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NSR database version of May 20, 2024.

Search: Author = D.Lu

Found 55 matches.

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2022CA06      Phys.Rev. C 105, 034304 (2022)

Y.Cao, D.Lu, Y.Qian, Z.Ren

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
Citations: PlumX Metrics

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
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2019SU11      Phys.Rev. C 99, 054604 (2019)

X.Sun, J.Chen, D.Lu

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
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2019SU26      Phys.Rev. C 100, 054605 (2019)

X.Sun, J.Chen, D.Lu

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
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2018SU01      Chin.Phys.C 42, 014101 (2018)

X-W.Sun, J.Chen, D.-H.Lu

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
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2018SU18      Phys.Rev. C 98, 024607 (2018)

X.Sun, J.Chen, D.Lu

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
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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
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2017SU24      Phys.Rev. C 96, 024614 (2017)

X.Sun, D.Lu

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
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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
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2004CH44      Chin.Phys.Lett. 21, 1459 (2004)

W.-F.Chen, D.-H.Lu

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
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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
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2001LU01      Nucl.Phys. A684, 296c (2001)

D.H.Lu, S.N.Yang, A.W.Thomas

On the Role of the Pion Cloud in Nucleon Electromagnetic Form Factors

doi: 10.1016/S0375-9474(01)00483-3
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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
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2000HS01      Phys.Rev. C61, 068201 (2000)

S.S.Hsiao, D.H.Lu, S.N.Yang

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
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2000LU06      J.Phys.(London) G26, L75 (2000)

D.H.Lu, S.N.Yang, A.W.Thomas

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
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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
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1999LU01      Chin.Phys.Lett. 16, 93 (1999)

D.-H.Lu, L.-M.Yang

Microscopic Treatment for the Degree of Freedom Beyond the S-D Model Space

doi: 10.1088/0256-307X/16/2/006
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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
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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
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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
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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
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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
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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
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1998LU14      Phys.Rev. C58, 2588 (1998)


Self-Consistent Structure of Correlated 2+ Nucleon Pairs

doi: 10.1103/PhysRevC.58.2588
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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
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1998LU18      Comput.Phys.Commun. 108, 75 (1998)

D.Lu, G.He, R.H.Landau

PiN: Computation of pion-nucleon scattering and bound states with the color dielectric quark model

doi: 10.1016/S0010-4655(97)00122-7
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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
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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
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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
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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)

D.Lu, S.C.Phatak, R.H.Landau

Pion-Nucleon Scattering and the πNN Coupling Constant in the Chiral Color Dielectric Model

doi: 10.1103/PhysRevC.51.2207
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1995LU07      Nucl.Phys. A585, 381c (1995)

D.Lu, S.C.Phatak, R.H.Landau

Applications of the Chiral Color Dielectric Model to Low Energy Meson-Baryon Interactions

doi: 10.1016/0375-9474(94)00619-X
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1995LU12      Phys.Rev. C52, 1662 (1995)

D.Lu, R.H.Landau, S.C.Phatak

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
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1994LU01      Phys.Rev. C49, 878 (1994)

D.H.Lu, R.H.Landau

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
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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
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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)

D.Lu, L.Chu, C.Wang

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)

L.M.Yang, D.H.Lu, Z.N.Zhou

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
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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
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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
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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
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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
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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
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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
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1962LU02      Bull.Am.Phys.Soc. 7, No.4, 353, XA9 (1962)

D.C.Lu, G.Schupp

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)

D.C.Lu, R.S.Dingus

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
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1961LU05      IS-272 (1961); Nuclear Sci.Abstr. 17, 920, Abstr.7079 (1963)

D.C.Lu, G.Schupp

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
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1960ST07      Phys.Rev. 117, 1044 (1960)

M.G.Stewart, D.C.Lu

Nuclear Levels of Cs133

NUCLEAR STRUCTURE 133Ba; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.117.1044
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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)

D.C.Lu, M.L.Wiedenbeck

Summation of γ-Ray Energies with a Single-Crystal Spectrometer

doi: 10.1103/PhysRev.94.501
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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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Note: The following list of authors and aliases matches the search parameter D.Lu: , D.C.LU, D.H.LU