NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = D.Lu Found 55 matches. 2022CA06 Phys.Rev. C 105, 034304 (2022) Uncertainty analysis for the nuclear liquid drop model and implications for the symmetry energy coefficients ATOMIC MASSES 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315U; calculated binding energies using liquid drop model (LD), including Wigner energy term, and associated statistical uncertainties using Monte Carlo bootstrap approach based on nonparametric sampling. Comparison with available experimental evaluated masses from AME2020.
doi: 10.1103/PhysRevC.105.034304
2020YE01 Phys.Rev. C 101, 034915 (2020) Y.Ye, Y.Wang, Q.Li, D.Lu, F.Wang Beam energy dependence of cumulants of the net-baryon, net-charge, and deuteron multiplicity distributions i Au + Au collisions at√ sNN = 3.0 - 5.0 GeV
doi: 10.1103/PhysRevC.101.034915
2019SU11 Phys.Rev. C 99, 054604 (2019) Neutron-proton mass splitting and pygmy dipole resonance in 208Pb NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated binding energies, charge radii, nuclear density, and other bulk properties of the nuclear matter. Comparison with experimental values. 48Ca, 208Pb; calculated neutron skin thicknesses, transition strength distribution of the electric dipole resonance, centroid energies of the giant dipole resonance (GDR) and pygmy dipole resonances (PDR). Comparison with experimental data. 208Pb; calculated dominating excited states in the pygmy dipole resonance of with the inclusion of δ meson, symmetry energy, relationship between the neutron-proton effective mass splitting and the difference of the centroid energies of GDR and PDR. Random phase approximation method, with the effect of the neutron-proton mass splitting treated in the framework of relativistic mean field theory by including the scalar-isovector meson δ explicitly.
doi: 10.1103/PhysRevC.99.054604
2019SU26 Phys.Rev. C 100, 054605 (2019) Effects of the γ-soft isomeric states on the giant monopole resonances in even-even cadmium isotopes 110, 112, 114, 116Cd NUCLEAR STRUCTURE 110,112,114,116Cd; calculated potential energy surfaces in (β, γ) plane, strength functions of giant monopole resonances (GMRs), β and γ deformation parameters, centroid energies of the GMRs built on isomeric states in the Cd isotopes. Discussed contribution of shape isomer mixing to the GMR strength in an excited nucleus. Quasiparticle random phase approximation (QRPA), implemented with a finite amplitude method. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.054605
2018SU01 Chin.Phys.C 42, 014101 (2018) Stagnancy of the pygmy dipole resonance NUCLEAR STRUCTURE 58,60,62,64,66,68,70,72,74,76,78Ni; calculated pygmy dipole resonance (PDR) parameters of nickel isotopes using the deformed random phase approximation; deduced a linear correlation between PDR integral σ and neutron skin thickness when the excess neutrons lie in pf orbits.
doi: 10.1088/1674-1137/42/1/014101
2018SU18 Phys.Rev. C 98, 024607 (2018) Pygmy dipole resonance built on the shape-isomeric state in 68Ni NUCLEAR REACTIONS 68Ni(γ, X), E*=7-35 MeV; calculated virtual γ photoabsorption σ for spherical ground state and prolate isomeric state of 68Ni using deformed relativistic random phase approximation method. 68Ni; calculated potential energy surface (PES) contour in (β, γ) plane, radial distributions of dominant states contributing to pygmy dipole resonance (PDR) and giant dipole resonance (GDR), pygmy dipole resonance energy of spherical ground state and prolate isomeric state; deduced effect of the shape-coexistence isomeric state in 68Ni. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.024607
2018YE05 Phys.Rev. C 98, 054620 (2018) Y.Ye, Y.Wang, J.Steinheimer, Y.Nara, H.-j.Xu, P.Li, D.Lu, Q.Li, H.Stoecker Cumulants of the baryon number from central Au+Au collision at Elab = 1.23GeV/nucleon reveal the nuclear mean-field potentials NUCLEAR REACTIONS 197Au(197Au, X), E=1.23 GeV/nucleon; calculated yield distributions of all baryons as functions of the reduced longitudinal and transverse rapidities, rapidity and time dependence for the cumulants and their ratios of free baryons, clustered baryons, and free protons using the Ultrarelativistic quantum molecular dynamics (UrQMD) and the JAM model, with soft momentum dependent (SM), the hard momentum-dependent (HM), and the hard without momentum-dependent (H) mean-field potentials. Relevance to experiments of HADES Collaboration at GSI, and STAR Collaboration at BNL.
doi: 10.1103/PhysRevC.98.054620
2017SU24 Phys.Rev. C 96, 024614 (2017) Implementation of a finite-amplitude method in a relativistic meson-exchange model NUCLEAR STRUCTURE 110,112,114,116Cd, 208Pb; calculated isoscalar giant monopole resonance (ISGMR) strength distributions, and compared with available experimental data. 60Ni; calculated electric dipole resonance strength distribution. Finite-amplitude method (FMA) and large scale random phase approximation (RPA) calculations.
doi: 10.1103/PhysRevC.96.024614
2011TS06 Phys.Rev. C 83, 065208 (2011) K.Tsushima, D.H.Lu, G.Krein, A.W.Thomas J/ψ-nuclear bound states
doi: 10.1103/PhysRevC.83.065208
2004CH44 Chin.Phys.Lett. 21, 1459 (2004) In-Medium Nucleon Electromagnetic Form Factors in Vector Meson Dominance Model NUCLEAR STRUCTURE 1n, 1H; calculated in-medium form factors.
doi: 10.1088/0256-307X/21/8/013
2003SO26 Phys.Rev. C 68, 055201 (2003) H.Q.Song, R.K.Su, D.H.Lu, W.L.Qian Strange hadronic matter with a weak Y-Y interaction
doi: 10.1103/PhysRevC.68.055201
2001LU01 Nucl.Phys. A684, 296c (2001) On the Role of the Pion Cloud in Nucleon Electromagnetic Form Factors
doi: 10.1016/S0375-9474(01)00483-3
2001TS01 Nucl.Phys. A680, 280c (2001) K.Tsushima, A.Sibirtsev, K.Saito, A.W.Thomas, D.H.Lu Effect of Changes in Meson Properties in a Nuclear Medium: J/ψ dissociation in nuclear matter, and meson-nucleus bound states
doi: 10.1016/S0375-9474(00)00428-0
2000HS01 Phys.Rev. C61, 068201 (2000) Pseudovector Versus Pseudoscalar Coupling in Kaon Photoproduction Reexamined NUCLEAR REACTIONS 1H(γ, K+X), E=0.9-2 GeV; calculated hyperon production associated σ, σ(θ). Comparison of coupling schemes. Comparisons with data.
doi: 10.1103/PhysRevC.61.068201
2000LU06 J.Phys.(London) G26, L75 (2000) Scaling Law for the Electromagnetic Form Factors of the Proton NUCLEAR STRUCTURE 1H; calculated ratio of electric and magnetic form factors as a function of square momentum transfer. Comparison with data and between different theoretical models.
doi: 10.1088/0954-3899/26/6/101
2000LU12 Chin.Phys.Lett. 17, 562 (2000) D.-H.Lu, L.-M.Yang, W.-Z.Deng, X.-L.Chen, J.-W.Zhang An Understanding of the Meaning Behind Boson-Description in the Collective Motion of Nuclei
1999LE25 Phys.Rev. D60, 034014 (1999) D.B.Leinweber, D.H.Lu, A.W.Thomas Nucleon Magnetic Moments Beyond the Perturbative Chiral Regime NUCLEAR STRUCTURE 1n, 1H; calculated magnetic moments; deduced quark mass dependence. Chiral perturbation theory, cloudy bag model.
doi: 10.1103/PhysRevD.60.034014
1999LU01 Chin.Phys.Lett. 16, 93 (1999) Microscopic Treatment for the Degree of Freedom Beyond the S-D Model Space
doi: 10.1088/0256-307X/16/2/006
1999LU11 Phys.Rev. C60, 068201 (1999) D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito Electromagnetic Form Factors of the Bound Nucleon NUCLEAR STRUCTURE 4He, 16O, 40Ca, 208Pb; calculated bound proton electric, magnetic form factors.
doi: 10.1103/PhysRevC.60.068201
1999SA03 Phys.Rev. C59, 1203 (1999) K.Saito, K.Tsushima, D.H.Lu, A.W.Thomas ω-Nucleus Bound States in the Walecka Model NUCLEAR STRUCTURE 6He, 11Be, 16O, 26Mg, 40Ca, 90Zr, 208Pb; calculated ω-meson bound state energies. Walecka model, comparison with quark-meson coupling model.
doi: 10.1103/PhysRevC.59.1203
1999TS03 Phys.Rev. C59, 2824 (1999) K.Tsushima, D.H.Lu, A.W.Thomas, K.Saito, R.H.Landau Charmed Mesic Nuclei: Bound D and D(bar) States with 208Pb NUCLEAR STRUCTURE 208Pb; calculated bound D-meson states energies, densities, wavefunctions.
doi: 10.1103/PhysRevC.59.2824
1998LU01 Phys.Lett. 417B, 217 (1998) D.H.Lu, A.W.Thomas, K.Tsushima, A.G.Williams, K.Saito In-Medium Electron-Nucleon Scattering
doi: 10.1016/S0370-2693(97)01385-3
1998LU03 Phys.Rev. C57, 2628 (1998) D.H.Lu, A.W.Thomas, A.G.Williams Electromagnetic Form Factors of the Nucleon in an Improved Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors; deduced Lorentz contraction effect. Cloudy bag model. Comparisons with data.
doi: 10.1103/PhysRevC.57.2628
1998LU06 Nucl.Phys. A634, 443 (1998) D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito Medium Dependence of the Bag Constant in the Quark-Meson Coupling Model
doi: 10.1016/S0375-9474(98)00181-X
1998LU14 Phys.Rev. C58, 2588 (1998) Self-Consistent Structure of Correlated 2+ Nucleon Pairs
doi: 10.1103/PhysRevC.58.2588
1998LU16 Phys.Lett. 441B, 27 (1998) D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito The Neutron Charge Form Factor in Helium-3 NUCLEAR STRUCTURE 1n, 3He; calculated neutron charge form factor; deduced medium effects.
doi: 10.1016/S0370-2693(98)01196-4
1998LU18 Comput.Phys.Commun. 108, 75 (1998) PiN: Computation of pion-nucleon scattering and bound states with the color dielectric quark model
doi: 10.1016/S0010-4655(97)00122-7
1998MA35 Nucl.Phys. A635, 497 (1998) W.X.Ma, D.H.Lu, A.W.Thomas, Z.P.Li Q2-Dependence of the Gerasimov-Drell-Hearn Sum Rule
doi: 10.1016/S0375-9474(98)00202-4
1998TS14 Phys.Lett. 443B, 26 (1998) K.Tsushima, D.H.Lu, A.W.Thomas, K.Saito Are η- and ω-Nuclear States Bound ? NUCLEAR STRUCTURE 6He, 11B, 16O, 26Mg, 40Ca, 90Zr, 208Pb; calculated η, ω meson single-particle energies, widths; deduced bound states.
doi: 10.1016/S0370-2693(98)01336-7
1997LU04 Phys.Rev. C55, 3108 (1997) D.H.Lu, A.W.Thomas, A.G.Williams Chiral Bag Model Approach to Δ Electroproduction
doi: 10.1103/PhysRevC.55.3108
1996YU07 High Energy Phys. and Nucl.Phys. (China) 20, 32 (1996) J.Yuan, M.Lu, D.Lu, Q.Chen, Z.Sun Study of Stretched States Populated by 56, 57Fe, 59Co(α, d) 58, 59Co, 61Ni Reactions
1995LU02 Phys.Rev. C51, 2207 (1995) Pion-Nucleon Scattering and the πNN Coupling Constant in the Chiral Color Dielectric Model
doi: 10.1103/PhysRevC.51.2207
1995LU07 Nucl.Phys. A585, 381c (1995) Applications of the Chiral Color Dielectric Model to Low Energy Meson-Baryon Interactions
doi: 10.1016/0375-9474(94)00619-X
1995LU12 Phys.Rev. C52, 1662 (1995) Kaon Photoproduction in the Color-Dielectric Model NUCLEAR REACTIONS 1H(γ, X), E=1.2, 1.4 GeV; calculated σ(θ) vs E for K+Λ, Λ polarization vs θ. Momentum-projected color dielectric quark model.
doi: 10.1103/PhysRevC.52.1662
1994LU01 Phys.Rev. C49, 878 (1994) Deep Pionic Bound States in a Nonlocal Optical Potential NUCLEAR STRUCTURE 16,18O, 40,44Ca, 108Ag, 208Pb, 209Bi; calculated pionic level shifts, widths. ATOMIC PHYSICS, Mesic-Atoms 208Pb; calculated pionic level shifts, widths, 1s, 2s, 2p state probability density, wave functions. Nonlocal, microscopic optical potential.
doi: 10.1103/PhysRevC.49.878
1994LU10 Phys.Rev. C50, 3037 (1994) D.H.Lu, T.Mefford, R.H.Landau, G.Song Coulomb Plus Nuclear Scattering in Momentum Space for Coupled Angular Momentum States NUCLEAR REACTIONS 3He(polarized p, p), E=500 MeV; analyzed σ(θ), analyzing power vs θ. Generalized Blatt-Biedenharn phase shift parametrization procedure. Coulomb plus short-range potentials.
doi: 10.1103/PhysRevC.50.3037
1993YU07 Chin.J.Nucl.Phys. 15, No 3, 215 (1993) J.Yuan, M.Lu, Q.Chen, D.Lu, Z.Sun Search for Stretched High-Spin States Populated by 56,57Fe, 59Co(α, d)58,59Co, 61Ni Reactions NUCLEAR REACTIONS 59Co, 56,57Fe(α, d), E=35 MeV; measured deuteron spectra, σ(θ). 59,58Co, 61Ni deduced stretched high spin states population features.
1991LU05 Chin.J.Nucl.Phys. 13, No 1, 59 (1991) Separable Nucleon-Nucleon Potential with Off-Shell Information NUCLEAR STRUCTURE 3H; calculated binding energy. 2H; calculated binding energy, quadrupole moment, D-state probability, radius; deduced separable nucleon-nucleon potential features.
1984YA05 Nucl.Phys. A421, 229c (1984) Microscopic Investigation of IBM and IBFM NUCLEAR STRUCTURE 110Cd, 112,114Sn, 148,150,152,154,156Sm; calculated levels. Interacting boson, boson-fermion models.
doi: 10.1016/0375-9474(84)90347-6
1980LU11 Phys.Rev.Lett. 45, 1066 (1980) D.C.Lu, L.Delker, G.Dugan, C.S.Wu, A.J.Caffrey, Y.T.Cheng, Y.K.Lee New High-Accuracy Measurement of the Pionic Mass NUCLEAR REACTIONS Ti, P(π-, X), E at rest; measured pionic X-rays; deduced pionic mass. ATOMIC PHYSICS, Mesic-Atoms Ti, P(π-, X), E at rest; measured pionic X-rays; deduced pionic mass.
doi: 10.1103/PhysRevLett.45.1066
1979DE05 Phys.Rev.Lett. 42, 89 (1979) L.Delker, G.Dugan, C.S.Wu, D.C.Lu, A.J.Caffrey, Y.T.Cheng, Y.K.Lee Experimental Verification of the Relativistic Fine-Structure Term of the Klein-Gordon Equation in Pionic Titanium Atoms ATOMIC PHYSICS, Mesic-Atoms Ti; measured pionic X-rays; deduced energy difference between 5g→4f, 5f→4d transitions. Comparison with prediction of Klein-Gordon equation. Large-aperture, high-resolution, bent-crystal spectrometer.
doi: 10.1103/PhysRevLett.42.89
1975CH35 Nucl.Phys. A254, 381 (1975) S.C.Cheng, Y.Asano, M.Y.Chen, G.Dugan, E.Hu, L.Lidofsky, V.Hughes, D.Lu K- Mass from Kaonic Atoms ATOMIC PHYSICS, Mesic-Atoms 208Pb(K-, X); measured circular transition energies. K- deduced mass.
doi: 10.1016/0375-9474(75)90224-9
1975CH36 Nucl.Phys. A254, 413 (1975) M.Y.Chen, Y.Asano, S.C.Cheng, G.Dugan, E.Hu, L.Lidofsky, V.Hughes, D.Lu E2 Dynamic Mixing in p-Bar and K- Atoms of 238U ATOMIC PHYSICS 238U(K-, X), (p-bar, X); measured atomic transitions; deduced dynamic E2 shift.
doi: 10.1016/0375-9474(75)90227-4
1975DU12 Nucl.Phys. A254, 396 (1975) G.Dugan, Y.Asano, M.Y.Chen, S.C.Cheng, E.Hu, L.Lidofsky, W.Patton, C.S.Wu, V.Hughes, D.Lu Mass and Magnetic Moment of Σ- by the Exotic Atom Method ATOMIC PHYSICS 208Pb(Σ-, X-ray); measured Σ- X-rays. Σ- deduced mass, μ. Natural target.
doi: 10.1016/0375-9474(75)90225-0
1975HU12 Nucl.Phys. A254, 403 (1975) E.Hu, Y.Asano, M.Y.Chen, S.C.Cheng, G.Dugan, L.Lidofsky, W.Patton, C.S.Wu, V.Hughes, D.Lu Mass and Magnetic Moment of the Antiproton by the Exotic Atom Method ATOMIC PHYSICS 208Pb, U(p-bar, X-ray); measured antiprotonic X-rays. p-bar deduced mass, μ. Natural target.
doi: 10.1016/0375-9474(75)90226-2
1962LU02 Bull.Am.Phys.Soc. 7, No.4, 353, XA9 (1962) Internal Conversion Coefficients of the 2+-0+, E2 Transitions in Even-Even Sm152 and Gd152 NUCLEAR STRUCTURE 152Eu; measured not abstracted; deduced nuclear properties.
1962LU03 Phys.Letters 3, 44 (1962) E2 Internal Conversion Coefficients for Rotational Transitions NUCLEAR STRUCTURE 152Eu, 154Eu, 160Tb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(62)90195-6
1961LU05 IS-272 (1961); Nuclear Sci.Abstr. 17, 920, Abstr.7079 (1963) Internal Conversion Coefficients of the 2+-0+, E2 Transitions in Even-Even Sm152 and Gd152 NUCLEAR STRUCTURE 152Eu; measured not abstracted; deduced nuclear properties.
1960LU05 Phys.Rev. 119, 286 (1960) Accurate Method for Measuring Internal Conversion Coefficients NUCLEAR STRUCTURE 111Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.119.286
1960ST07 Phys.Rev. 117, 1044 (1960) Nuclear Levels of Cs133 NUCLEAR STRUCTURE 133Ba; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.117.1044
1959LU65 Bull.Am.Phys.Soc. 4, No.4, 277, U2 (1959) Accurate Method for Measuring Internal Conversion Coefficients
1958LU65 ISC-1048, p.15 (1958)
1958ST31 Bull.Am.Phys.Soc. 3, No.3, 208, S2 (1958) M.G.Stewart, D.C.Lu, F.M.Clikeman Decay of Ba133
1954LU22 Phys.Rev. 94, 501 (1954) Summation of γ-Ray Energies with a Single-Crystal Spectrometer
doi: 10.1103/PhysRev.94.501
1954LU35 Phys.Rev. 95, 121 (1954) D.C.Lu, W.H.Kelly, M.L.Wiedenbeck Decay Schemes of Cd114 and Te125
doi: 10.1103/PhysRev.95.121
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