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NSR database version of May 24, 2024.

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2022LE15      Eur.Phys.J. A 58, 252 (2022)

T.-S.H.Lee, S.Sakinah, Y.Oh

Models of J/Ψ photo-production reactions on the nucleon

doi: 10.1140/epja/s10050-022-00901-9
Citations: PlumX Metrics


2021KI10      Phys.Rev. C 104, 045202 (2021)

S.-H.Kim, T.-S.H.Lee, S.-i.Nam, Y.Oh

Dynamical model of φ meson photoproduction on the nucleon and 4He

NUCLEAR REACTIONS 1H(γ, pφ), E=1-400 GeV; calculated total σ(E) forphotoproduction of ρ0, φ, and J/ψ, total σ(E). 1H(γ, pφ), E=1.985-2.815 GeV; calculated differential σ(θ, E), total σ(E), and compared with experimental data from CLAS Collaboration and other experiments. 4He(γ, αφ), E=1.5-3 GeV; calculated differential σ(θ, E), and compared with experimental data from LEPS Collaboration and other experiments. Dynamical model based on a Hamiltonian describing production mechanisms by the Pomeron and meson exchanges.

doi: 10.1103/PhysRevC.104.045202
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2021LE09      Phys.Lett. B 817, 136301 (2021)

T.-G.Lee, O.Bayrak, C.-Y.Wong

Pocket resonances in low-energy antineutron reactions with nuclei

NUCLEAR REACTIONS C, Ag, Pb(n-bar, X), E=0.001-10 MeV; analyzed available data; deduced resonances using Bethe-Landau power law, antineutron-nucleus annihilation σ.

doi: 10.1016/j.physletb.2021.136301
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2019RO17      Phys.Rev. C 100, 045503 (2019)

N.Rocco, S.X.Nakamura, T.-S.H.Lee, A.Lovato

Electroweak pion production on nuclei within the extended factorization scheme

NUCLEAR REACTIONS 12C(e, e'π), E=620, 730, 961, 1650 MeV; 12C(ν, ν'), (ν, μ-), E=1.0 GeV; 1H(e, e'π0), (e, e'π+), Q2=0.4, 1.76, 2.95 MeV; 1H(ν, μ-π+), 1n(ν, μ-π0), (ν, μ-π+), E<2.25 GeV muon neutrinos; calculated double differential σ(E) using the dynamical coupled-channel (DCC) ANL-Osaka model and Metropolis Monte Carlo integration techniques for generating the matrix elements of current operators relevant to pion production off the nucleon. Comparison with experimental data from ANL and BNL.

doi: 10.1103/PhysRevC.100.045503
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2019WU10      Phys.Rev. C 100, 035206 (2019)

J.-J.Wu, T.-S.H.Lee, B.-S.Zou

Nucleon resonances with hidden charm in ψp reactions

doi: 10.1103/PhysRevC.100.035206
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2018LE09      Phys.Rev. C 97, 054617 (2018)

T.-G.Lee, C.-Yi.Wong

Optical model potential analysis of n(-bar)A and nA interactions

NUCLEAR REACTIONS C, Al, Fe, Cu, Ag, Sn, Pb(n-bar, X), (n, X), (p-bar, X), E at 50-500 MeV/c; analyzed experimental data for annihilation reaction and nonelastic reaction channel σ(E) for antiparticle and neutron reactions by solving momentum-dependent optical model potential; deduced optical model potential well depth, power law dependence of annihilation σ on projectile momentum and atomic mass, and difference between antineutron-nucleus and antiproton-nucleus potentials.

doi: 10.1103/PhysRevC.97.054617
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2016KA31      Phys.Rev. C 94, 015201 (2016)

H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato

Isospin decomposition of γN → N* transitions within a dynamical coupled-channels model

NUCLEAR REACTIONS 1n(γ, π-)p, E=1101-1996 MeV; 1n(γ, π0)n, E=1202-1912 MeV; 1H(γ, π0)p, E=1869-2092 MeV; 1H(γ, π+)n, E=1313-2092 MeV; analyzed σ(θ), photon asymmetry, target polarization and recoil polarization using database of the INS DAC Services at GWU; deduced transition amplitudes for photoexcitation of the neutron-to-nucleon resonances, helicity amplitudes. Dynamical coupled-channels analysis.

doi: 10.1103/PhysRevC.94.015201
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2016KA54      Phys.Rev. C 94, 065205 (2016)

H.Kamano, T.-S.H.Lee

Toward establishing low-lying Λ ans Σ hyperon resonances with the K-bar + d → π + Y + N reaction

doi: 10.1103/PhysRevC.94.065205
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2016LE03      Phys.Rev. C 93, 014616 (2016), Erratum Phys.Rev. C 95, 029901 (2017)

T.-G.Lee, C.-Y.Wong

Nuclear annihilation by antinucleons

NUCLEAR REACTIONS 1,2H, 4He, Be, C, Ne, Al, Ni, Cu, Cd, Sn, Pt, Pb(p-bar, X), 1H, C, Al, Fe, Cu, Ag, Sn, Pb(n-bar, X), E at 20-1100 MeV/c; calculated antiproton-proton, antiproton-nucleus, antineutron-proton and antineutron-nucleus annihilation cross sections as functions of antiproton and antineutron momenta. Pomeranchuk's equality limit and extended Glauber model analysis. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.014616
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2015KA32      Phys.Rev. C 92, 025205 (2015); Erratum Phys.Rev. C 95, 049903 (2017)

H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato

Dynamical coupled-channels model of K-p reactions. II. Extraction of Λ* and Σ* hyperon resonances

doi: 10.1103/PhysRevC.92.025205
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2015WU02      Phys.Rev. C 91, 035203 (2015)

J.-J.Wu, T.Sato, T.-S.H.Lee

Incoherent pion production in neutrino-deuteron interactions

NUCLEAR REACTIONS 2H(γ, X), E=208-343 MeV; calculated differential σ(E, θ), total σ(E). 2H(ν, X), E(outgoing muon)=550, 600, 650 MeV; calculated differential σ(E, θ) as function of pion scattering and other variables. Comparison with experimental data. Prediction of the cross sections of electroweak pion production on the deuteron in the energy region near the Δ(1232) resonance. Multiple scattering formulation.

doi: 10.1103/PhysRevC.91.035203
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2014KA49      Phys.Rev. C 90, 065204 (2014)

H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato

Dynamical coupled-channels model of K-p reactions: Determination of partial-wave amplitudes

doi: 10.1103/PhysRevC.90.065204
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2014LE11      Phys.Rev. C 89, 054601 (2014)

T.-G.Lee, C.-Y.Wong

Extended Glauber model of antiproton-nucleus annihilation for all energies and mass numbers

NUCLEAR REACTIONS 1,2H, 4He, Be, C, Ne, Al, Ni, Cu, Cd, Sn, Pt, Pb(p-bar, X), E at 10-3000 MeV/c; calculated antiproton-nucleus annihilation σ(E) based on extended Glauber model. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.054601
Citations: PlumX Metrics


2014WU09      Phys.Rev. C 90, 055206 (2014)

J.-J.Wu, T.-S.H.Lee, A.W.Thomas, R.D.Young

Finite-volume Hamiltonian method for coupled-channels interactions in lattice QCD

doi: 10.1103/PhysRevC.90.055206
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2013KA41      Phys.Rev. C 88, 035209 (2013)

H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato

Nucleon resonances within a dynamical coupled-channels model of πN and γN reactions

doi: 10.1103/PhysRevC.88.035209
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2013WU02      Phys.Rev. C 88, 015205 (2013)

J.-J.Wu, T.-S.H.Lee

Production of J/Ψ on the nucleon and on deuteron targets

doi: 10.1103/PhysRevC.88.015205
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2012CH43      Phys.Rev. C 86, 054001 (2012)

J.-W.Chen, T.-K.Lee, C.-P.Liu, Y.-S.Liu

Quark-mass dependence of two-nucleon observables

doi: 10.1103/PhysRevC.86.054001
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2012WU02      Phys.Rev. C 85, 044002 (2012)

J.-J.Wu, T.-S.H.Lee, B.S.Zou

Nucleon resonances with hidden charm in coupled-channels models

doi: 10.1103/PhysRevC.85.044002
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2012WU03      Phys.Rev. C 86, 065203 (2012)

J.-J.Wu, T.-S.H.Lee

Photoproduction of bound states with hidden charm

doi: 10.1103/PhysRevC.86.065203
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2010CR03      Phys.Rev. C 82, 045211 (2010)

C.Crawford, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.R.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, D.Hasell, P.Karpius, M.Kohl, H.Kolster, T.Lee, E.Lomon, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.Milner, J.Rapaport, R.Redwine, J.Seely, A.Shinozaki, A.Sindile, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart

Role of mesons in the electromagnetic form factors of the nucleon

doi: 10.1103/PhysRevC.82.045211
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2010KA20      Phys.Rev. C 81, 065207 (2010)

H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato

Extraction of P11 resonances from πN data

doi: 10.1103/PhysRevC.81.065207
Citations: PlumX Metrics


2010NA04      Phys.Rev. C 81, 035502 (2010)

S.X.Nakamura, T.Sato, T.-S.H.Lee, B.Szczerbinska, K.Kubodera

Dynamical model of coherent pion production in neutrino-nucleus scattering

NUCLEAR REACTIONS 12C(π-, X), E=75-275 MeV; calculated total cross section. 12C(π+, π+), E=40, 80 MeV; 12C(π-, π-), E=120, 180, 230, 280 MeV; 12C(γ, π0), E=173 MeV; 12C(γ, π0), E(cm)=200, 290, 350 MeV; calculated σ(θ) of differential cross section. 12C(ν, X), E=0.2-1.5 GeV; calculated σ, pion and muon momentum distributions. Microscopic dynamical model describing neutrino-induced coherent pion production. Comparisons with experimental data.

doi: 10.1103/PhysRevC.81.035502
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2010RI03      Phys.Rev. C 82, 015202 (2010)

F.Riek, R.Rapp, Y.Oh, T.-S.H.Lee

Medium modifications of the ρ meson in nuclear photoproduction

NUCLEAR REACTIONS 12C, 27Al, 56Fe, 88Sr, 120Sn, 152Sm, 197Au, 208Pb, 238U(γ, X), E=1-3.5 GeV; calculated invariant mass excess spectra, total σ of the dileptons, nuclear transparency ratio. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.015202
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2010SU01      Phys.Rev.Lett. 104, 042302 (2010)

N.Suzuki, B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato

Disentangling the Dynamical Origin of P11 Nucleon Resonances

doi: 10.1103/PhysRevLett.104.042302
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2010SU25      Phys.Rev. C 82, 045206 (2010)

N.Suzuki, T.Sato, T.-S.H.Lee

Extraction of electromagnetic transition form factors for nucleon resonances within a dynamical coupled-channels model

doi: 10.1103/PhysRevC.82.045206
Citations: PlumX Metrics


2009JU04      Phys.Rev. C 80, 025207 (2009)

B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato, N.Suzuki

Dynamical coupled-channels analysis of 1H(e, e'π)N reactions

doi: 10.1103/PhysRevC.80.025207
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2009KA08      Phys.Rev. C 79, 025206 (2009)

H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato

Dynamical coupled-channels study of πN → ππN reactions

doi: 10.1103/PhysRevC.79.025206
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2009KA39      Phys.Rev. C 80, 065203 (2009)

H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato

Double and single pion photoproduction within a dynamical coupled-channels model

doi: 10.1103/PhysRevC.80.065203
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2009MO25      Phys.Rev. C 80, 045212 (2009)

V.I.Mokeev, V.D.Burkert, T.-S.H.Lee, L.Elouadrhiri, G.V.Fedotov, B.S.Ishkhanov

Model analysis of the ep → e'pπ+π- electroproduction reaction on the proton

doi: 10.1103/PhysRevC.80.045212
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2009SU02      Phys.Rev. C 79, 025205 (2009)

N.Suzuki, T.Sato, T.-S.H.Lee

Extraction of resonances from meson-nucleon reactions

doi: 10.1103/PhysRevC.79.025205
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2008CA12      Eur.Phys.J. A 35, 253 (2008)

S.Capstick, A.Svarc, L.Tiator, J.Gegelia, M.M.Giannini, E.Santopinto, C.Hanhart, S.Scherer, T.-S.H.Lee, T.Sato, N.Suzuki

The physical meaning of scattering matrix singularities in coupled-channel formalisms BRAG 2007 Workshop summary

doi: 10.1140/epja/i2007-10576-1
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2008CH23      Chin.J.Phys.(Taiwan) 46, 560 (2008)

H.-W.Chen, T.Lee, T.-L.Ku, J.P.Das

Production Ratio of Nuclear Fallout 137Cs/135Cs


2008DU17      Phys.Rev. C 78, 025204 (2008)

J.Durand, B.Julia-Diaz, T.-S.H.Lee, B.Saghai, T.Sato

Coupled-channels study of the π- p → ηn process

doi: 10.1103/PhysRevC.78.025204
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2008JU04      Phys.Rev. C 77, 045205 (2008)

B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato, L.C.Smith

Dynamical coupled-channels effects on pion photoproduction

NUCLEAR REACTIONS p(γ, p)π0, E=1154-1632 MeV; calculated cross sections, angular distributions using dynamical coupled-channel model. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.045205
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2008LE14      Nucl.Phys. A805, 54c (2008)

T.D.Lee

Symmetry and Asymmetry

doi: 10.1016/j.nuclphysa.2008.02.272
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2007CR01      Phys.Rev.Lett. 98, 052301 (2007)

C.B.Crawford, A.Sindile, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, D.Dutta, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, W.Haeberli, D.Hasell, W.Hersman, M.Holtrop, P.Karpius, M.Kohl, H.Kolster, T.Lee, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.G.Milner, R.P.Redwine, J.Seely, A.Shinozaki, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, J.F.J.van den Brand, J.van der Laan, F.Wang, T.Wise, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart

Measurement of the Proton's Electric to Magnetic Form Factor Ratio from 1H(pol)(e(pol), e'p)

NUCLEAR REACTIONS 1H(polarized e, e'p), E=high; measured asymmetries. 1H deduced electric to magnetic form factor ratios. Polarized target.

doi: 10.1103/PhysRevLett.98.052301
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2007JU01      Phys.Rev. C 75, 015205 (2007)

B.Julia-Diaz, T.-S.H.Lee, T.Sato, L.C.Smith

Extraction and interpretation of γN → Δ form factors within a dynamical model

NUCLEAR REACTIONS 1H(e, e'π0), E=high; analyzed σ(θ), related data; deduced form factors.

doi: 10.1103/PhysRevC.75.015205
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2007JU07      Phys.Rev. C 76, 065201 (2007)

B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato

Dynamical coupled-channels model of πN scattering in the W ≤ 2 GeV nucleon resonance region

NUCLEAR REACTIONS p(π-, π-), (π-, π0), E<2 GeV; analyzed pion-nucleon scattering using dynamical coupled-channel model.

doi: 10.1103/PhysRevC.76.065201
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2007LE17      J.Phys.(London) G34, S83 (2007)

T.-S.H.Lee, L.C.Smith

Study of nucleon resonances with electromagnetic interactions

doi: 10.1088/0954-3899/34/7/S05
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2007MA11      Phys.Rep. 439, 193 (2007)

A.Matsuyama, T.Sato, T.-S.H.Lee

Dynamical coupled-channel model of meson production reactions in the nucleon resonance region

doi: 10.1016/j.physrep.2006.12.003
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2007SA19      Eur.Phys.J. A 31, 512 (2007)

B.Saghai, J.-C.David, B.Julia-Diaz, T.-S.H.Lee

Search for missing baryon resonances via associated strangeness photoproduction

NUCLEAR REACTIONS 1H(γ, K+X), E ≈ 1.1, 1.3 GeV; analyzed hyperon production σ(θ), polarization observables.

doi: 10.1140/epja/i2006-10226-2
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2007SI31      Eur.Phys.J. A 34, 49 (2007)

A.Sibirtsev, J.Haidenbauer, S.Krewald, T.-S.H.Lee, U.-G.Meissner, A.W.Thomas

Regge approach to charged pion photoproduction at invariant energies above 2 GeV

doi: 10..1140/epja/i2007-10482-6
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2007SZ03      Phys.Lett. B 649, 132 (2007)

B.Szczerbinska, T.Sato, K.Kubodera, T.-S.H.Lee

Neutrino-nucleus reactions in the delta resonance region

NUCLEAR REACTIONS 12C(ν, X), (e, X), E=1, 1.1 GeV; calculated e-, μ energy spectra, σ(θ, Q2). Sato-Lee model.

doi: 10.1016/j.physletb.2007.03.046
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2006JU02      Phys.Rev. C 73, 055204 (2006)

B.Julia-Diaz, B.Saghai, T.-S.H.Lee, F.Tabakin

Dynamical coupled-channels approach to hadronic and electromagnetic kaon-hyperon production on the proton

NUCLEAR REACTIONS 1H(π-, K0X), (γ, K+X), E(cm) ≈ 1.6-2.3 GeV; calculated hyperon production associated σ(θ), recoil polarization asymmetry, excitation functions. Dynamical coupled-channels approach, comparison with data.

doi: 10.1103/PhysRevC.73.055204
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2006OH01      Phys.Rep. 423, 49 (2006)

Y.Oh, K.Nakayama, T.-S.H.Lee

Pentaquark Θ+ (1540) production in γN → K(K-bar)N reactions

NUCLEAR REACTIONS 1n, 1H(γ, K+K-), E=1-4.5 GeV; calculated σ, invariant mass spectra, pentaquark production features.

doi: 10.1016/j.physrep.2005.10.002
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2006SA36      Nucl.Phys. B(Proc.Supp.) S159, 141 (2006)

T.Sato, B.Szczerbinska, K.Kubodera, T.-S.H.Lee

Dynamical model of electroweak pion production in the resonance region

NUCLEAR REACTIONS 1H(e, e'π+), (e, e'π0), (ν, eπ+), (ν, μ-π+), E ≈ 1-1.4 GeV; calculated σ(Q2).

doi: 10.1016/j.nuclphysbps.2006.08.030
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2005JU08      Nucl.Phys. A755, 463c (2005)

B.Julia-Diaz, B.Saghai, F.Tabakin, W.-T.Chiang, T.-S.H.Lee, Z.Li

Dynamical coupled-channel study of K+Λ photoproduction

NUCLEAR REACTIONS 1H(γ, K+X), E(cm) ≈ 1.6-2.3 GeV; calculated hyperon production σ(θ), excitation functions. Constituent quark model, coupled-channels approach, comparison with data.

doi: 10.1016/j.nuclphysa.2005.03.056
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2005KU46      Nucl.Instrum.Methods Phys.Res. A547, 73 (2005)

C.Kunz, S.Thiess, B.Cowie, T.-L.Lee, J.Zegenhagen

Outer sub-shell photoabsorption cross-sections determined by X-ray photoelectron spectroscopy up to 14.5 keV

NUCLEAR REACTIONS C, Au(γ, X), E<14.5 keV; measured reaction products; deduced σ. Comparison with available data.

doi: 10.1016/j.nima.2005.05.014
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2005LE05      Nucl.Phys. A750, 1 (2005)

T.D.Lee

The strongly interacting quark-gluon plasma and future physics

doi: 10.1016/j.nuclphysa.2004.11.003
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2005MA63      Phys.Rev. C 72, 025204 (2005)

K.Matsui, T.Sato, T.-S.H.Lee

Quark-hadron duality and parity violating asymmetry of electroweak reactions in the Δ region

NUCLEAR REACTIONS 1H(e, e'), (ν, e), (ν, ν'), E=high; calculated structure functions. 1H(e, e'π+), (e, e'π0), E=high; calculated polarization observables. 1H(polarized e, e'), E ≈ 0.5-3 GeV; calculated parity-violating asymmetry. Dynamical model, neutral current contributions. Comparisons with data.

doi: 10.1103/PhysRevC.72.025204
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2004BU26      Int.J.Mod.Phys. E13, 1035 (2004)

V.D.Burkert, T.S.H.Lee

Electromagnetic meson production in the nucleon resonance region

doi: 10.1142/S0218301304002545
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2004CH32      Phys.Rev. C 69, 065208 (2004)

W.-T.Chiang, B.Saghai, F.Tabakin, T.-S.H.Lee

Dynamical coupled-channel model of kaon-hyperon interactions

NUCLEAR REACTIONS 1H(π-, K0X), E=high; calculated hyperon production σ(θ), σ, polarization asymmetries. Dynamical coupled-channels model.

doi: 10.1103/PhysRevC.69.065208
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2004HW03      Nucl.Phys. A737, 294 (2004)

W.-H.P.Hwang, T.-S.H.Lee, B-Q.Ma

A Replay of Few-Body Reactions in Particle Cosmology

doi: 10.1016/j.nuclphysa.2004.03.091
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2004OH02      Phys.Rev. C 69, 025201 (2004)

Y.Oh, T.-S.H.Lee

ρ meson photoproduction at low energies

NUCLEAR REACTIONS 1H(γ, X), E=2.8, 3.28, 3.55, 3.82 GeV; calculated ρ-meson production σ(E, θ), polarization asymmetries; deduced reaction mechanism features.

doi: 10.1103/PhysRevC.69.025201
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2003JU05      Mod.Phys.Lett. A 18, 200 (2003)

B.Julia-Diaz, T.-S.H.Lee

Quark-exchange mechanism of γd → np reaction at 2-6 GeV

NUCLEAR REACTIONS 2H(γ, n), E=2-6 GeV; calculated σ(θ), role of quark-exchange mechanism.

doi: 10.1142/S0217732303010247
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2003OH08      Nucl.Phys. A721, 743c (2003)

Y.Oh, T.-S.H.Lee

π and ρ loop corrections to ω photoproduction in the resonance region

NUCLEAR REACTIONS 1H(γ, X), E=1.125-1.68 GeV; calculated ω meson production σ(θ), one-loop corrections.

doi: 10.1016/S0375-9474(03)01171-0
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2003SA18      Phys.Rev. C 67, 065201 (2003)

T.Sato, D.Uno, T.-S.H.Lee

Dynamical model of weak pion production reactions

NUCLEAR REACTIONS 1n, 1H(ν, μ-π+), E=0.4-2 GeV; 1n(ν, μ-π0), E=0.4-2 GeV; calculated total σ, σ(Q2). Dynamical model, comparisons with data.

doi: 10.1103/PhysRevC.67.065201
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2003TI08      Phys.Rev. C 67, 065205 (2003)

A.I.Titov, T.-S.H.Lee

Spin effects and baryon resonance dynamics in φ-meson photoproduction at few GeV

NUCLEAR REACTIONS 1H(γ, X), (polarized γ, X), E ≈ 2-4 GeV; calculated ω- and φ-meson production σ(E, θ), polarization observables; deduced resonance contributions.

doi: 10.1103/PhysRevC.67.065205
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2002DU12      Phys.Rev. C65, 044619 (2002)

D.Dutta, H.Gao, T.-S.H.Lee

Nucleon Resonances with Double Polarization Observables of Pion Photoproduction

NUCLEAR REACTIONS 1H(γ, π+), (γ, π0), E=1.10, 1.40 GeV; 1n(γ, π-), E=1.10, 1.45 GeV; calculated σ(θ), polarization observables; deduced role of nucleon resonances.

doi: 10.1103/PhysRevC.65.044619
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2002LE39      Ann.Rev.Nucl.Part.Sci. 52, 23 (2002)

T.-S.H.Lee, R.P.Redwine

Pion-Nucleus Interactions

doi: 10.1146/annurev.nucl.52.050102.090713
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2002NA11      Phys.Rev. C65, 045210 (2002)

K.Nakayama, J.Speth, T.-S.H.Lee

η Meson Production in NN Collisions

NUCLEAR REACTIONS 1H(p, X), (n, X), E ≈ threshold; calculated η meson production σ, σ(θ), Ay(θ). Relativistic meson exchange model, comparison with data.

doi: 10.1103/PhysRevC.65.045210
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2002OH04      Phys.Rev. C66, 045201 (2002)

Y.Oh, T.-S.H.Lee

One-loop corrections to ω photoproduction near threshold

NUCLEAR REACTIONS 1H(γ, X), (π-, X), E=high; calculated ω production σ(θ), one-loop corrections. Coupled-channels approach, comparison with data.

doi: 10.1103/PhysRevC.66.045201
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2002TI08      Phys.Rev. C66, 015204 (2002)

A.I.Titov, T.-S.H.Lee

Effective Lagrangian Approach to the ω Photoproduction Near Threshold

NUCLEAR REACTIONS 1H(γ, X), E ≈ threshold; calculated ω production σ(θ), asymmetries. Effective Lagrangian approach.

doi: 10.1103/PhysRevC.66.015204
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2002TI09      Phys.Rev. C66, 022202 (2002)

A.I.Titov, M.Fujiwara, T.S.H.Lee

Coherent φ and ω meson photoproduction from deuteron and nondiffractive channels

NUCLEAR REACTIONS 2H(γ, X), E=1.92, 2.2 GeV; calculated φ and ω meson production σ(E, θ), nondiffractive channel contributions.

doi: 10.1103/PhysRevC.66.022202
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2001CH65      Phys.Lett. 517B, 101 (2001)

W.-T.Chiang, F.Tabakin, T.-S.H.Lee, B.Saghai

Coupled-Channel Study of γp → K+Λ

NUCLEAR REACTIONS 1H(γ, K+), E(cm)=1.6-2.5 GeV; analyzed σ; deduced parameters. Coupled-channels approach.

doi: 10.1016/S0370-2693(01)00945-5
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2001GA07      Phys.Rev. C63, 022201 (2001)

H.Gao, T.-S.H.Lee, V.Marinov

φ-N Bound State

NUCLEAR REACTIONS 12C(γ, X), E=1-2 GeV; calculated σ for formation of φ-Nucleus bound state. Possibilities for experimental detection discussed.

doi: 10.1103/PhysRevC.63.022201
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2001HA44      Phys.Rev. C64, 024306 (2001)

M.A.Hasan, J.P.Vary, T.-S.H.Lee

Medium-Mass Nuclei with Δ Excitations under Compression

NUCLEAR STRUCTURE 90Zr, 100,132Sn; calculated constrained spherical Hartree-Fock energy vs radius, sensitivity to size of nucleon and Δ isobar model spaces.

doi: 10.1103/PhysRevC.64.024306
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2001HA63      Phys.Rev. C64, 064607 (2001)

K.Hafidi, T.-S.H.Lee

Dynamical Study of the 2H(e, e'π+) Reaction

NUCLEAR REACTIONS 2H(e, e'π+), E=645, 844 MeV; calculated σ, missing mass; deduced role of interference effects. Dynamical model, comparisons with data.

doi: 10.1103/PhysRevC.64.064607
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2001HU15      Phys.Rev. C64, 034309 (2001)

C.-T.Hung, S.N.Yang, T.-S.H.Lee

Meson-Exchange πN Models in Three-Dimensional Bethe-Salpeter Formulation

NUCLEAR REACTIONS 1n, 1H(π, X), E < 400 MeV; calculated phase shifts, matrix elements. Three-dimensional reduction of Bethe-Salpeter formulation.

doi: 10.1103/PhysRevC.64.034309
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2001LE01      Phys.Rev. C63, 014006 (2001)

T.-S.H.Lee, R.B.Wiringa

Quantum Monte Carlo Calculations of Pion Scattering from Li

NUCLEAR STRUCTURE 6,7Li; calculated transitions B(E2), transition densities. Quantum Monte-Carlo approach.

NUCLEAR REACTIONS 6Li(π-, π-), (π-, π-'), E=100-240 MeV; 7Li(π+, π+'), (π-, π-'), E=164 MeV; calculated σ(θ). Quantum Monte-Carlo approach, comparisons with data.

doi: 10.1103/PhysRevC.63.014006
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2001LE14      Nucl.Phys. A684, 327c (2001)

T.-S.H.Lee, T.Sato

Dynamical Study of Δ Excitation with N(e, e'π) Reaction

NUCLEAR REACTIONS 1H(e, e'π0), E=high; calculated σ(θ), form factors for Δ resonance production.

doi: 10.1016/S0375-9474(01)00431-6
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2001OH01      Phys.Rev. C63, 025201 (2001)

Y.Oh, A.I.Titov, T.-S.H.Lee

Nucleon Resonances in ω Photoproduction

NUCLEAR REACTIONS 1H(γ, X), E=1.2-4.7 GeV; calculated ω meson production associated σ(E, θ); deduced resonance contributions.

doi: 10.1103/PhysRevC.63.025201
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2001SA17      Phys.Rev. C63, 055201 (2001)

T.Sato, T.-S.H.Lee

Dynamical Study of the Δ Excitation in N(e, e'π) Reaction

NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), E=200-450 MeV; 1H(e, e'π0), E=high; calculated σ(θ); deduced Δ resonance excitation features. Dynamical model, comparisons with data.

doi: 10.1103/PhysRevC.63.055201
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2000HA02      Phys.Rev. C61, 014301 (2000)

M.A.Hasan, J.P.Vary, T.-S.H.Lee

Effect of Neutron Excess on Δ Excitations in Exotic Nuclei

NUCLEAR STRUCTURE 28O, 60,70Ca; calculated Δ resonance states features; deduced role of neutron excess. Constrained spherical Hartree-Fock approach.

doi: 10.1103/PhysRevC.61.014301
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2000LE09      Phys.Lett. 475B, 207 (2000)

T.Lee, Y.Oh

Higher Dimension Operators and Chiral Symmetry Breaking in Nambu-Jona-Lasinio Model

doi: 10.1016/S0370-2693(00)00072-1
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2000OS04      Nucl.Phys. A670, 111c (2000)

E.Oset, J.A.Oller, J.R.Pelaez, A.Ramos, H.C.Chiang, F.Guerrero, S.Hirenzaki, T.S.H.Lee, E.Marco, J.C.Nacher, Y.Okumura, A.Parreno, H.Toki, M.Vicente-Vacas

Recent Progress on the Chiral Unitary Approach to Meson Meson and Meson Baryon Interactions

NUCLEAR REACTIONS 1H(γ, K+X), E=1.7 GeV; calculated pion, hyperon production σ. Unitary approach.

doi: 10.1016/S0375-9474(00)00080-4
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2000TZ01      Phys.Rev. C61, 031305 (2000)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee, V.G.Stoks

Two-Frequency Shell Model for Hypernuclei and Meson-Exchange Hyperon-Nucleon Potentials

NUCLEAR STRUCTURE 16O; calculated hypernucleus levels, J, π. Two-frequency shell model approach.

doi: 10.1103/PhysRevC.61.031305
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2000TZ02      J.Phys.(London) G26, 1765 (2000)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee

A Local Density Approximation Treatment for the Pauli Exclusion Operator in Hypernuclei

NUCLEAR STRUCTURE 16O; calculated hypernuclei single particle energies, levels, J, π. Shell model calculations, comparison with data.

doi: 10.1088/0954-3899/26/12/301
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2000VR01      Phys.Rep. 328, 181 (2000)

T.P.Vrana, S.A.Dytman, T.-S.H.Lee

Baryon Resonance Extraction from πN Data using a Unitary Multichannel Model

doi: 10.1016/S0370-1573(99)00108-8
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2000YO06      Phys.Rev. C61, 065203 (2000)

T.Yoshimoto, T.Sato, M.Arima, T.-S.H.Lee

Dynamical Test of Constituent Quark Models with πN Reactions

NUCLEAR REACTIONS 1H(π-, nX), E=1400-1900 MeV; calculated η production σ. Constituent quark model, dynamical approach, comparison with data.

doi: 10.1103/PhysRevC.61.065203
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1999CA19      Phys.Rev. C59, R3002 (1999)

S.Capstick, T.-S.H.Lee, W.Roberts, A.Svarc

Evidence for the Fourth P11 Resonance Predicted by the Constituent Quark Model

doi: 10.1103/PhysRevC.59.R3002
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1999LE43      Phys.Lett. 462B, 1 (1999)

T.Lee

Normalization Constants of Large Order Behavior

doi: 10.1016/S0370-2693(99)00932-6
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1999ST21      Phys.Rev. C60, 024006 (1999)

V.G.J.Stoks, T.-S.H.Lee

Strange Hadron Matter and SU(3) Symmetry

doi: 10.1103/PhysRevC.60.024006
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1999TI06      Phys.Rev. C59, R2993 (1999)

A.I.Titov, T.-S.H.Lee, H.Toki

Isotopic Effect in φ Photoproduction at a Few GeV

NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm) ≈ 2-5 GeV; calculated φ photoproduction σ, decay asymmetry; deduced isotopic effect.

doi: 10.1103/PhysRevC.59.R2993
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1999TI08      Phys.Rev. C60, 035205 (1999)

A.I.Titov, T.-S.H.Lee, H.Toki, O.Streltsova

Structure of the φ Photoproduction Amplitude at a Few GeV

NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm)=2-5 GeV; calculated φ meson production σ(θ), spin-density matrix elements, polarization observables. Pomeron-exchange and meson-exchange mechanisms.

doi: 10.1103/PhysRevC.60.035205
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1999TZ01      Phys.Rev. C60, 044305 (1999)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee

Particle-Hole Folded-Diagram Calculation of the Hypernucleus Λ16O using Meson-Exchange Interactions

NUCLEAR STRUCTURE 16O; calculated hypernucleus levels, J, π. Folded-diagram G-matrix calculations.

doi: 10.1103/PhysRevC.60.044305
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1998BA39      Phys.Scr. 58, 15 (1998)

M.Batinic, I.Dadic, I.Slaus, A.Svarc, B.M.K.Nefkens, T.-S.H.Lee

The New Determination of the ηN S-Wave Scattering Length from a Three-Channel, Multi-Resonance Amplitude Analysis


1998BE02      Phys.Rev. C57, 424 (1998)

S.R.Beane, V.Bernard, T.-S.H.Lee, U.-G.Meissner

Isoscalar S-Wave π-N Scattering Length a+ from π-Deuteron Scattering

NUCLEAR REACTIONS 2H(π, X), E not given; calculated scattering length; deduced πN scattering length related features.

doi: 10.1103/PhysRevC.57.424
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1998KA17      Nucl.Phys. A631, 519c (1998)

H.Kamada, M.P.Locher, T.-S.H.Lee, J.Golak, V.E.Markushin, W.Glockle, H.Witala

Pion Absorption Reaction on 2H and 3He in the Δ-Isobar Region

NUCLEAR REACTIONS 2H(π+, 2p), 3He(π+, 3p), E < 350 MeV; analyzed total σ, σ(θ). Fadeev equations.

doi: 10.1016/S0375-9474(98)00059-1
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1998LE09      Nucl.Phys. A629, 180c (1998)

T.-S.H.Lee

Chiral Constituent Quark Model Predictions of Electroproduction of the Δ on the Nucleon and 3He

NUCLEAR REACTIONS 3He(e, e'X), E=high; calculated Δ(++) production associated σ(θ). Chiral constituent quark model.

doi: 10.1016/S0375-9474(97)00684-2
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1998LE23      Phys.Rev. C58, 1551 (1998)

T.-S.H.Lee, Z.-Y.Ma, B.Saghai, H.Toki

Photoproduction of a Λ on 12C

NUCLEAR REACTIONS 12C(γ, K+), E=0.7-1.2 GeV; calculated hypernucleus production σ(θ); deduced dependence on pγ amplitudes, possible medium effects. Comparison with data.

doi: 10.1103/PhysRevC.58.1551
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1998LE26      Nucl.Phys. A639, 247c (1998)

T.-S.H.Lee, V.Stoks, B.Saghai, C.Fayard

Study of Hyperon-Nucleon Interactions with d(e, e'K) Reactions

NUCLEAR REACTIONS 2H(e, e'K+), E not given; calculated hyperon production σ(Q2, θ). Hyperon-nucleon interactions compared.

doi: 10.1016/S0375-9474(98)00280-2
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1998LE29      Acta Phys.Hung.N.S. 7, 263 (1998)

T.-S.H.Lee, J.A.Lopez, J.Morales, G.Thondikulam

Separable Potentials for the Hadronic Phase


1998LE38      Nucl.Phys. A643, 402 (1998)

T.-S.H.Lee, J.A.Oller, E.Oset, A.Ramos

Non-Perturbative Chiral Approach to K-p → γY Reactions

NUCLEAR REACTIONS 1H(K-, γX), E ≈ threshold; calculated branching ratios for Λ, Σ0 production. Non-perturbative chiral approach.

doi: 10.1016/S0375-9474(98)00581-8
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1998TZ01      Nucl.Phys. A639, 165c (1998)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee

Folded-Diagram Effective Interactions for Hypernuclei

NUCLEAR STRUCTURE 16O; calculated hypernucleus levels, J, π. Folded diagram G-matrix framework.

doi: 10.1016/S0375-9474(98)00266-8
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1997BA65      Phys.Scr. 56, 321 (1997)

M.Batinic, A.Svarc, T.-S.H.Lee

Near Threshold η Production in Proton-Proton Collisions

NUCLEAR REACTIONS 1H(p, X), E=1260-1360 MeV; analyzed σ; deduced η production mechanism features.


1997BE19      Nucl.Phys. A618, 381 (1997)

S.R.Beane, V.Bernard, T.-S.H.Lee, Ulf.-G.Meissner, U.van Kolck

Neutral Pion Photoproduction on Deuterium in Baryon Chiral Perturbation Theory to Order q4

NUCLEAR REACTIONS 2H(γ, X), E ≈ threshold; calculated π0 production σ related features; deduced sensitivity to γn → π0n amplitude. Baryon chiral perturbation theory to order q4.

doi: 10.1016/S0375-9474(97)00133-4
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1997FR01      Phys.Rev. C55, 909 (1997)

L.Frankfurt, T.-S.H.Lee, G.A.Miller, M.Strikman

Chiral Transparency

NUCLEAR REACTIONS 3He(e, e'X), E not given; calculated Δ++n-quasielastic production associated chiral transparency ratio vs Q2.

doi: 10.1103/PhysRevC.55.909
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1997HA56      Phys.Rev. C56, 3063 (1997)

M.A.Hasan, T.-S.H.Lee, J.P.Vary

Mean-Field Calculation of Compressed Finite Nuclei with Δ Excitations

NUCLEAR STRUCTURE 90Zr; calculated proton, neutron, Δ radial density distributions, compressibility; deduced Δ component vs compression. Constrained Hartree-Fock.

doi: 10.1103/PhysRevC.56.3063
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1997KA23      Phys.Rev. C55, 2563 (1997)

H.Kamada, M.P.Locher, T.-S.H.Lee, J.Golak, V.E.Markushin, W.Glockle, H.Witala

Pion Absorption Cross Section for 2H and 3He in the Δ-Isobar Region: A phenomenological connection

NUCLEAR REACTIONS 2H(π, p), 3He(π+, 3p), E ≤ 300 MeV; calculated σ(E). Exact final state interaction inclusion.

doi: 10.1103/PhysRevC.55.2563
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