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NSR database version of April 11, 2024.

Search: Author = R.Sharma

Found 83 matches.

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2021GU03      Nucl.Phys. A1005, 121967 (2021)

S.Gupta, R.Sharma

Warm Pions in Real Time

doi: 10.1016/j.nuclphysa.2020.121967
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2017GU27      Nucl.Phys. A967, 716 (2017)

S.Gupta, R.Sharma

Effective Field Theory Models for Thermal QCD

doi: 10.1016/j.nuclphysa.2017.04.036
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2015SH15      Phys.Rev. C 91, 042801 (2015)

R.Sharma, S.Bacca, A.Schwenk

Neutrino-pair bremsstrahlung from nucleon-α versus nucleon-nucleon scattering

doi: 10.1103/PhysRevC.91.042801
Citations: PlumX Metrics

2014GU10      Phys.Rev. C 89, 057901 (2014)

S.Gupta, R.Sharma

Thermalization of quarkonia at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.89.057901
Citations: PlumX Metrics

2013SH18      Phys.Rev. C 87, 044905 (2013)

R.Sharma, I.Vitev

High transverse momentum quarkonium production and dissociation in heavy ion collisions

doi: 10.1103/PhysRevC.87.044905
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2012GE01      Phys.Rev. C 85, 015806 (2012)

A.Gezerlis, R.Sharma

Phase separation in low-density neutron matter

doi: 10.1103/PhysRevC.85.015806
Citations: PlumX Metrics

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
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2011SH05      Phys.Rev. C 83, 025803 (2011)

R.Sharma, S.Reddy

Anisotropic electronic screening and damping in magnetars

doi: 10.1103/PhysRevC.83.025803
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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
Citations: PlumX Metrics

2009SH43      Phys.Rev. C 80, 054902 (2009)

R.Sharma, I.Vitev, B.-W.Zhang

Light-cone wave function approach to open heavy flavor dynamics in QCD matter

doi: 10.1103/PhysRevC.80.054902
Citations: PlumX Metrics

2006RA29      J.Phys.(London) G32, S483 (2006)

K.Rajagopal, R.Sharma

The crystallography of strange quark matter

doi: 10.1088/0954-3899/32/12/S61
Citations: PlumX Metrics

1999IS06      Pramana 52, 609 (1999)

M.Ismail, R.P.Sharma

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6157.

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0692.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6295.

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6293.

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
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1987JO02      J.Chem.Phys. 86, 5294 (1987)

C.H.W.Jones, R.D.Sharma

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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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1976SH22      Phys.Rev. C14, 2340 (1976)

R.C.Sharma, J.N.Leboeuf

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
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1975SH26      Can.J.Phys. 53, 2645 (1975)

R.C.Sharma, J.N.Leboeuf

Effect of Initial Nuclear State on Penetrability Through Two-Peaked Fission Barriers

NUCLEAR STRUCTURE 240Pu; calculated fission penetrability.

doi: 10.1139/p75-324
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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)

A.K.Sharma, R.R.Sharma

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
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1973LE01      Can.J.Phys. 51, 446 (1973)

J.N.LeBoeuf, R.C.Sharma

Penetrability Calculations Through a Double-Hump Barrier in Nuclear Fission

doi: 10.1139/p73-058
Citations: PlumX Metrics

1973SA18      Indian J.Phys. 47, 61 (1973)

H.S.Sahota, R.K.Sharma

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
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1972AH03      Can.J.Phys. 50, 622 (1972)

R.Ahooja, R.C.Sharma

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
Citations: PlumX Metrics

1972SH12      Lett.Nuovo Cim. 4, 257 (1972)


On the Alpha Intensities to Rotational Bands of Odd-A Nuclei

doi: 10.1007/BF02757240
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13836.

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
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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
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1970SH10      Nucl.Phys. A152, 401 (1970)

R.P.Sharma, H.L.Nielsen

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
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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
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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
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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
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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
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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
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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
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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
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1965SH12      Current Sci.(India) 34, 524 (1965)

R.P.Sharma, B.V.Thosar

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
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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
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1964SH29      J.Chem.Phys. 41, 3581 (1964)

R.R.Sharma, T.P.Das

Crystalline Fields in Corundum-Type Lattices

NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.

doi: 10.1063/1.1725771
Citations: PlumX Metrics

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
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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)

R.P.Sharma, H.G.Devare

Levels in In115

NUCLEAR STRUCTURE 115Cd; measured not abstracted; deduced nuclear properties.

1963SH14      Phys.Rev. 131, 384 (1963)

R.P.Sharma, H.G.Devare

Decay of Cd115m

NUCLEAR STRUCTURE 115Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.131.384
Citations: PlumX Metrics

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
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1962AM03      Nuclear Phys. 29, 657 (1962)

S.Y.Ambiye, R.P.Sharma

Decay of Rh106

NUCLEAR STRUCTURE 106Rh; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90215-8
Citations: PlumX Metrics

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
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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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Note: The following list of authors and aliases matches the search parameter R.Sharma: , R.C.SHARMA, R.D.SHARMA, R.K.SHARMA, R.P.SHARMA, R.R.SHARMA