NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = F.Khanna Found 61 matches. 2014IM01 J.Phys.(London) G41, 065101 (2014) M.Imran, A.A.Usmani, M.Ikram, Z.Hasan, F.C.Khanna Fully correlated variational Monte Carlo study of 4ΛH and 4ΛH* hypernuclei NUCLEAR STRUCTURE 4H; calculated hypernuclei separation energy, quenching factors, energy splitting between 0+ and 1+ states, one-body density. Comparison with available data.
doi: 10.1088/0954-3899/41/6/065101
2008US01 J.Phys.(London) G35, 025105 (2008) Behaviour of the ΛN and ΛNN potential strengths in the 5ΛHe hypernucleus
doi: 10.1088/0954-3899/35/2/025105
2004TS11 J.Phys.(London) G30, 1765 (2004) L+c, Σc, Ξc and Λb hypernuclei in the quark-meson coupling model NUCLEAR STRUCTURE 17O, 41,49Ca, 91Zr, 209Pb; calculated hypernucleus binding energies, single-particle energies, hyperon-nucleus potential features. Quark-meson coupling model.
doi: 10.1088/0954-3899/30/12/001
2003TS01 Phys.Lett. 552B, 138 (2003) Properties of charmed and bottom hadrons in nuclear matter: a plausible study
doi: 10.1016/S0370-2693(02)03157-X
2003TS02 Phys.Rev. C 67, 015211 (2003) Λ+c and Λb hypernuclei NUCLEAR STRUCTURE 41Ca, 209Pb; calculated hypernucleus density distributions, potential strengths. 16,17O, 40,41,49Ca, 89Y, 91Zr, 208,209Pb; calculated hypernucleus single-particle energies. Quark-meson coupling model.
doi: 10.1103/PhysRevC.67.015211
2003YA09 Phys.Rev. C 68, 048201 (2003) U.T.Yakhshiev, A.W.Thomas, F.C.Khanna Meson-nucleon vertex form factors a finite temperature using a soft pion form factor
doi: 10.1103/PhysRevC.68.048201
2002MA39 Eur.Phys.J. A 14, 81 (2002) D.U.Matrasulov, F.C.Khanna, Kh.Yu.Rakhimov, Kh.T.Butanov Spectra of Baryons Containing Two Heavy Quarks
doi: 10.1007/s10050-002-8792-3
2002TR05 Phys.Rev. C65, 045504 (2002) Radiative Muon Capture in Hydrogen NUCLEAR REACTIONS 1H(μ, γ), E at rest; calculated capture rate, γ-spectra. Chiral Lagrangian approach, comparison with data.
doi: 10.1103/PhysRevC.65.045504
2001RA39 Phys.Rev. C64, 064907 (2001) Finite Temperature Amplitudes and Reaction Rates in Thermofield Dynamics
doi: 10.1103/PhysRevC.64.064907
2001RI06 Eur.Phys.J. A 10, 97 (2001) R.A.Ritchie, H.G.Miller, F.C.Khanna Landau-Ginzburg Treatment of Nuclear Matter at Finite Temperature
doi: 10.1007/s100500170148
2001TR07 Nucl.Phys. A684, 481c (2001) Lepton U(1) Symmetry and Interaction of Neutrinos with Deuterons at High Energies
doi: 10.1016/S0375-9474(01)00429-8
2001TR13 Nucl.Phys. A689, 741 (2001) E.Truhlik, J.Smejkal, F.C.Khanna Electromagnetic Isoscalar ρπγ Exchange Current and the Anomalous Action
doi: 10.1016/S0375-9474(00)00610-2
2000KH14 Nucl.Phys. A673, 455 (2000) Weak Axial Exchange Currents for the Bethe-Salpeter Equation
doi: 10.1016/S0375-9474(00)00060-9
2000RA03 Phys.Rev. C61, 024907 (2000) A.Rakhimov, U.Yakhshiev, F.C.Khanna Meson-Nucleon Vertex Form Factors at Finite Temperature
doi: 10.1103/PhysRevC.61.024907
1999SM14 Few-Body Systems 26, 175 (1999) J.Smejkal, E.Truhlik, F.C.Khanna Chiral Lagrangians and the Transition Amplitude for Radiative Muon Capture NUCLEAR REACTIONS 1H(μ-, γ), E at rest; calculated transition amplitude.
doi: 10.1007/s006010050112
1998RA22 Phys.Rev. C58, 1738 (1998) A.M.Rakhimov, M.M.Musakhanov, F.C.Khanna, U.T.Yakhshiev Medium Modification of Nucleon Properties in the Skyrme Model
doi: 10.1103/PhysRevC.58.1738
1998RA32 Nucl.Phys. A643, 383 (1998) A.M.Rakhimov, F.C.Khanna, U.T.Yakhshiev, M.M.Musakhanov Density Dependence of Meson-Nucleon Vertices in Nuclear Matter
doi: 10.1016/S0375-9474(98)00561-2
1997UM04 Phys.Lett. 398B, 6 (1997) A.Yu.Umnikov, H.-X.He, F.C.Khanna Chiral-Odd Structure Function h1(D)(x) and Tensor Charge of the Deuteron NUCLEAR STRUCTURE 2H; calculated chiral odd structure function, ratio with respect to nucleon, tensor charge. Bethe-Salpeter formalism.
doi: 10.1016/S0370-2693(97)00195-0
1997UM05 Phys.Rev. C56, 1700 (1997) A.Yu.Umnikov, F.C.Khanna, L.P.Kaptari Deep Inelastic Scattering on the Deuteron in the Bethe-Salpeter Formalism. II. Realistic NN Interaction NUCLEAR STRUCTURE 2H; calculated charge, spin densities, structure functions; deduced relativistic effects. Bethe-Salpeter formalism, deep inelastic scattering.
doi: 10.1103/PhysRevC.56.1700
1996KA23 Phys.Rev. C54, 986 (1996) L.P.Kaptari, A.Yu.Umnikov, S.G.Bondarenko, K.Yu.Kazakov, F.C.Khanna, B.Kampfer Bethe-Salpeter Amplitudes and Static Properties of the Deuteron NUCLEAR STRUCTURE 2H; calculated nucleon density, spin distributions, μ, quadrupole moment, other static properties. Bethe-Salpeter formalism, relativistic corrections.
doi: 10.1103/PhysRevC.54.986
1996KH05 Phys.Rev. C54, 1133 (1996) F.C.Khanna, H.G.Miller, R.M.Quick Spontaneous Symmetry Breaking and the Dissipation of Nuclear Collective Degrees of Freedom at Finite Temperature NUCLEAR STRUCTURE 20Ne; calculated collective degrees of freedom dissipation associated critical temperature. Elliott model, spontaneous U(3) symmetry breaking.
doi: 10.1103/PhysRevC.54.1133
1996RA19 Phys.Lett. 378, 12 (1996) A.Rahimov, T.Okazaki, M.M.Musakhanov, F.C.Khanna The Deformation of the Interacting Nucleon in the Skyrme Model NUCLEAR STRUCTURE 1H; calculated interacting proton (in two-nucleon system) intrinsic quadrupole moment. Nucleon deformation under strong NN-interaction.
doi: 10.1016/0370-2693(96)00365-6
1996UM01 Phys.Rev. C53, 377 (1996) A.Yu.Umnikov, F.C.Khanna, L.P.Kaptari Off-Mass-Shell Deformation of the Nucleon Structure Function NUCLEAR STRUCTURE 2H; calculated structure function relative to nucleon. 1n; calculated structure function relative to deuteron, free neutron. Sullivan model, off-mass shell behavior.
doi: 10.1103/PhysRevC.53.377
1995KA27 Phys.Lett. 351B, 400 (1995) L.P.Kaptari, A.Yu.Umnikov, F.C.Khanna, B.Kampfer The Tensor Analyzing Power T20 in Deuteron Break-Up Reactions within the Bethe-Salpeter Formalism NUCLEAR REACTIONS 1H(polarized d, X), E=high; calculated T20, polarization transfer vs proton momentum after deuteron breakup, differential σ. Relativistic approach based on the Bethe-Salpeter equation, realistic meson exchange potential.
doi: 10.1016/0370-2693(95)00365-R
1994DA25 Phys.Rev. C50, 3135 (1994) I.C.Danchev, F.C.Khanna, H.Umezawa Spontaneous Breakdown of Isospin Symmetry in Nuclei and Isobaric Analog States
doi: 10.1103/PhysRevC.50.3135
1994KH04 Nucl.Phys. A577, 369c (1994) F.C.Khanna, H.Umezawa, I.Danchev Gamow-Teller States and Broken SU(4) Symmetry
doi: 10.1016/0375-9474(94)90882-6
1994UM01 Phys.Rev. C49, 2311 (1994) Deep Inelastic Scattering on the Deuteron in the Bethe-Salpeter Formalism: Scalar meson exchange NUCLEAR STRUCTURE 2H; calculated structure function relative to nucleon. Fully convariant field theoretical approach, deep inelastic scattering.
doi: 10.1103/PhysRevC.49.2311
1994UM03 Z.Phys. A348, 211 (1994) A.Yu.Umnikov, F.C.Khanna, L.P.Kaptari On the Unfolding of Neutron Structure Functions from the Deuteron Data NUCLEAR STRUCTURE 2,1H; analyzed structure function data. 1n deduced structure function.
doi: 10.1007/BF01291919
1994UM04 Phys.Lett. 334B, 163 (1994) A.Yu.Umnikov, L.P.Kaptari, K.Yu.Kazakov, F.C.Khanna A Relativistic Approach to Deep Inelastic Scattering on the Deuteron NUCLEAR STRUCTURE 2H; calculated structure function. Covariant field theoretical approach, realistic NN-interaction.
doi: 10.1016/0370-2693(94)90605-X
1991TR06 Few-Body Systems 11, 25 (1991) Disintegration of the Deuteron by Reactor Antineutrinos NUCLEAR REACTIONS 2H(ν-bar, X), E=reactor; calculated disintegration σ.
1990DY01 Phys.Rev. C41, 828 (1990) Reaction 2He(e, e')pn Near Breakup Threshold at Backward Angles NUCLEAR REACTIONS 2H(e, e'p), E ≈ threshold; calculated σ(θ=180°), σ(θ, E(e')). Nonrelativistic model, isobar currents.
doi: 10.1103/PhysRevC.41.828
1990DY02 Nucl.Phys. A507, 560 (1990) e-d Scattering and Δ-Isobars in the Deuteron NUCLEAR REACTIONS 2H(e, e), E not given; calculated form factor. Elastic, inclusive inelastic scattering, nucleon-nucleon interaction with Δ-isobar. NUCLEAR STRUCTURE 2H; calculated structure function. Elastic, inclusive inelastic scattering, nucleon-nucleon interaction with Δ-isobar.
doi: 10.1016/0375-9474(90)90171-H
1990DY03 Phys.Rev. C41, 2438 (1990) Deuteron Form Factors and the Short-Range Structure of the Deuteron NUCLEAR STRUCTURE 2H; calculated form factors, structure function.
doi: 10.1103/PhysRevC.41.2438
1990DY05 Nucl.Phys. A516, 549 (1990) The Δ-Isobars in the Deuteron NUCLEAR STRUCTURE 2H; calculated magnetic, charge form factors, structure function.
doi: 10.1016/0375-9474(90)90127-8
1986DY01 Phys.Rev.Lett. 56, 1448 (1986) Tensor Polarization of the Deuteron in Elastic e-d Scattering NUCLEAR STRUCTURE 2H; calculated nucleon-nucleon, isobar-isobar component percentage in wave function. NUCLEAR REACTIONS 2H(e, e), E not given; calculated tensor polarization t20 vs momentum transfer; deduced QCD testing ambiguity.
doi: 10.1103/PhysRevLett.56.1448
1986MC10 Nucl.Phys. A456, 577 (1986) W.J.McDonald, R.N.MacDonald, W.C.Olsen, R.Dymarz, F.Khanna, L.Antonuk, J.M.Cameron, P.Kitching, G.C.Neilson, D.M.Sheppard, D.A.Hutcheon, C.A.Miller, J.Kallne Quasi-Free Nucleon Scattering on 16O NUCLEAR REACTIONS 16O(p, 2p), (p, pn), E=505 MeV; measured σ(E1, θ1, θ2). H2O target.
doi: 10.1016/0375-9474(86)90076-X
1984TO06 J.Phys.(Paris), Colloq.C4, 519 (1984); See 1984To15 On l-Forbidden M1 and GT Transitions in A = 39
1984TO15 J.Phys.(Paris), Colloq.C-4, 519 (1984) On l-Forbidden M1 and GT Transitions in A = 39 NUCLEAR STRUCTURE A=39; calculated isovector single particle matrix element, l-allowed transition corrections. One boson exchange model.
1983TO08 Nucl.Phys. A399, 334 (1983) Corrections to the Single-Particle M1 and Gamow-Teller Matrix Elements NUCLEAR STRUCTURE A=3, 15, 17, 39, 41; calculated magnetic moment, M1, Gamow-Teller matrix element corrections. Second-order core polarization, isobar, meson exchange currents.
doi: 10.1016/0375-9474(83)90252-X
1981TO03 Nucl.Phys. A356, 445 (1981) Meson-Exchange Currents in Thermal n - 3He Radiative Capture NUCLEAR REACTIONS 3He(n, γ), E=thermal; calculated σ. Oscillator wave functions, meson exchange effects.
doi: 10.1016/0375-9474(81)90200-1
1981TO16 Nucl.Phys. A372, 331 (1981) Role of 2p-2h States in Weak 0+-0- Transitions in A = 16 Nuclei NUCLEAR REACTIONS 16O(μ-, ν), E at rest; calculated muon capture rate. Meson exchange, second-order perturbation theory. RADIOACTIVITY 16N; calculated β-decay rate. Meson exchange, second-order perturbation theory.
doi: 10.1016/0375-9474(81)90039-7
1981VA07 J.Phys.(London) G7, 1029 (1981) M.G.Vassanji, F.C.Khanna, I.S.Towner A Calculation of the Deuteron Static Moments in a One-Boson-Exchange Model NUCLEAR STRUCTURE 2H; calculated μ, quadrupole moment, rms radius. One-boson exchange model.
doi: 10.1088/0305-4616/7/8/009
1978LE03 Can.J.Phys. 56, 149 (1978) Electromagnetic Field in the Nucleus and the Salam-Strathdee Phase Transitions NUCLEAR MOMENTS 5Li, 13N, 17F, 19Ne, 31P, 35Ar, 41Sc, 63Cu, 89Y, 93Nb, 121Sb, 209Bi; calculated μ.
doi: 10.1139/p78-021
1977MC05 Nucl.Phys. A281, 325 (1977) A.B.McDonald, E.D.Earle, M.A.Lone, F.C.Khanna, H.C.Lee Doubly Radiative Thermal Neutron Capture in 2H and 16O: Experiment and Theory NUCLEAR REACTIONS 2H, 16O(n, γ), E=th; measured σ(Eγ); deduced upper limit for σ(2γ). 17O levels deduced γ-branching. Enriched target.
doi: 10.1016/0375-9474(77)90029-X
1977TO04 Nucl.Phys. A277, 285 (1977) I.S.Towner, F.C.Khanna, O.Hausser Magnetic Moments in N = 126 Isotones and Core Polarisation Blocking NUCLEAR MOMENTS 209Bi, 210Po, 211At, 212Rn, 213Fr, 214Ra; calculated core-polarization corrections to g.
doi: 10.1016/0375-9474(77)90314-1
1976HA37 Phys.Lett. 63B, 279 (1976) O.Hausser, J.R.Beene, A.B.McDonald, T.K.Alexander, E.D.Earle, F.C.Khanna, I.S.Towner, G.A.Beer, A.Olin Precise Magnetic Moments of (h9/2)n Proton States NUCLEAR REACTIONS 205Tl(12C, 4n), E=71-80 MeV; measured γγ(θ, H, t). Fr, Ra recoils in Tl Knight shift. 213Fr deduced levels, T1/2, B(λ), g. 214Ra level deduced g.
doi: 10.1016/0370-2693(76)90263-X
1976HA56 Nucl.Phys. A273, 253 (1976) O.Hausser, T.K.Alexander, J.R.Beene, E.D.Earle, A.B.McDonald, F.C.Khanna, I.S.Towner Magnetic Moments and Half-Lives of Isomeric States in Polonium Isotopes NUCLEAR REACTIONS 206,207,208Pb(α, 2n), E=35-30 MeV; 194Pt(12C, 4n), E=80 MeV; measured Iγ(γ, H, t). 202,208,209,210Po levels deduced g, T1/2. 209Bi deduced quadrupole moment. Natural Pb, enriched 194Pt targets. Ge(Li) detectors. RADIOACTIVITY 210At; measured γγ(t). 210Po levels deduced T1/2.
doi: 10.1016/0375-9474(76)90312-2
1976HA62 Hyperfine Interactions 2, 334 (1976) O.Hausser, T.K.Alexander, J.R.Beene, E.D.Earle, A.B.McDonald, F.C.Khanna, I.S.Towner Measurements of Accurate g-Factors in Translead Nuclei with Heavy-Ion Induced Reactions
1976LE24 Phys.Rev. C14, 1306 (1976) Doubly Radiative np Capture NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated σ(2γ).
doi: 10.1103/PhysRevC.14.1306
1976LE27 Phys.Lett. 65B, 201 (1976) H.C.Lee, F.C.Khanna, M.A.Lone, A.B.McDonald Doubly Radiative Neutron Capture by 2H, 3He, 16O and 208Pb NUCLEAR REACTIONS 2H, 3He, 16O, 208Pb(n, γ), E=th; calculated σ(2γ), σ(2γ)/σ(γ).
doi: 10.1016/0370-2693(76)90162-3
1976MC02 Nucl.Phys. A258, 152 (1976) A.B.McDonald, T.K.Alexander, C.Broude, J.S.Forster, O.Hausser, F.C.Khanna, I.V.Mitchell Lifetime of the 1.89 MeV 2+ Level of 18Ne: Two-Body Contributions to E2 Transition Rates NUCLEAR REACTIONS 3He(16O, nγ), E=38 MeV; measured nγ-coin, Doppler broadened line shape. 18Ne level deduced T1/2, B(E2).
doi: 10.1016/0375-9474(76)90536-4
1975SE06 Phys.Lett. 56B, 1 (1975) The Incoherent Neutron Scattering Length of 3He NUCLEAR REACTIONS 3He(n, n); calculated neutron scattering length.
doi: 10.1016/0370-2693(75)90484-0
1974HA20 Nucl.Phys. A221, 77 (1974) Distribution of Dipole and Spin-Dipole Strength in Nuclei NUCLEAR STRUCTURE 56Ni, 90Zr, 132Sn, 208Pb; calculated levels, dipole, spin-dipole strength.
doi: 10.1016/0375-9474(74)90100-6
1973HA53 Phys.Lett. 47B, 8 (1973) Origin of Electric Quadrupole Enhancements in A = 17 Nuclei NUCLEAR STRUCTURE A=17; calculated enhancements of electric quadrupole matrix elements.
doi: 10.1016/0370-2693(73)90555-8
1972HA59 Nucl.Phys. A194, 113 (1972) Gamma Decay of Low-Lying States Near the 208Pb Closed Shell NUCLEAR REACTIONS 204,206,207,208Pb, 209Bi(α, α'γ), E=15-18 MeV; 204,206,207,208Pb, 209Bi(16O, 16O'γ), E=69-80 MeV; measured Eγ, σ(Eγ), DSA. 208Pb(7Li, α2nγ), 208Pb(7Li, 6Li), E=28-31.5 MeV; measured αγ-coin, Eγ, DSA. 204,206,207,208,209Pb, 209Bi deduced B(EL), B(ML), T1/2. Enriched, natural targets.
doi: 10.1016/0375-9474(72)91055-X
1971KH01 Nucl.Phys. A164, 612 (1971) Effective Operators for the Nuclear Shell Model (III). E2 Effective Charge with Realistic Reaction Matrices NUCLEAR STRUCTURE 15O, 41Ca, 41Sc, 39Ca, 39K, 17F, 17O, 15N; calculated E2 effective charges. Time-dependent perturbation theory, realistic reaction matrices.
doi: 10.1016/0375-9474(71)90783-4
1971KH02 Nucl.Phys. A165, 475 (1971) High-Energy Electron Scattering and Nuclear Structure NUCLEAR REACTIONS 3H, 3,4He, 16O, 40,48Ca(e, e), E=250 MeV; calculated charge form factors.
doi: 10.1016/0375-9474(71)90462-3
1970HA49 Nucl.Phys. A155, 337 (1970) Effective Operators in the Nuclear Shell Model (II). Phenomenology of E2 Operators NUCLEAR STRUCTURE 18O, 18F, 18,20Ne; calculated B(E2), reduced matrix elements. Coupling operator, E2 effective charge.
doi: 10.1016/0375-9474(70)90900-0
1970HA75 Nucl.Phys. A152, 588 (1970) Effective operators in the nuclear shell model: (I). General theory
doi: 10.1016/0375-9474(70)90935-8
1969SE04 Nucl.Phys. A130, 342 (1969) A Projection Operator for the Spurious Centre-of-Mass Motion NUCLEAR STRUCTURE 16O; calculated levels.
doi: 10.1016/0375-9474(69)90735-0
1961KH03 Phys.Rev. 124, 515 (1961) F.C.Khanna, Y.C.Tang, K.Wildermuth Li6 Plus Neutron Configuration in Li7 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.124.515
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