NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.L.Rustgi Found 66 matches. 1993OZ01 Can.J.Phys. 71, 162 (1993) Nuclear Charge Density Radius Parameter and the β Decay Between Mirror Nuclei
doi: 10.1139/p93-026
1993ZH24 Phys.Rev. C48, 2585 (1993) Nucleon Polarization and Cross Section in Photodisintegration of Aligned and Polarized Deuterons at Low and Medium Energies NUCLEAR REACTIONS 2H(γ, p), E=10, 20 MeV; calculated σ(θ), photoproton polarization vs θ; deduced 2H polarization, alignment role. Meson exchange currents, relativistic effects.
doi: 10.1103/PhysRevC.48.2585
1990RA01 Phys.Rev. C41, 374 (1990) Spurious States in Quasiparticle Theory NUCLEAR STRUCTURE 59,61,63,65,60,62,64,66Ni; calculated levels, B(λ). Quasiparticle modified TDA, spuriosity elimination.
doi: 10.1103/PhysRevC.41.374
1989KA05 Phys.Rev. C39, 1142 (1989) A.Kassaee, L.N.Pandey, M.L.Rustgi, E.Hadjimichael Contributions to the E2 Transition in the Reaction 2H(γ, n)p NUCLEAR REACTIONS 2H(γ, n), E=4-20 MeV; calculated σ(θ) ratio; deduced contributions to E2 transition.
doi: 10.1103/PhysRevC.39.1142
1989RA10 Nuovo Cim. 101A, 507 (1989) Projected Spectra of Fe Isotopes in the Modified Deformed BCS Approach NUCLEAR STRUCTURE 52,54,56,58Fe; calculated levels. Modified deformed BCS approach.
doi: 10.1007/BF02789433
1989RU04 Phys.Rev. C40, 1581 (1989) Deuteron Photodisintegration Near Threshold NUCLEAR REACTIONS 2H(γ, p), E ≈ 2.3-4 MeV; calculated σ(E), P(n), asymmetry vs E; deduced σ(θ) ratio, photodisintegration mechanism.
doi: 10.1103/PhysRevC.40.1581
1987HA14 Phys.Rev. C36, 44 (1987) E.Hadjimichael, M.L.Rustgi, L.N.Pandey E2 Transition in the Reaction 2H(γ, n)1H NUCLEAR REACTIONS 2H(γ, n), E=10-20 MeV; calculated σ(θ), ratios, percentage polarization vs θ, σ(E); deduced nucleon-nucleon system nonspherical components, transition multipole components.
doi: 10.1103/PhysRevC.36.44
1987RU01 Phys.Rev. C35, 841 (1987) M.L.Rustgi, A.Kassaee, L.N.Pandey Photodisintegration of Deuteron at Low Energies: Isolation of electric and magnetic contributions NUCLEAR REACTIONS 2H(polarized γ, n), E=5 MeV; calculated photodisintergration σ(θ, φ), percentage polarization; deduced E1, M1 contributions.
doi: 10.1103/PhysRevC.35.841
1987RU03 Phys.Rev. C35, 1242 (1987); Erratum Phys.Rev. C41, 2946 (1990) M.L.Rustgi, A.Kassaee, L.N.Pandey Photodisintegration of the Deuteron with Elliptically Polarized Gamma Rays NUCLEAR REACTIONS 2H(polarized γ, p), E=2.5, 10, 20 MeV; calculated σ(θ, φ), proton polarization vs (θ, φ), σ(θp). Elliptically polarized beam.
doi: 10.1103/PhysRevC.35.1242
1986RU03 Phys.Rev. C33, 1823 (1986) M.L.Rustgi, L.N.Pandey, A.Kassaee Asymmetry and Angular Distribution of Deuteron Photodisintegration in the 20-60 MeV Range NUCLEAR REACTIONS 2H(polarized γ, p), E=19.8, 29, 38.6, 60.8 MeV; calculated asymmetry function, σ(θ) parameters; deduced multipole limits.
doi: 10.1103/PhysRevC.33.1823
1985PA23 Phys.Rev. C32, 1191 (1985) Relativistic Effects in the Sum Rules for the d(γ, p)n Reaction NUCLEAR REACTIONS 2H(γ, p), E ≈ breakup; calculated relativistic effect contribution to σ, bremsstrahlung weighted σ; deduced relativistic effects sensitivity to two-body potentials.
doi: 10.1103/PhysRevC.32.1191
1985PA28 Phys.Rev. C32, 1842 (1985) Relativistic Effects and Deuteron Photodisintegration with Polarized and Unpolarized Gamma Rays NUCLEAR REACTIONS 2H(γ, p), (γ, n), E=4-100 MeV; calculated photodisintegration σ(θ), nucleon polarization, asymmetry. Relativistic effects.
doi: 10.1103/PhysRevC.32.1842
1985VY01 Phys.Rev. C31, 41 (1985) Two-Body Effects in Triton Photodisintegration Sum Rules NUCLEAR REACTIONS 3H(γ, X), E=threshold; calculated photodisintegration enhancement factor, bremsstrahlung weighted σ.
doi: 10.1103/PhysRevC.31.41
1984RU01 Phys.Rev. C29, 785 (1984) M.L.Rustgi, R.Vyas, O.P.Rustgi Two-Body Effects and Deuteron Photodisintegration with Polarized and Unpolarized Gamma Rays NUCLEAR REACTIONS 2H(γ, n), (polarized γ, n), E=4-150 MeV; calculated σ(θ), asymmetry, nucleon polarization. Realistic nucleon-nucleon interactions.
doi: 10.1103/PhysRevC.29.785
1984RU02 Phys.Rev. C29, 1580 (1984) M.L.Rustgi, R.Vyas, O.P.Rustgi Desirability of Measurements on the Asymmetry Function at Low Energies in the 2H(γ, n)1H Reaction NUCLEAR REACTIONS 2H(γ, n), E=2.4-3.3 MeV; calculated asymmetry function.
doi: 10.1103/PhysRevC.29.1580
1983RA22 Phys.Rev. C28, 935 (1983) Odd Ni Isotopes in the Lipkin-Nogami Approach NUCLEAR STRUCTURE 59,61,63,65Ni; calculated levels, μ, B(λ). Modified Tamm-Dancoff approximation, Kuo-Brown interaction.
doi: 10.1103/PhysRevC.28.935
1983RU02 Phys.Rev.Lett. 50, 236 (1983); Erratum Phys.Rev.Lett. 50, 1825 (1983) Two-Body Effects and Neutron Polarization in the Reaction 2H(γ, n)H at Low Energies NUCLEAR REACTIONS 2H(γ, n), E=8-14 MeV; calculated neutron polarization vs E, θ. Two-body charge, current density effects.
doi: 10.1103/PhysRevLett.50.236
1983RU05 Phys.Lett. 121B, 365 (1983) Exchange Corrections and Deuteron Photodisintegration with Polarized Gamma Rays NUCLEAR REACTIONS 2H(polarized γ, n), E ≈ 10-180 MeV; calculated asymmetry (θ=90°) vs E. 2H(γ, n), E=100 MeV; calculated neutron polarization vs θ; 2H(γ, n), E=50, 150 MeV; calculated σ(θ). Exchange corrections to photodisintegration.
doi: 10.1016/0370-2693(83)91178-4
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
1982LO06 Lett.Nuovo Cim. 33, 47 (1982) Photodisintegration of 6Li in the Sum Rule Formalism NUCLEAR REACTIONS 6Li(γ, X), E not given; calculated total σ(photodisintegration), integrated σ(bremsstrahlung). Sum rule method.
doi: 10.1007/BF02727574
1982RA12 Phys.Rev. C26, 243 (1982) Modified Tamm-Dancoff Approximation Calculations using Lipkin-Nogami Approach NUCLEAR STRUCTURE 60,62,64,66Ni; calculated levels, B(E2). Modified Tamm-Dancoff approximation, Kuo-Brown interaction.
doi: 10.1103/PhysRevC.26.243
1982VY01 Phys.Rev. C25, 1801 (1982) γ(d, n)p Reaction with Polarized and Unpolarized Gamma Rays NUCLEAR REACTIONS 2H(γ, n), (polarized γ, n), E=20-150 MeV; calculated σ(θ), σ(total), asymmetry vs E. Paris, supersoft core potentials, photodisintegration process.
doi: 10.1103/PhysRevC.25.1801
1982VY04 Phys.Rev. C26, 1399 (1982) Two-Body Effects in the Sum Rules for the d(γ, p)n Reaction NUCLEAR REACTIONS 2H(γ, p), E not given; calculated integrated, bremsstrahlung weighted σ. Pion exchange effects, different potentials.
doi: 10.1103/PhysRevC.26.1399
1979RU04 Phys.Rev. C20, 24 (1979) M.L.Rustgi, T.S.Sandhu, O.P.Rustgi Photodisintegration of the Deuteron Employing a Supersoft Core Potential NUCLEAR REACTIONS 2H(γ, n), E=100, 150 MeV; calculated σ(θ), P(θ). Supersoft core potential.
doi: 10.1103/PhysRevC.20.24
1979SA11 Phys.Rev. C19, 1530 (1979) Deformed Nuclei in the Lipkin-Nogami Approach NUCLEAR STRUCTURE 44,46,48,50Ti; calculated ground state energies, pairing energies projected spectra. Lipkin-Nogami model with modified deformed BCS approximation, effective Kuo-Brown interaction.
doi: 10.1103/PhysRevC.19.1530
1979ZI04 Nuovo Cim. 52A, 247 (1979) W.Zickendraht, M.L.Rustgi, R.G.Brandt Cross-Section and Polarization in the Photodisintegration of the Deuteron with Arbitrary Number of Electromagnetic Multipoles NUCLEAR REACTIONS 2H(γ, n), E not given; calculated all electromagnetic multipole transition amplitudes. Radiation field, nucleon interaction, final state interactions considered.
doi: 10.1007/BF02902046
1978RA18 Lett.Nuovo Cim. 23, 126 (1978) R.Raj, B.B.Roy, O.P.Rustgi, M.L.Rustgi Negative-Parity Levels in Even Nickel Isotopes NUCLEAR STRUCTURE 60,62,64,66Ni; calculated negative parity levels, B(λ).
doi: 10.1007/BF02763077
1978SA02 Phys.Rev. C17, 796 (1978); Erratum Phys.Rev. C18, 1081 (1978) Lipkin-Nogami Method Using Effective Yale Interaction NUCLEAR STRUCTURE 58,60,62,64,66Ni, 60,62,64,66,68Zn, 64,66,68,70Ge; calculated ground state properties. Effective Yale interaction.
doi: 10.1103/PhysRevC.17.796
1977MP01 Phys.Rev. C16, 816 (1977) Generalized BCS Calculations for the 2s-1d Shell with Realistic Interactions NUCLEAR STRUCTURE 20Ne, 24Mg, 32S, 36Ar; calculated ground-state properties. Generalized BCS method.
doi: 10.1103/PhysRevC.16.816
1977MP02 Nuovo Cim. 41A, 279 (1977) Structure Calculations for 40Ca with the Supersoft-Core Potential NUCLEAR STRUCTURE 40Ca; calculated ground state properties.
doi: 10.1007/BF02730108
1977RU01 Can.J.Phys. 55, 158 (1977) M.L.Rustgi, O.P.Rustgi, T.S.Sandhu Photodisintegration Cross Sections of the Deuteron NUCLEAR REACTIONS 2H(γ, X); calculated σ.
doi: 10.1139/p77-020
1977RU07 Phys.Lett. 70B, 145 (1977) M.L.Rustgi, T.S.Sandhu, O.P.Rustgi Theoretical Investigation of the Photodisintegration of Deuteron at 0° for the Outgoing Protons NUCLEAR REACTIONS 2H(γ, p), E=30-150 MeV; calculated σ(E).
doi: 10.1016/0370-2693(77)90506-8
1976MP01 Phys.Rev. C14, 365 (1976) Axial Symmetry of 24Mg and 32S in the BCS Approximation NUCLEAR STRUCTURE 24Mg, 32S; calculated ground state properties. BCS method.
doi: 10.1103/PhysRevC.14.365
1976SA11 Phys.Lett. 62B, 271 (1976) T.S.Sandhu, M.L.Rustgi, H.Chandra Pairing Correlations in Even-Even Isotopes NUCLEAR STRUCTURE 52,54,56,58Fe; calculated pairing correlations, quadrupole moment, p-, n-pickup strengths.
doi: 10.1016/0370-2693(76)90072-1
1976SA17 Phys.Rev. C14, 675 (1976) Hartree-Fock-Bogoliubov Calculations with T = 1 Plus T = 0 Pairing Correlations NUCLEAR STRUCTURE 46,48,50Ti, 50,52,54Cr, 54,56,58Fe, 58,60,62,64Ni, 62,64,66,68Zn; calculated quadrupole moment, pickup strengths. Hartree-Fock, Hartree-Fock-Bogoliubov methods, Kuo-Brown interaction.
doi: 10.1103/PhysRevC.14.675
1975MP01 Phys.Rev. C12, 2072 (1975) N = Z Even-Even Nuclei in the 2s-1d Shell NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated binding energy, potential.
doi: 10.1103/PhysRevC.12.2072
1975SA07 Phys.Rev. C12, 666 (1975) Hartree-Fock-Bogoliubov Calculations for Odd-Mass Nuclei in the 0f-1p Shell NUCLEAR STRUCTURE 44,45,46,47,48,49,50,51Ti, 48,49,50,51,52,53,54,55Cr, 52,53,54,55,56,57,58,59Fe, 56,57,58,59,60,61,62,63,64,65Ni, 61,62,63,64,65,66,67Zn, 70,65,66,67,68,69Ge, 47,49,51,53V, 51,53,55,57Mn, 55,57,59,61Co, 61,63,65,67Cu, 62,64,66,68Zn, 64,65,67,69Ga, 71As; calculated binding energies, quadrupole moment, proton, neutron pickup strengths. 45,47Ti, 51Cr, 53Fe, 59Ni, 61,63,67Zn, 47,49,51,53V, 55,57Co, 61,65,67Cu; calculated B(E2).
doi: 10.1103/PhysRevC.12.666
1975SA10 Phys.Rev. C12, 1340 (1975) T.S.Sandhu, M.L.Rustgi, A.L.Goodman Generalized Pairing in N = Z Even-Even 2p-1f Shell Nuclei NUCLEAR STRUCTURE 44Ti, 48Cr, 52Fe, 56Ni, 60Zn; calculated binding energies, quadrupole moments, pickup strengths. Hartree-Fock-Bogoliubov method with generalized pairing.
doi: 10.1103/PhysRevC.12.1340
1975SA12 Lett.Nuovo Cim. 14, 161 (1975) Odd-Mass 2s-1d-Shell Nuclei in Hartree-Fock-Bogoliubov Approach NUCLEAR STRUCTURE 21Ne, 23Na, 25Mg, 27Al, 33S, 35Cl; calculated p, n separation energies, quadrupole moment, B(E2).
doi: 10.1007/BF02748123
1974FU12 Phys.Rev. C10, 2649 (1974) Shell-Model Calculations for 51Ti and 52V NUCLEAR STRUCTURE 51V, 51Ti; calculated levels. 51Ti; calculated μ. NUCLEAR REACTIONS 50Ti(d, p); calculated S.
doi: 10.1103/PhysRevC.10.2649
1974MP01 Phys.Rev. C9, 2261 (1974) Nuclear-Structure Calculations with the Modified Yale Potential for the 2s-1d Shell NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated single-particle energies, ground-state energies, rms radii, ground-state deformations. Hartree-Fock method. Modified Yale interaction.
doi: 10.1103/PhysRevC.9.2261
1973CH03 Phys.Rev. C7, 180 (1973) Projected Hartree-Fock and Hartree-Fock-Bogoliubov Spectra for Even Ti, Cr, and Fe Isotopes NUCLEAR STRUCTURE 44,46,48,50Ti, 48,50,52,54Cr, 52,54,56,58Fe; calculated levels. Projected Hartree-Fock, Hartree-Fock-Bogoliubov theory.
doi: 10.1103/PhysRevC.7.180
1973SA24 Phys.Rev. C8, 1152 (1973) Note on the Single-Closed-Shell Nuclei NUCLEAR STRUCTURE 18,20O; calculated binding energies.
doi: 10.1103/PhysRevC.8.1152
1973SI19 Phys.Lett. 44B, 409 (1973) M1 and E2 Transitions in 59Ni NUCLEAR STRUCTURE 59Ni; calculated B(M1), B(E2).
doi: 10.1016/0370-2693(73)90320-1
1972CH14 Phys.Rev. C5, 1791 (1972) Generalized Bardeen-Cooper-Schrieffer and Self-Consistent Hartree-Fock-Bogoliubov Approximations NUCLEAR STRUCTURE 44,46,48,50Ti; calculated ground-state energy, pairing energy, chemical potential, quadrupole moment, hexadecapole moment. Self-consistent HFB, generalized BCS approximations.
doi: 10.1103/PhysRevC.5.1791
1972CH32 Phys.Rev. C6, 907 (1972) Study of Even Calcium and Nickel Isotopes with Self-Consistent Approximations NUCLEAR STRUCTURE 42,44,46,48,50Ca, 58,60,62,64Ni; calculated levels, pairing energy. Self-consistent approximations.
doi: 10.1103/PhysRevC.6.907
1972CH37 Phys.Rev. C6, 1281 (1972) Investigation of Asymmetric Shapes for the Even-Even 2p-1f Shell Nuclei NUCLEAR STRUCTURE 48Ti, 48,50,52Cr, 52,56,58Fe, 58,60Ni, 60,62,64,66,68Zn, 68Ge; calculated levels, quadrupole moment, single-particle energies; analyzed pairing effects. Hartree-Fock, Hartree-Fock-Bogoliubov theory; triaxial shapes.
doi: 10.1103/PhysRevC.6.1281
1972FU02 Phys.Rev. C5, 1137 (1972) C.C.Fu, R.P.Singh, R.Raj, M.L.Rustgi Level Structure of Ca44 with the Hamada-Johnston and Tabakin Interactions NUCLEAR STRUCTURE 44Ca; calculated levels, B(E2), S for 43Ca(d, p). Hamada-Johnston, Tabakin interactions.
doi: 10.1103/PhysRevC.5.1137
1971BR04 Nucl.Phys. A161, 337 (1971) Proposed Polarized-Target-Beam Test for 3S1-3S1 Radiative Transitions in Thermal n-p Capture NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated Iγ(θ), Pγ.
doi: 10.1016/0375-9474(71)90373-3
1971CH11 Phys.Rev. C3, 1476 (1971) Self-Consistent Calculations for Even Ti, Cr, and Fe Isotopes NUCLEAR STRUCTURE 44,46,48,50Ti, 48,50,52,54Cr, 52,54,56,58Fe; calculated ground-state energies, quadrupole moment. Hartree-Fock, Hartree-Fock-Bogoliubov, spherical BCS approximation.
doi: 10.1103/PhysRevC.3.1476
1971CH29 Phys.Rev. C4, 406 (1971) Self-Consistent Study of Even Nickel Isotopes with Central Yukawa and Hamada-Johnson Interactions NUCLEAR STRUCTURE 56,58,60,62,64Ni; calculated levels, quadrupole moment, ±. Central Yukawa, Hamada-Johnston interactions.
doi: 10.1103/PhysRevC.4.406
1971CH33 Phys.Rev. C4, 874 (1971) Self-Consistent Study of Even Zn and Ge Isotopes NUCLEAR STRUCTURE 60,62,64,66,68,70Zn, 64,66,68,70,72Ge; calculated levels, binding energy, quadrupole moment, ±. Hartree-Fock, Hartree-Fock-Bogoliubov, spherical BCS approximations.
doi: 10.1103/PhysRevC.4.874
1971CH36 Phys.Lett. 36B, 185 (1971) Pairing Force, Intrinsic Quadrupole Moment and Moment of Inertia NUCLEAR MOMENTS 62Zn, 64Ge, 64Zn, 68Ge, 66Zn; calculated quadrupole moment, hexadecapole moments. Cranking model, pairing force.
doi: 10.1016/0370-2693(71)90063-3
1971RU06 Phys.Rev. C3, 2238 (1971) M.L.Rustgi, R.P.Singh, B.B.Roy, R.Raj, C.C.Fu Shell-Model Calculations for V51 and Cr52 NUCLEAR STRUCTURE 51V, 52Cr; calculated levels, B(λ), μ, quadrupole moment, S for 50Ti(3He, d), 51V(3He, d).
doi: 10.1103/PhysRevC.3.2238
1971RU09 Phys.Rev. C4, 854 (1971) M.L.Rustgi, H.W.Kung, R.Raj, R.A.Nisley, M.H.Hull, Jr. Reaction Matrix Elements and Structure Calculations with the Yale and Reid Potentials for the Ni Region NUCLEAR STRUCTURE 58,59,60Cu, 58,59,60Ni, 60Zn; calculated levels, B(E2). Shell-model, quasiparticle formalisms.
doi: 10.1103/PhysRevC.4.854
1971SI05 Phys.Rev. C3, 1172 (1971) Shell-Model Calculations for Cu60 and Zn60 with Reaction Matrix Elements NUCLEAR STRUCTURE 60Cu, 60Zn; calculated levels. Shell model, reaction matrix elements.
doi: 10.1103/PhysRevC.3.1172
1970BA06 Phys.Rev. C1, 207 (1970) B.Barman Roy, R.Raj, M.L.Rustgi Nuclear-Structure Calculations for Cr52 and Even Ni Isotopes NUCLEAR STRUCTURE 52Cr, 58,60,62,64Ni; calculated levels, B(λ).
doi: 10.1103/PhysRevC.1.207
1970KU07 Phys.Rev. C1, 1994 (1970); Erratum Phys.Rev. C2, 1581 (1970) H.W.Kung, R.P.Singh, R.Raj, M.L.Rustgi Level Structure of Sc43 and Odd-Mass Ca Isotopes with Reaction Matrix Elements NUCLEAR STRUCTURE 43Sc, 43Ca; calculated odd-parity levels. Shell model, reaction elements. 43,45,47Ca; calculated levels. Modified Tamm-Dancoff approximation.
doi: 10.1103/PhysRevC.1.1994
1970RU03 Phys.Rev. C1, 1138 (1970) Theoretical Study of 1+ and 3+ States in Even-A Nickel Isotopes NUCLEAR STRUCTURE 58,60,62,64,66Ni; calculated levels, B(λ). Modified Tamm-Dancoff approximation.
doi: 10.1103/PhysRevC.1.1138
1970RU10 Phys.Rev. C2, 2446 (1970) M1 and E2 Transitions from 1+ and 3+ States in Even-A Nickel Isotopes NUCLEAR STRUCTURE 58,60,62,64Ni; calculated B(M1), B(E2).
doi: 10.1103/PhysRevC.2.2446
1970SI18 Phys.Rev. C2, 1715 (1970) R.P.Singh, R.Raj, M.L.Rustgi, H.W.Kung Nuclear-Structure Calculations for Cu59 and Odd Nickel Isotopes NUCLEAR STRUCTURE 59Cu, 59,61,63,65Ni; calculated levels. Shell model.
doi: 10.1103/PhysRevC.2.1715
1969RA03 Phys.Lett. 28B, 468 (1969) Nuclear Energy Levels of 51V and 59Ni NUCLEAR STRUCTURE 51V, 59Ni calculated levels.
doi: 10.1016/0370-2693(69)90517-6
1969RA19 Phys.Rev. 181, 1536 (1969) Nuclear Energy Levels of V51, Mn53, and Co55 by the Quasiparticle Method NUCLEAR STRUCTURE 51V, 53Mn, 55Co; calculated levels using modified Tamm-Dancoff approximation.
doi: 10.1103/PhysRev.181.1536
1969SI08 Nucl.Phys. A133, 365(1969) Charge Form Factor of the Alpha Particle NUCLEAR STRUCTURE 4He; calculated nuclear charge form factor.
doi: 10.1016/0375-9474(69)90638-1
1968RU05 Nucl.Phys. A117, 321 (1968) M.L.Rustgi, J.G.Lucas, S.N.Mukherjee Application of Intermediate-Coupling Unified Nuclear Model to Odd-Mass Iodine Isotopes
doi: 10.1016/0375-9474(68)90846-4
1967SH09 Phys. Letters 25B, 391 (1967) On the Odd-Parity States in 4He
doi: 10.1016/0370-2693(67)90154-2
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