NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = V.S.Ramamurthy Found 52 matches. 2013MO26 Phys.Rev. C 88, 034606 (2013) G.Mohanto, N.Madhavan, S.Nath, J.Gehlot, I. Mukul, A.Jhingan, T.Varughese, A.Roy, R.K.Bhowmik, I.Mazumdar, D.A.Gothe, P.B.Chavan, J.Sadhukhan, S.Pal, M.Kaur, V.Singh, A.K.Sinha, V.S.Ramamurthy Evaporation residue excitation function and spin distribution for 31P+170Er NUCLEAR REACTIONS 170Er(31P, xn), E=134.4, 136.5, 141.6, 146.7, 151.9, 157.0, 162.1, 167.3, 172.0, 177.2 MeV; measured reaction products, Eγ, Iγ, TOF, evaporation residue (ER) σ(E) and spin distribution, ER-gated γ-multiplicity distributions using HYbrid Recoil mass Analyzer (HYRA) and a 4π spin spectrometer for γ rays at IUAC facility in Delhi. Comparison with statistical model calculations using CCFULL computer code. Discussed effect of compound nucleus shell closure.
doi: 10.1103/PhysRevC.88.034606
2012MO21 Nucl.Phys. A890-891, 62 (2012) G.Mohanto, N.Madhavan, S.Nath, J.Sadhukhan, J.Gehlot, I.Mazumdar, M.B.Naik, E.Prasad, I.Mukul, T.Varughese, A.Jhingan, R.K.Bhowmik, A.K.Sinha, D.A.Gothe, P.B.Chavan, S.Pal, V.S.Ramamurthy, A.Roy Entrance channel effect on ER spin distribution NUCLEAR REACTIONS 170Er(30Si, X), E=126.0, 130.1, 135.2, 140.3, 145.4, 150.5, 155.6, 160.7 MeV; measured evaporation residue E(ER), I(ER) using multiwire proportional counter, Eγ, Iγ(θ), γγ-coin, (ER)γ-coin; calculated compound nucleus spin distribution using CCFULL code, fusion σ, evaporation residue σ; deduced γ multiplicity, level density parameters, fission barrier, compound nucleus spin distribution, fusion σ, evaporation residue σ. Compared other reactions leading to the same composite system.
doi: 10.1016/j.nuclphysa.2012.07.004
2008SH21 Phys.Lett. B 670, 99 (2008) P.D.Shidling, N.Madhavan, V.S.Ramamurthy, S.Nath, N.M.Badiger, S.Pal, A.K.Sinha, A.Jhingan, S.Muralithar, P.Sugathan, S.Kailas, B.R.Behera, R.Singh, K.M.Varier, M.C.Radhakrishna Experimental signature of entrance channel effect in heavy mass region via evaporation residue cross section and spin distribution measurements NUCLEAR REACTIONS 184W(16O, F), 181Ta(19F, F), E*=50-90 MeV; measured Eγ, Iγ, (particle)γ-coin, Evaporation Residue cross sections and γ multiplicity distributions.
doi: 10.1016/j.physletb.2008.10.044
1998RA01 Phys.Rev. C57, 971 (1998) G.V.Ravi Prasad, A.M.Samant, A.Shrivastava, A.Navin, A.Chatterjee, P.Singh, S.Kailas, V.S.Ramamurthy Fission Fragment Angular Distributions at Near-Barrier Energies in 11B, 12C, 14N + 209Bi NUCLEAR REACTIONS 209Bi(11B, F), (12C, F), (14N, F), E ≈ barrier; measured fission σ(E), fragment anisotropies; deduced target deformation role. Statistical model analysis, other reactions compared.
doi: 10.1103/PhysRevC.57.971
1997BI08 Phys.Rev. C56, 1926 (1997) D.C.Biswas, R.K.Choudhury, B.K.Nayak, D.M.Nadkarni, V.S.Ramamurthy Single and Multinucleon Transfer in 19F, 16O, 12C + 232Th Reactions at Near Barrier Energies NUCLEAR REACTIONS 232Th(19F, X), E=92-114 MeV; 232Th(16O, X), E=86.6, 94.8 MeV; 232Th(12C, X), E=59-82 MeV; measured projectile-like fragment σ(E, Z), σ(θ) for quasielastic, transfer reactions; deduced model parameters, transfer probabilities, Q-value dependence. Semiclassical model.
doi: 10.1103/PhysRevC.56.1926
1996RA22 Phys.Rev. C54, 815 (1996) G.V.Ravi Prasad, V.S.Ramamurthy Light Fragment Emission During Mass Asymmetry Relaxation in Heavy-Ion Induced Fission NUCLEAR REACTIONS 232Th(12C, F), E not given; calculated fission like fragments mass-charge distributions; deduced binary fragment production mechanism.
doi: 10.1103/PhysRevC.54.815
1995BI21 Phys.Rev. C52, R2827 (1995) D.C.Biswas, R.K.Choudhury, D.M.Nadkarni, V.S.Ramamurthy Evidence of Massive Cluster Transfers in 19F + 232Th Reaction at Near Barrier Energies NUCLEAR REACTIONS 232Th(19F, X), E=113.6, 106.5 MeV; measured σ(fragment θ); deduced reduced transfer probability, Q-value dependence.
doi: 10.1103/PhysRevC.52.R2827
1995RA07 Phys.Rev. C51, 2833 (1995) G.V.Ravi Prasad, V.S.Ramamurthy, R.T.Yadav Simple Formula for Conditional Fission Barriers of Rotating Nuclei NUCLEAR STRUCTURE 75Br, 110In, 55Co; calculated fission barrier vs fragment charge. 244Cm; calculated fission fragment yield vs charge. Extended Swiatecki's fusion model.
doi: 10.1103/PhysRevC.51.2833
1995UM01 Phys.Rev. C52, 1431 (1995) V.S.Uma Maheswari, V.S.Ramamurthy, L.Satpathy Nuclear Incompressibility: An analytical study on the leptodermous expansion
doi: 10.1103/PhysRevC.52.1431
1994KA45 Pramana 42, 107 (1994) S.K.Kataria, A.Nijasure, V.S.Ramamurthy, A.K.Dutta Leptodermous Expansion of Nuclear Ground State Energies and the Anomaly in the Nuclear Curvature Energy NUCLEAR STRUCTURE A=40-200; calculated total energy, other aspects. Liquid drop model Leptodermous expansion.
doi: 10.1007/BF02847506
1994UM02 Phys.Rev. C49, 2854 (1994) V.S.Uma Maheswari, V.S.Ramamurthy, L.Satpathy Reply to ' Comment on ' Influence of Bulk Properties on the Surface Structure of Finite Nuclei ' '
doi: 10.1103/PhysRevC.49.2854
1993RA02 Phys.Rev. C47, 1311 (1993) Determination of Extra-Push Energies for Fusion from Differential Fission Cross-Section Measurements NUCLEAR REACTIONS 208Pb(40Ar, X), (40Ar, F), E(cm)=172 MeV; analyzed σ data; deduced no inconsistencies in extra push energies for fusion determined by both reactions.
doi: 10.1103/PhysRevC.47.1311
1992MO19 Phys.Rev. C46, 2012 (1992) A.K.Mohanty, S.V.S.Sastry, S.K.Kataria, V.S.Ramamurthy Experimental Determination of Energy-Dependent Barriers for Fusion NUCLEAR REACTIONS, ICPND 154Sm(16O, X), 59Co(37Cl, X), E(cm)=55-70 MeV; analyzed fusion, average angular momentum vs σ(E). Energy dependent barrier penetration model, other reactions studied.
doi: 10.1103/PhysRevC.46.2012
1991KA03 Phys.Rev. C43, 1466 (1991) S.Kailas, A.Navin, A.Chatterjee, P.Singh, R.K.Choudhury, A.Saxena, D.M.Nadkarni, S.S.Kapoor, V.S.Ramamurthy, B.K.Nayak, S.V.Suryanarayana Fission Fragment Angular Distributions for the System 19F + 232Th NUCLEAR REACTIONS 232Th(19F, F), E=94-108 MeV; measured fission fragment σ(θ), anisotropy; deduced entrance channel dependences. Saddle-point statistical model.
doi: 10.1103/PhysRevC.43.1466
1991VA02 Phys.Rev. C43, 1850 (1991) R.Varma, G.K.Mehta, R.K.Choudhury, S.S.Kapoor, B.K.Nayak, V.S.Ramamurthy Prompt Gamma-Ray Multiplicity Distributions in Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured prompt γ-ray multiplicity distribution; deduced fission fragment average spin, width.
doi: 10.1103/PhysRevC.43.1850
1990KA09 Nucl.Instrum.Methods Phys.Res. A288, 585 (1990) S.K.Kataria, V.S.Ramamurthy, M.Blann, T.T.Komoto Shell-Dependent Level Densities in Nuclear Reaction Codes NUCLEAR REACTIONS, ICPND 54Fe(α, p), (α, np), (α, n), (α, 2n), (α, xnyp), (α, 2np), (α, 3np), (α, 4np), (α, 3n), (α, 4n), E=threshold-70 MeV; calculated σ(E). Shell dependent level densities, exciton model.
doi: 10.1016/0168-9002(90)90155-Y
1990MO19 Phys.Rev.Lett. 65, 1096 (1990) A.K.Mohanty, S.V.S.Sastry, S.K.Kataria, V.S.Ramamurthy Use of an Energy-Dependent Barrier for Heavy-Ion Fusion NUCLEAR REACTIONS, ICPND 122Sn(40Ar, X), E(cm)=101-109 MeV; calculated fusion σ(E); deduced energy dependent barrier role. Full dynamical coupled-channels model.
doi: 10.1103/PhysRevLett.65.1096
1990MO28 Phys.Lett. 247B, 215 (1990) A.K.Mohanty, S.V.S.Sastry, S.K.Kataria, S.Kailas, V.S.Ramamurthy A New Optical Model Approach for Heavy Ion Fusion NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E ≈ 76-112 MeV; calculated fusion σ(E). Optical model, energy dependent imaginary potential.
doi: 10.1016/0370-2693(90)90884-9
1990RA11 Phys.Rev. C41, 2702 (1990) V.S.Ramamurthy, A.K.Mohanty, S.K.Kataria, G.Rangarajan Sub-Barrier Fusion in a Macroscopic Model of Nuclear Shape Evolutions NUCLEAR REACTIONS 144,154Sm(40Ar, X), E(cm) ≈ 100-150 MeV; calculated effective fusion barrier vs E.
doi: 10.1103/PhysRevC.41.2702
1989AN05 Ann.Nucl.Energy 16, 87 (1989) R.P.Anand, H.M.Jain, S.Kailas, S.K.Gupta, V.S.Ramamurthy Neutron Capture Cross Section Measurement of 232Th in the Energy Range of 400-900 keV NUCLEAR REACTIONS 232Th(n, γ), E=400-950 keV; measured capture σ(E). Activation analysis.
doi: 10.1016/0306-4549(89)90032-7
1989KA46 Pramana 33, 161 (1989) Fragment Angular Distributions in Fission and Fission-Like Reactions NUCLEAR REACTIONS, ICPND 209Bi(14N, F), (11B, F), E(cm) ≈ 60-110 MeV; 209Bi(16O, F), (12C, F), E(cm) ≈ 70-150 MeV; compiled calculated fission σ(E).
doi: 10.1007/BF02845914
1987CH04 Nucl.Phys. A463, 597 (1987) R.K.Choudhury, A.Saxena, V.S.Ramamurthy, D.M.Nadkarni, S.S.Kapoor Variation of Kinetic Energy Distributions of Fission Fragments with Bombarding Energy in 4He Induced Fision of 238U at Medium Energies NUCLEAR REACTIONS, ICPND 238U(α, F), E=32, 40, 48, 56 MeV; measured fission fragment yield vs mass, kinetic energy distributions.
doi: 10.1016/0375-9474(87)90632-4
1986AN15 Radiat.Eff. 93, 189 (1986) R.P.Anand, H.M.Jain, S.Kailas, S.K.Gupta, V.S.Ramamurthy, S.S.Kapoor Neutron Capture Cross Section of Th-232 NUCLEAR REACTIONS 232Th(n, γ), E=400-935 keV; measured σ. Gold standard.
doi: 10.1080/00337578608207449
1986RA09 Radiat.Eff. 92, 301 (1986) Pre-Equilibrium Fission: A new decay channel for composite systems formed in fusion reactions NUCLEAR REACTIONS 27Al(236U, F), E(cm)=90, 146 MeV; calculated fission fragment σ(θ); deduced three fission component contributions, preequilibrium fission role. 263Db deduced fission characteristics.
doi: 10.1080/00337578608208339
1986SA37 Pramana 27, 679 (1986) Surface Diffuseness of Deformed and Rotating Nuclei NUCLEAR REACTIONS 150Sm(α, α), E not given; calculated interaction barrier. Energy density formalism. NUCLEAR STRUCTURE 150Sm; calculated binding energy vs surface diffuseness anisotropy. Energy density formalism.
doi: 10.1007/BF02845294
1985KA15 Pramana 24, 119 (1985) Nucleon Transport Processes in Fission and Heavy Ion Reactions NUCLEAR REACTIONS 209Bi(136Xe, X), E=940, 1130, 1422 MeV; 208Pb(208Pb, X), E=7, 7.6 MeV/nucleon; 208Pb(238U, X), E=7.5 MeV/nucleon; calculated fragment kinetic energy loss vs charge variance. 235U(n, F), E=thermal; calculated fission fragment kinetic energy dependence vs charge, mass variances, their ratios. Nucleon transport process, mean fragment temperature. NUCLEAR STRUCTURE 226Ra, 252Cf, 256Fm; calculated fission fragment mass yields. Nucleon transport process, mean fragment temperature.
doi: 10.1007/BF02894823
1985RA01 Phys.Rev.Lett. 54, 178 (1985) Interpretation of Fission-Fragment Angular Distributions in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 208Pb(19F, F), E=110, 150, 190 MeV; 208Pb(24Mg, F), E=140, 170, 210 MeV; 208Pb(28Si, F), E=160, 200, 260 MeV; 208Pb(32S, F), E=185, 205, 225 MeV; calculated fission fragment σ(θ); deduced K equilibrium characteristic time.
doi: 10.1103/PhysRevLett.54.178
1985RA25 Phys.Rev. C32, 2182 (1985) Effect of Fission following Incomplete Fusion on the Interpretation of Fission Fragment Angular Distributions in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 232Th(16O, F), E=95 MeV; 248Cm, 238U, 232Th, 197Au(32S, F), E=218 MeV; 238U(16O, F), E(cm)=90 MeV; 238U(27Al, F), E(cm)=146 MeV; calculated fission fragment σ(θ); deduced incomplete fusion role.
doi: 10.1103/PhysRevC.32.2182
1984KA19 Pramana 22, 275 (1984) S.S.Kapoor, V.S.Ramamurthy, R.Ramanna Fusion-Fission Angular Distributions: A new probe of fast fission fractionation in nucleus-nucleus collisions NUCLEAR REACTIONS 208Pb(19F, X), (19F, F), E=110, 150, 190 MeV; 208Pb(24Mg, X), (24Mg, F), E=140 MeV; 208Pb(28Si, X), (28Si, F), E=160 MeV; 208Pb(32S, F), (32S, X), E=185 MeV; analyzed fusion-fission fragment σ(θ); deduced fast, compound nucleus fission competition.
doi: 10.1007/BF02846379
1984KU22 Phys.Rev. C30, 2096 (1984) K.Kumar, R.K.Choudhury, V.S.Ramamurthy, S.S.Kapoor Dynamical Aspects of the Correlation between Nucleon Exchange and Energy Loss for the 136Xe + 209Bi System NUCLEAR REACTIONS 209Bi(136Xe, X), E=825-1650 MeV; calculated fragment mass, charge variances, energy loss correlation; deduced nucleon exchange rate. Classical dynamic, one-body transport models.
doi: 10.1103/PhysRevC.30.2096
1984PR02 Phys.Rev.Lett. 52, 990 (1984); Erratum Phys.Rev.Lett. 53, 2520 (1984) M.Prakash, V.S.Ramamurthy, S.S.Kapoor, J.M.Alexander Transition-State Theory for Fission Angular Distributions: A flexible-rotor model NUCLEAR REACTIONS 198Pt(12C, F), E=186 MeV; 208Pb(19F, F), E=135 MeV; 208Pb(28Si, F), E=170 MeV; calculated fission fragment σ(θ), anisotropies. Transition state theory, flexible rotor model. NUCLEAR STRUCTURE 225Pa; calculated fission barrier, saddle point configuration vs K/I. Transition state theory, flexible, rigid rotor models.
doi: 10.1103/PhysRevLett.52.990
1983BE05 Z.Phys. A309, 253 (1983) D.Belhafaf, J.P.Bocquet, R.Brissot, Ch.Ristori, J.Crancon, H.Nifenecker, J.Mougey, V.S.Ramamurthy Kinetic Energy Distributions around Symmetric Thermal Fission of U234 and U236 NUCLEAR REACTIONS 233,235U(n, F), E=thermal; measured fission fragment kinetic energy vs mass. 234,236U deduced symmetric fission characteristics.
doi: 10.1007/BF01413757
1983DI15 Pramana 20, 523 (1983) A.N.Dixit, V.S.Ramamurthy, Y.R.Waghmare Classical Description of Low Energy 16O + 16O Collisions NUCLEAR REACTIONS, ICPND 16O(16O, X), E(cm)=16.64-66.56 MeV; calculated fusion σ(E); deduced classical approximation limitations. Lennard-Jones potential, classical microscopic description.
doi: 10.1007/BF02846287
1983RA11 Nucl.Phys. A398, 544 (1983) V.S.Ramamurthy, M.Asghar, S.K.Kataria Mean Distribution of Single-Particle Levels in Thin-Skinned Potential Wells and the Macroscopic Level Density Parameters of Nuclei NUCLEAR STRUCTURE A ≈ 27-220; calculated level density parameter. Thin skinned potential well single particle level densities, droplet model potential parameters.
doi: 10.1016/0375-9474(83)90301-9
1981PR01 Phys.Lett. 98B, 413 (1981) M.Prakash, S.Shlomo, V.S.Ramamurthy, S.S.Kapoor, S.K.Kataria Microscopic Calculation of Mass Transport Coefficients in Heavy Ion Collisions NUCLEAR REACTIONS 108Ag(40Ar, X), E=288 MeV; 165Ho, 209Bi(84Kr, X), E=714 MeV; 166Er(86Kr, X), E=515 MeV; 197Au(86Kr, X), E=620 MeV; 120Sn(132Xe, X), E=779 MeV; 209Bi(136Xe, X), E=1130 MeV; 238U(238U, X), E=1766 MeV; calculated drift, diffusion coefficients; deduced nucleon transfer probability. Microscopic approach, Fermi golden rule, Pauli blocking effect, deep inelastic collision.
doi: 10.1016/0370-2693(81)90442-1
1980KA27 Nucl.Phys. A349, 10 (1980) Macroscopic Systematics of Nuclear Level Densities NUCLEAR STRUCTURE A=90, 180, 208; calculated nuclear level density systematics; deduced level density parameter dependence on isospin, neutron separation energies. Independent-particle model, shell, pairing effects.
doi: 10.1016/0375-9474(80)90440-6
1980KA29 Phys.Rev. C22, 2263 (1980) Macroscopic Level Density Parameters of Nuclei NUCLEAR STRUCTURE A=40-210; calculated level density parameters; deduced dependence on last nucleon separation energy. Woods-Saxon potential, isospin dependence, semiempirical macroscopic approach.
doi: 10.1103/PhysRevC.22.2263
1980RA03 Phys.Rev. C21, 752 (1980) V.S.Ramamurthy, M.Prakash, S.S.Kapoor Magnitude of Energy Dissipation in Fission RADIOACTIVITY 252Cf (SF); calculated energy dissipation, scission energy.
doi: 10.1103/PhysRevC.21.752
1980RA04 Nucl.Phys. A334, 477 (1980) V.S.Ramamurthy, S.K.Kataria, S.S.Kapoor Analysis of Fission Excitation Functions and Fission Barrier Heights of Preactinide Nuclei NUCLEAR REACTIONS 194Pt, 197Au, 203,205Tl, 206,208Pb, 209Bi(α, F), E not given; analyzed σ(E); deduced fission barrier heights. Liquid drop model, single particle effects.
doi: 10.1016/0375-9474(80)90612-0
1978CH24 Phys.Rev. C18, 2213 (1978) Scission-Point Configurations in Ternary Fission of 252Cf from Trajectory Calculations RADIOACTIVITY 252Cf; calculated E(fragment), Eα(θ) for ternary SF.
doi: 10.1103/PhysRevC.18.2213
1978KA24 Phys.Rev. C18, 549 (1978) S.K.Kataria, V.S.Ramamurthy, S.S.Kapoor Semiempirical Nuclear Level Density Formula with Shell Effects NUCLEAR STRUCTURE A=41-242; calculated level density. Semiempirical level density formula.
doi: 10.1103/PhysRevC.18.549
1978RA11 Pramana 10, 319 (1978); see 78Ra26 Analysis of Fission Excitation Functions and the Determination of Shell Effects at the Saddle Point
doi: 10.1007/BF02872030
1978RA26 Pramana 10, 319 (1978) Analysis of Fission Excitation Functions and the Determination of Shell Effects at the Saddle Point NUCLEAR REACTIONS 208Pb(α, F); analyzed fission σ(E). 212Po deduced shell effects at saddle point.
doi: 10.1007/BF02872030
1977RA09 Pramana 8, 322 (1977) V.S.Ramamurthy, R.K.Choudhury, J.C.Mohankrishna Prompt Gamma Ray Multiplicity Distributions in Spontaneous Fission of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured prompt γ-multiplicity; deduced shape parameters.
doi: 10.1007/BF02847802
1977RA27 Pramana 9, 623 (1977) V.S.Ramamurthy, R.K.Choudhury, J.C.M.Krishna Multiplicity Distribution of Prompt Gamma Rays in Spontaneous Ternary Fission of 252Cf RADIOACTIVITY, Fission 252Cf (SF); measured prompt γ-ray multiplicity distribution.
doi: 10.1007/BF02848149
1976RA14 Phys.Lett. 62B, 124 (1976) V.S.Ramamurthy, M.Prakash, S.S.Kapoor On the Uncertainties in the Shell Correction by Strutinsky Smearing Procedure for Certain Shapes Relevant in Fission NUCLEAR STRUCTURE 240Pu; calculated neutron, proton shell corrections.
doi: 10.1016/0370-2693(76)90483-4
1975KA41 Pramana 5, 124 (1975) Statistical Properties of Excited Fissioning Nuclei NUCLEAR STRUCTURE 242Pu; calculated statistical properties of fissioning nuclei.
doi: 10.1007/BF02875183
1972RA45 Phys.Lett. 42B, 399 (1972) Statistical Properties of Excited Nuclei and the Determination of the Ground-State Shell Correction Energies NUCLEAR STRUCTURE 24Na, 41Ca, 208Pb, 232Th, 232Pa, 236U, 242Pu; Z=114; analyzed ground state shell corrections energies.
doi: 10.1016/0370-2693(72)90091-3
1971KA28 Phys.Rev. C4, 2165 (1971) S.S.Kapoor, S.K.Kataria, S.R.S.Murthy, D.M.Nadkarni, V.S.Ramamurthy, P.N.Rama Rao Studies of the Times of Emission and Multiplicities of K X Rays from Fission Fragments of Specified Atomic Numbers RADIOACTIVITY, Fission 236U, 252Cf; measured K X-ray average emission times, multiplicities.
doi: 10.1103/PhysRevC.4.2165
1970RA21 Phys.Rev.Lett. 25, 386 (1970) V.S.Ramamurthy, S.S.Kapoor, S.K.Kataria Excitation Energy Dependence of Shell Effects on Nuclear Level Densities and Fission Fragment Anisotropies NUCLEAR STRUCTURE 208Pb, 242Pu; calculated shell effects on level densities.
doi: 10.1103/PhysRevLett.25.386
1969KA04 Phys.Rev. 177, 1776(1969) S.S.Kapoor, V.S.Ramamurthy, R.Zaghloul Yield of K X Rays Emitted from U236 Fragments NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured K X-ray yield of fission fragments.
doi: 10.1103/PhysRev.177.1776
1968KA31 Phys.Rev. 166, 1190 (1968) S.S.Kapoor, V.S.Ramamurthy, P.N.Rama Rao K X Rays from Cf252 Fission Fragments in Ternary Fission RADIOACTIVITY, Fission 252Cf(SF); measured E(K X-ray), K X-ray yields.
doi: 10.1103/PhysRev.166.1190
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