlung from nucleon-α versus nucleon-nucleon scattering
doi: 10.1103/PhysRevC.91.042801
2014GU10 Phys.Rev. C 89, 057901 (2014) Thermalization of quarkonia at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.89.057901
2013SH18 Phys.Rev. C 87, 044905 (2013) High transverse momentum quarkonium production and dissociation in heavy ion collisions
doi: 10.1103/PhysRevC.87.044905
2013SH23 Nucl.Phys. A904-905, 631c (2013) High transverse momentum quarkonium production and dissociation in heavy ion collisions
doi: 10.1016/j.nuclphysa.2013.02.095
2012GE01 Phys.Rev. C 85, 015806 (2012) Phase separation in low-density neutron matter
doi: 10.1103/PhysRevC.85.015806
2011CI07 Phys.Rev. C 84, 045809 (2011) V.Cirigliano, S.Reddy, R.Sharma Low-energy theory for superfluid and solid matter and its application to the neutron star crust
doi: 10.1103/PhysRevC.84.045809
2011SH05 Phys.Rev. C 83, 025803 (2011) Anisotropic electronic screening and damping in magnetars
doi: 10.1103/PhysRevC.83.025803
2009SH39 Nucl.Phys. A830, 857c (2009) Light Cone wavefunction approach to open heavy flavor dynamics in the QGP
doi: 10.1016/j.nuclphysa.2009.10.127
2009SH43 Phys.Rev. C 80, 054902 (2009) Light-cone wave function approach to open heavy flavor dynamics in QCD matter
doi: 10.1103/PhysRevC.80.054902
2006RA29 J.Phys.(London) G32, S483 (2006) The crystallography of strange quark matter
doi: 10.1088/0954-3899/32/12/S61
1999IS06 Pramana 52, 609 (1999) Complete and Incomplete Fusion Studies in 7Li and 16O Induced Reactions on 51V by Measurement of Excitation Functions and Recoil Ranges NUCLEAR REACTIONS 51V(7Li, X)51Cr/52Mn/54Mn/56Mn, E=40-50 MeV; 51V(16O, X)51Cr/52Mn/54Mn/56Co/57Co/58Co/56Ni/61Cu/62Zn/63Zn, E=60-90 MeV; measured production σ, recoil ranges; deduced complete, incomplete fusion reaction mechanisms. Activation technique. Comparison with statistical model.
doi: 10.1007/BF02829867
1998IS02 Phys.Rev. C57, 1290 (1998) M.Ismail, R.P.Sharma, M.H.Rashid The 181Ta(7Li, 5n)183Os Reaction: Measurement and analysis of the excitation function and isomeric cross-section ratios NUCLEAR REACTIONS, ICPND 181Ta(7Li, 5n), E=30-50 MeV; measured Eγ, Iγ, total residual σ, isomer ratio. Statistical model calculations.
doi: 10.1103/PhysRevC.57.1290
1997IS14 Pramana 49, 623 (1997) M.Ismail, R.P.Sharma, M.H.Rashid Measurement of Excitation Functions and Mean Projected Recoil Ranges of Nuclei in 12C-Induced Reactions on Vanadium NUCLEAR REACTIONS, ICPND 51V(12C, X)24Na/54Mn/56Co/57Co/58Co, E=34-83 MeV; measured production σ, recoil ranges. Stacked foil, thick-target thick-recoil-catcher techniques.
doi: 10.1007/BF02848336
1996AN26 Nucl.Instrum.Methods Phys.Res. B118, 190 (1996) J.U.Andersen, G.C.Ball, J.A.Davies, J.S.Forster, J.S.Geiger, R.Haakenaasen, N.E.Hecker, L.E.Rehn, R.P.Sharma, A.Uguzzoni Use of the 7.6 MeV 16O(α, α) Resonance in Studying the Anomalous Channeling Behaviour of YBa2Cu3O(7-x) Near T(c) NUCLEAR REACTIONS 16O, Y, Ba, Cu(α, α), E=7.62 MeV; measured σ(θ); deduced YBa2Cu3O(7-x) channeling behaviour.
doi: 10.1016/0168-583X(96)00243-1
1995GU03 Phys.Scr. 51, 316 (1995) J.B.Gupta, A.K.Kavathekar, R.Sharma A Single Term Expression of Ground Band Level Energies of a Soft Rotor NUCLEAR STRUCTURE A=150-200; calculated levels, band structure. Power law, single term expression.
doi: 10.1088/0031-8949/51/3/005
1994BA01 Phys.Rev. C49, 650 (1994) S.Basu, J.M.Chatterjee, D.Banik, R.K.Chattopadhyay, R.P.Sharma, S.K.Pardhasaradhi Octupole Deformation in 149,151Sm Nuclei NUCLEAR REACTIONS 148,150Nd(α, 3nγ), E=35, 37 MeV; measured Eγ, Iγ, γγ-coin. 149,151Sm deduced levels, J, π, B(E1)/B(E2) ratios, shape features, average electric dipole moment, band structure. Cranked shell model.
doi: 10.1103/PhysRevC.49.650
1994BA06 Phys.Rev. C49, 1221 (1994) V.Banerjee, A.Banerjee, G.S.N.Murthy, R.P.Sharma, S.K.Pardhasaradhi, A.Chakrabarti Decay of 98Rh RADIOACTIVITY 98,98mRh(β+) [from 96Ru(α, np), E=30.25 MeV]; measured βγ-coin, Eβ, Eγ, Iγ, T1/2;deduced log ft, Qβ, β-end point energy. He-jet recoil transport, plastic scintillator, hyperpure Ge detectors.
doi: 10.1103/PhysRevC.49.1221
1993IY01 Phys.Rev. C48, 87 (1993) R.H.Iyer, A.K.Pandey, P.C.Kalsi, R.C.Sharma Helium-Ion-Induced Fission Excitation Functions of Terbium and Ytterbium NUCLEAR REACTIONS, ICPND 159Tb, 170,171,172,173,174,176Yb(α, F), E=40-65 MeV; measured fission σ(E). 163Ho, 177Hf deduced fission barrier. Data on other nuclei analyzed.
doi: 10.1103/PhysRevC.48.87
1993PA29 Nucl.Instrum.Methods Phys.Res. B82, 151 (1993) A.K.Pandey, R.C.Sharma, P.C.Kalsi, R.H.Iyer Measurement of Alpha to Fission Branching Ratios of Heavy Actinides by Sequential Etching of Alpha and Fission Tracks in CR-39 RADIOACTIVITY 244Cm, 252Cf(SF), (α); measured α-, SF-decay branching ratio. Sequential etching procedure.
doi: 10.1016/0168-583X(93)95095-M
1992CH43 Z.Phys. A344, 149 (1992) J.M.Chatterjee, S.Basu, R.K.Chattopadhyay, K.Kar, D.Banik, R.P.Sharma, S.K.Pardhasaradhi High Spin Isomer in 151Sm NUCLEAR REACTIONS 150Nd(α, 3nγ), E=35 MeV; measured γγ-coin. 151Sm deduced isomer, other levels T1/2.
doi: 10.1007/BF01291698
1991IY01 Phys.Rev. C44, 2644 (1991) R.H.Iyer, A.K.Pandey, P.C.Kalsi, R.C.Sharma Excitation Functions for the Helium-Ion-Induced Fission of Holmium and Erbium NUCLEAR REACTIONS, ICPND 165Ho, Er(α, F), E=34-70 MeV; measured total fission σ(E). 169Tm, Yb deduced fission barrier, Γ(F)/Γn. Fission track detectors.
doi: 10.1103/PhysRevC.44.2644
1988SH42 Pramana 31, 185 (1988) Development of High Resolution Silicon Surface Barrier Detectors RADIOACTIVITY 241Am(α); measured Eα, Iα. 207Bi, 137Cs; measured I(ce). High resolution Si surface barrier detector.
doi: 10.1007/BF02848805
1987JO02 J.Chem.Phys. 86, 5294 (1987) A Correlation between NMR Chemical Shifts and Mossbauer Quadrupole Splittings for 119Sn and 125Te in Organotin and Organotellurium Compounds NUCLEAR MOMENTS 119Sn, 125Te; calculated NMR chemical shifts, Mossbauer quadrupole splittings; deduced correlation.
doi: 10.1063/1.452553
1987KU15 Hyperfine Interactions 34, 311 (1987) M.B.Kurup, K.G.Prasad, R.P.Sharma Hyperfine Fields at Implanted 119Sn in Fe NUCLEAR REACTIONS 119Sn(γ, γ), E=89.53 keV; measured Mossbauer I(ce); deduced 119Sn hyperfine fields in Fe.
doi: 10.1007/BF02072728
1985KU16 Hyperfine Interactions 23, 89 (1985) M.B.Kurup, K.G.Prasad, K.Raghunathan, R.P.Sharma Electric Quadrupole Interaction at 181Ta in RNi5 Compounds RADIOACTIVITY 181Hf(β-); measured γγ(θ, H, t); deduced electric quadrupole interaction at 181Ta in RNi5 compounds.
doi: 10.1007/BF02060140
1985MU08 Indian J.Phys. 59A, 92 (1985) G.S.Mudahar, R.K.Sharma, H.S.Sahota Pair Production Cross Sections at 2.754 MeV for 6 ≤ Z ≤ 72 NUCLEAR REACTIONS C, Mg, S, Ti, Ni, Cu, Zr, Nb, Mo, Ag, Sn, La, Gd, Hf(γ, X), E=2.754 MeV; analyzed absorption σ; deduced total attenuation coefficient.
1985SH02 J.Phys.(London) B18, 637 (1985) R.K.Sharma, K.Singh, H.S.Sahota Measurement of Pair Production Cross Sections in Ge for the 1.238-3.548 MeV Energy Range NUCLEAR REACTIONS Ge(γ, e+e-), E=1.238-3.548 MeV; measured pair production σ(E). Ge(Li) detector.
doi: 10.1088/0022-3700/18/4/011
1985SH17 Indian J.Phys. 59A, 89 (1985) R.K.Sharma, K.Singh, H.S.Sahota Absolute Pair Production Cross Sections for Z = 13, 26, 29, 50 and 82 at (1.173+1.333) MeV NUCLEAR REACTIONS 27Al, Fe, Cu, Sn, Pb(γ, e+e-), E=1.173, 1.333 MeV; measured absolute pair production σ. Internal 60Co source.
1983RU10 Nuovo Cim. 77A, 317 (1983) M.L.Rustgi, R.D.Nunemaker, R.D.Sharma Effects of Eletromagnetic Retardation in the Photodisintegration of the Deuteron NUCLEAR REACTIONS 2H(γ, p), E=threshold-180 MeV; calculated σ(θ), proton polarization vs θ. 2H(γ, p), E=2.72-20 MeV; analyzed σ(θ). 2H(γ, p), E=2.76-20 MeV; calculated σ. 2H(γ, n), E=2.76 MeV; calculated neutron polarization vs θ. 2H(γ, n), E ≈ 5-22.5 MeV; calculated neutron polarization vs E. Electromagnetic retardation, nucleon magnetic moment effects, realistic interactions.
doi: 10.1007/BF02816659
1983SH46 Indian J.Phys. 57A, 302 (1983) R.K.Sharma, G.S.Mudahar, K.Singh, H.S.Sahota Absolute Pair Production Cross Sections for Z = 29 and 50 ATOMIC PHYSICS Cu, Sn(γ, e+e-), E ≈ 1.25-3 MeV; measured absolute pair-production σ(E), total attenuation coefficients.
1983SI19 Phys.Rev. C28, 2115 (1983) K.Singh, G.Singh, R.K.Sharma, H.S.Sahota K-Shell Fluorescence Yield of Cs RADIOACTIVITY 133Ba(EC); measured Iγ, I(K X-ray); deduced K-shell fluorescence yield. Sum peak analysis.
doi: 10.1103/PhysRevC.28.2115
1979SH01 Lett.Nuovo Cim. 24, 86 (1979) Fission Penetrabilities in 230Th and 232Th NUCLEAR STRUCTURE 230,232Th; calculated potential barriers, fission penetrabilities; deduced existence of third asymmetic minimum.
doi: 10.1007/BF02725991
1976KU04 Phys.Rev. B13, 2735 (1976) M.B.Kurup, K.G.Prasad, R.P.Sharma Interaction of 154Gd Nuclei with their Environment in a Cu Matrix RADIOACTIVITY 154Eu; measured γγ(θ, H, t). 154Gd deduced attenuation coefficients in Cu.
doi: 10.1103/PhysRevB.13.2735
1976SH22 Phys.Rev. C14, 2340 (1976) Three-Hump Potential Barrier in the 234Th Nucleus NUCLEAR STRUCTURE 234Th; calculated fission penetrability through a three hump potential barrier.
doi: 10.1103/PhysRevC.14.2340
1975SH26 Can.J.Phys. 53, 2645 (1975) Effect of Initial Nuclear State on Penetrability Through Two-Peaked Fission Barriers NUCLEAR STRUCTURE 240Pu; calculated fission penetrability.
doi: 10.1139/p75-324
1974RA29 Indian J.Pure Appl.Phys. 12, 391 (1974) I.V.S.Rathore, R.R.Sharma, B.P.Singh On the Decay of 106Rh RADIOACTIVITY 106Rh; measured βγγ(θ). 106Pd levels deduced J, π.
1974SH24 Phys.Rev. B10, 3792 (1974) Theory of Ligand Distortions-Application to the Study of Nuclear Quadrupole Interactions of the Excited States of 111Cd and 117In in CdCl2 NUCLEAR STRUCTURE 111Cd, 117In; calculated quadrupole moment.
doi: 10.1103/PhysRevB.10.3792
1973LE01 Can.J.Phys. 51, 446 (1973) Penetrability Calculations Through a Double-Hump Barrier in Nuclear Fission
doi: 10.1139/p73-058
1973SA18 Indian J.Phys. 47, 61 (1973) Penetration Effects in the 134 keV Transition in 187Re NUCLEAR STRUCTURE 187Re; calculated nuclear penetration factor.
1973SH07 Nucl.Phys. A204, 371 (1973) R.P.Sharma, J.U.Andersen, K.O.Nielsen Application of the Blocking Technique to Measure Lifetimes of Nuclear Levels Excited in (p, α) Resonance Reactions in P and Al NUCLEAR REACTIONS 31P(p, α), E=642 keV; 27Al(p, α), E=633 keV; studied blocking pattern. 32S, 28Si deduced compound nuclear T1/2. GaP, Al single-crystal targets.
doi: 10.1016/0375-9474(73)90279-0
1972AH03 Can.J.Phys. 50, 622 (1972) Surface Distributions of Alpha Particles from Odd-A Nuclei NUCLEAR STRUCTURE 229Pa, 233U, 235,237Np, 241,243Am, 243Cm; calculated α-particle surface distributions.
doi: 10.1139/p72-086
1972SH12 Lett.Nuovo Cim. 4, 257 (1972) On the Alpha Intensities to Rotational Bands of Odd-A Nuclei
doi: 10.1007/BF02757240
1972VO08 Phys.Rev. C6, 266 (1972) T.von Egidy, O.W.B.Schult, D.Rabenstein, J.R.Erskine, O.A.Wasson, R.E.Chrien, D.Breitig, R.P.Sharma, H.A.Baader, H.R.Koch Nuclear Levels in 233Th Excited by Neutron Capture and (d, p) Reactions NUCLEAR REACTIONS 232Th(n, γ), E=slow; measured Eγ, Iγ; deduced Q. 232Th(d, p), E=12 MeV; measured Q, σ(Ep). 233Th deduced levels, L(n), J, π, S, γ-branching. RADIOACTIVITY 233Th; measured Eγ.
doi: 10.1103/PhysRevC.6.266
1971SH03 Phys.Rev.Lett. 26, 563 (1971) Ferrous-Ferric Anomaly in Quadrupole Moment of Fe57m NUCLEAR MOMENTS 57mFe; measured nothing; analyzed electric field gradients, quadrupole splitting data; deduced quadrupole moment.
doi: 10.1103/PhysRevLett.26.563
1971VO02 Z.Naturforsch. 26a, 1092 (1971) T.von Egidy, O.W.B.Schult, W.Kallinger, D.Breitig, R.P.Sharma, H.R.Koch, H.A.Baader Precision Measurement of Transition and Level Energies in 233U RADIOACTIVITY 233Pa; measured Eγ, Iγ. 233U deduced levels, transitions. Crystal spectrometer.
1970SH09 Nucl.Phys. A152, 225 (1970) R.P.Sharma, H.L.Nielsen, P.G.Hansen Hindrance Factors for Unique First-Forbidden Beta Transitions in Deformed Nuclei RADIOACTIVITY 159Dy[from 158Dy(n, γ)]; 169Er[from 168Er(n, γ)]; 185W[from 184W(n, γ)]; measured Eγ, Iγ; deduced log f1t, hindrance factors, Iβ.
doi: 10.1016/0375-9474(70)90824-9
1970SH10 Nucl.Phys. A152, 401 (1970) The E2 Strength of the 191 keV Transition in 197Au RADIOACTIVITY 197Hg[from 196Hg(n, γ)]; measured I(ce). 197Au transitions deduced γ-multipolarity, B(E2). Enriched target.
doi: 10.1016/0375-9474(70)90840-7
1970SH12 Nucl.Phys. A154, 312 (1970) Inelastic Scattering of Deuterons from 197Au NUCLEAR REACTIONS 197Au(d, d'), E=12.1 MeV; measured σ(Ed', θ). 197Au(16O, 16O'γ), E=52 MeV; measured σ(E(16O'), Eγ). 197Au deduced levels, B(E2). Natural targets.
doi: 10.1016/0375-9474(70)90159-4
1970SH16 Phys.Rev.Lett. 25, 1622 (1970) Nuclear Quadrupole Moment of Al27 in Al2O3 NUCLEAR MOMENTS 27Al; measured nothing; analyzed electric field gradient in Al2O3; deduced quadrupole moment.
doi: 10.1103/PhysRevLett.25.1622
1968PA01 Nucl.Phys. A109, 81 (1968) V.R.Pandharipande, K.G.Prasad, R.P.Sharma, B.V.Thosar Level Structure of 117In from the Decay of 117Cd RADIOACTIVITY 117Cd [from 116Cd(n, γ)] measured Eγ, Iγ, γγ-coin, γγ(θ), βγ(θ), ICC. 117In deduced levels J, π, multipolarities. Enriched target.
doi: 10.1016/0375-9474(68)90560-5
1967PA16 Nucl.Phys. A104, 525 (1967) V.R.Pandharipande, K.G.Prasad, R.P.Sharma Magnetic Moment of the 660 keV State in 117In RADIOACTIVITY 117Cd [from 116Cd(n, γ)]; measured γγ(θ, t, H) 117In level deduced g, μ. Enriched targets.
doi: 10.1016/0375-9474(67)90470-8
1966PA07 Phys.Rev. 143, 740 (1966) V.R.Pandharipande, K.G.Prasad, R.M.Singru, R.P.Sharma Low-Lying Excited States in In115 and In117 NUCLEAR STRUCTURE 115Cd, 117Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.143.740
1966PR05 Phys.Rev. 149, 980 (1966) K.G.Prasad, R.P.Sharma, B.V.Thosar Level Structure of Au199 from Decay of Pt199 NUCLEAR STRUCTURE 199Pt; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.149.980
1966SH01 Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn.(1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.549 (1966) R.P.Sharma, B.V.Thosar, K.G.Prasad X-Ray Yields from K-Shell Ionization by Alpha Particles NUCLEAR STRUCTURE 152Sm, 154Sm, 186W, 160Gd, 144Sm, 130Te, 140Ce, 120Sn, 208Pb; measured not abstracted; deduced nuclear properties.
1965PA09 Phys.Rev. 140, B1488 (1965) V.R.Pandharipande, R.M.Singru, R.P.Sharma Decay of Pd111 and Pd111m NUCLEAR STRUCTURE 111Pd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B1488
1965SH12 Current Sci.(India) 34, 524 (1965) Nuclear Structure Effects on Internal Conversion Coefficients NUCLEAR STRUCTURE 186Re, 160Tb, 156Sm, 170Tm, 166Ho, 170Lu, 176Ta, 188Ir; measured not abstracted; deduced nuclear properties.
1965TH06 Priv.Comm. (August 1965) B.V.Thosar, M.C.Joshi, R.P.Sharma, K.G.Prasad K-Shell Internal Conversion Coefficients of Pure E2 Transitions NUCLEAR STRUCTURE 188Os, 186Os, 160Dy, 170Yb, 176Hf; measured not abstracted; deduced nuclear properties.
1964PA18 Phys.Rev. 136, B346 (1964) V.R.Pandharipande, R.P.Sharma, G.Chandra Angular Correlation Measurements in the Decay of Cd115m NUCLEAR STRUCTURE 115Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B346
1964SH17 Phys.Rev. 134, B730 (1964) R.P.Sharma, K.P.Gopinathan, S.R.Amtey Decay of Cd117 NUCLEAR STRUCTURE 117Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B730
1964SH29 J.Chem.Phys. 41, 3581 (1964) Crystalline Fields in Corundum-Type Lattices NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1063/1.1725771
1964TH02 Nucl.Phys. 50, 305 (1964) B.V.Thosar, M.C.Joshi, R.P.Sharma, K.G.Prasad Internal Conversion Studies of the 2+ → 0+ Transitions in Some Deformed Even Nuclei NUCLEAR STRUCTURE 188Re, 166Ho, 170Tm, 176Lu, 186Re, 160Tb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90211-1
1963SH12 Proc.Nucl.Phys.Symp.Bombay, p.34 (1963) R.P.Sharma, K.P.Gopinathan, S.R.Amtey Radiation from the Decay of Cd117 NUCLEAR STRUCTURE 117Cd; measured not abstracted; deduced nuclear properties.
1963SH13 Proc.Nucl.Phys.Symp.Bombay, p.39 (1963) Levels in In115 NUCLEAR STRUCTURE 115Cd; measured not abstracted; deduced nuclear properties.
1963SH14 Phys.Rev. 131, 384 (1963) Decay of Cd115m NUCLEAR STRUCTURE 115Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.384
1963TH02 Nucl.Phys. 41, 380 (1963) B.V.Thosar, R.P.Sharma, K.G.Prasad Further Studies on the Decay of Eu156 NUCLEAR STRUCTURE 156Eu; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90517-0
1962AM03 Nuclear Phys. 29, 657 (1962) Decay of Rh106 NUCLEAR STRUCTURE 106Rh; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90215-8
1962DE19 Proc.Nucl.Phys.Symp.(Madras) p.166 (1962) S.H.Devare, R.P.Sharma, B.Saraf First Forbidden Beta-Spectra of Nd147 NUCLEAR STRUCTURE 147Nd; measured not abstracted; deduced nuclear properties.
1962SH08 Phys.Rev. 125, 2071 (1962) R.P.Sharma, S.H.Devare, B.Saraf Beta Spectrum of Neodymium-147 NUCLEAR STRUCTURE 198Au, 147Nd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.125.2071
1962SH28 Proc.Nucl.Phys.Symp.(Madras) p.141 (1962) R.P.Sharma, S.H.Devare, M.C.Joshi Further Studies on the Decay of Eu156 NUCLEAR STRUCTURE 156Eu; measured not abstracted; deduced nuclear properties.
1960AM04 Proc.Indian Acad.Sci. 52, 157 (1960) K.S.Y.Ambiye, S.D.Bhagwat, M.C.Joshi, R.P.Sharma, B.N.Subbarao Decay Scheme of Eu156 NUCLEAR STRUCTURE 156Eu; measured not abstracted; deduced nuclear properties.
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