NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Y.Lu Found 48 matches. 2023LU10 Phys.Rev. C 108, 024612 (2023) Systematic single-folding optical potential for 6Li and 7Li based on KD02 potentials NUCLEAR REACTIONS 24,25,26Mg, 27Al, 28Si, 39K, 40Ca, 58Ni, 89Y, 90,91,92,94,96Zr, 112,116,120,124Sn, 208Pb, 209Bi(6Li, 6Li), E=31-240 MeV;24,26Mg, 28Si, 40,44,48Ca, 54,56Fe, 58,60Ni, 89Y, 90Zr, 116,118Sn, 142Nd, 144Sm, 208Pb(7Li, 7Li), E=33-350 MeV; analyzed experimental data of nucleus-nucleus elastic scattering and σ energy dependence; deduced optical potential parameters; calculated σ(θ), σ(E). 116Sn, 208Pb(6Li, X), E=5-300 MeV; 28Si, 64Zn, 116Sn, 208Pb(7Li, X), E=5-360 MeV; calculated σ(E). Energy-dependent systematic optical potential on the KD02 optical potential within the framework of the single-folding model. Comparison to experimental data and calculations performed with Cook's systematic optical potential.
doi: 10.1103/PhysRevC.108.024612
2023MA17 Phys.Rev. C 107, 034316 (2023) β-decay half-lives of the r-process waiting-point isotones of N=8 and 82 nuclei RADIOACTIVITY 131,130In, 130,129Cd, 129,128Ag, 128,127Pd, 127,126Rh, 126,125Ru, 125,124Tc, 124,123Mo, 123,122Nb, 122,121Zr, 121,120Y, 120,119Sr(β-); calculated T1/2, Gamow-Teller decay rates from the ground state. 125mTc, 123mNb, 129mCd, 127mPd, 125mRu, 123mMo, 121mZr, 119mSr(β-); calculated isomers states T1/2. Nucleon-pair approximation (NPA) method assuming S pair condensation in the ground state of parent nuclei. Comparison to available experimental data and other theoretical calculation (shell-model, QRPA, RQRPA+RHB). NUCLEAR STRUCTURE 130Sn, 129,130Cd, 130,131In, 129Ag, 127Rh, 125Tc, 123Nb, 121Y; calculated levels J, π, occupation probability of the proton orbits. Shell-model calculations. NUCLEAR MOMENTS 131,129In, 131Sn, 129,127Ag, 129Cd, 127,125Rh, 127Pd, 125Ru, 125,123Tc, 123,121Nb, 123Mo, 121Zr, 121,119Y, 119Sr; calculated electrical quadrupole moments, magnetic moments. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.034316
2023PA19 Chin.Phys.C 47, 064102 (2023) Y.-F.Pan, Y.-Y.Cheng, Y.Lu, H.Jiang, X.-R.Zhou, Y.-M.Zhao Robustness of pair structures for nuclear yrast states NUCLEAR STRUCTURE 28Si, 50Cr, 132Xe; calculated energy levels, J, π, quadrupole moments, yrast states using the nucleon-pair approximation (NPA) and shell-model effective interactions. Comparison with available data.
doi: 10.1088/1674-1137/acc1cc
2022LU03 Phys.Rev. C 105, 034317 (2022) Y.Lu, Y.Lei, C.W.Johnson, J.Shen Nuclear states projected from a pair condensate NUCLEAR STRUCTURE 22,24,26,28,30,32,34Si, 46,48Ca, 48,50Ti, 50,52Cr, 104Sn, 106Te, 108Xe; calculated levels J, π, B(E2). 52Fe; calculated backbending of yrast state band. 124,126Xe, 126,128Ba; calculated levels J, π. Projection after variation of pair condensates (PVPC) method. Comparison to experimental data and projected Hartree-Fock (PHF) and shell-model calculations.
doi: 10.1103/PhysRevC.105.034317
2022YU04 Phys.Rev. C 106, 044309 (2022) Y.X.Yu, Y.Lu, G.J.Fu, C.W.Johnson, Z.Z.Ren Nucleon-pair truncation of the shell model for medium-heavy nuclei NUCLEAR STRUCTURE 44,46,48Ti, 48,50Cr, 52Fe, 60,62,64Zn, 66,68Ge, 68Se, 108,110Xe, 112,114Ba, 116,118,120Ce; calculated levels, J, π, yrast states, B(E2). Particle-number conserved Bardeen-Cooper-Schrieffer (NBCS) approximation developed for implementing efficient truncation scheme in the frame of shell-model. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.044309
2021LU06 Eur.Phys.J. A 57, 115 (2021) Y.Lu, D.Binosi, M.Ding, C.D.Roberts, H.-Y.Xing, C.Xu Distribution amplitudes of light diquarks
doi: 10.1140/epja/s10050-021-00427-6
2021RA28 Eur.Phys.J. A 57, 266 (2021) K.Raya, L.X.Gutierrez-Guerrero, A.Bashir, L.Chang, Z.-F.Cui, Y.Lu, C.D.Roberts, J.Segovia Dynamical diquarks in the γ*p → N(1535) 1 over 2- transition
doi: 10.1140/epja/s10050-021-00574-w
2020JO07 J.Phys.(London) G47, 105107 (2020) Exact sum rules with approximate ground states NUCLEAR STRUCTURE 52,53,54,56Fe; analyzed available data; calculated M-scheme dimensions; deduced sum rules for E2 transitions in the sd shell nuclei.
doi: 10.1088/1361-6471/abacda
2019BA08 Phys.Rev. C 99, 024619 (2019) H.Bai, H.Jiang, Y.Lu, Z.Cui, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, Xi.Ruan, H.Huang, J.Ren, Q.Fan 56, 54Fe (n, α) 53, 51Cr cross sections in the MeV region NUCLEAR REACTIONS 54,56Fe(n, α), E=5.5, 7.7, 8.5, 9.5, 10.5 MeV; measured α-particles, E(n), I(n), and σ(E) using twin-gridded ionization chamber for charged particle detection and 238U fission chamber for neutron fluence at the 4.5-MV Van de Graaff accelerator of Peking University (PKU). Comparison with theoretical calculations using TALYS-1.8 code, and evaluated data in ENDF-B/VII.1, JEFF-3.3, JENDL-4.0, and several other libraries.
doi: 10.1103/PhysRevC.99.024619
2019BA33 Appl.Radiat.Isot. 152, 180 (2019) H.Bai, H.Jiang, Y.Lu, Z.Cui, J.Chen, G.Zhang Determination of the number of 238U target nuclei and simulation of the neutron induced fission fragment energy spectrum RADIOACTIVITY 238U(α); measured decay products, Eα, Iα; deduced energy spectrum of neutron induced fission fragments. Comparison with Monte Carlo calculations.
doi: 10.1016/j.apradiso.2019.06.026
2018GL03 Phys.Rev. C 98, 034605 (2018) Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, H.Bai, H.Jiang, Y.Lu, Z.Cui, J.Chen, G.Zhang Measurement of the cross sections of the 25Mg (n, α) 22Ne reaction in the 4-6 MeV region NUCLEAR REACTIONS 25Mg(n, α), E=4.0-6.0 MeV; measured Eα, Iα, σ(E) using enriched target and a twin-gridded ionization chamber for charged particle detection at the 4.5 MV Van de Graaff accelerator of Peking University Comparison with previous experimental values, evaluated data libraries, and theoretical predictions.
doi: 10.1103/PhysRevC.98.034605
2018LU05 Phys.Rev. C 97, 034330 (2018) Transition sum rules in the shell model NUCLEAR STRUCTURE 34Cl, 10B, 21,27Ne; analyzed energy-weighted sum rules (EWSR) and transition strength function centroids as a function of initial energy for isoscalar E2 in 34Cl, for E1 in 10B, M1 in 21Ne and GT transitions for 27Ne; calculated ground-state E1 energy-weighted sum rule (EWSR) for Z=N nuclides. Z=11, 13, 15, 17, N=9-19; calculated centroids of E2 transitions from the ground state as a function of neutron number. Z=10, 12, 14, 16, N=10, 12, 14, 16, 18; calculated energies of the first 2+ states. Shell model occupation-space framework using the code PANDASCOMMUTE for non-energy weighted and energy-weighted sums rules of transition strength functions.
doi: 10.1103/PhysRevC.97.034330
2018WA34 Yuan.Wul.Ping. 35, 445 (2018); Nucl.Phys.Rev. 35, 445 (2018) Y.Wang, J.Su, Z.Han, B.Tang, B.Cui, T.Ge, Y.Lu, Z.Chen, B.Guo, X.Li, Y.Li, Z.Li, G.Lian, T.Ma, Y.Ma, Y.Shen, Y.Su, C.Wang, H.Wu, S.Yan, S.Zeng, Y.Zheng, C.Zhou, Y.Dang, G.Fu, Y.He, F.Liu, D.Wu, T.Zhang, W.Liu, for the BRIF collaboration Study of the Exotic Decay Mode of 20Na with an Intense ISOL Beam RADIOACTIVITY 20Na(β+α) [from 24Mg(p, nα), E<100 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced γ-ray energies and intensities, exotic β-γ-α decay mode.
doi: 10.11804/NuclPhysRev.35.04.445
2017GU09 Chin.Phys.C 41, 054002 (2017) X-C.Guan, Y.-K.Lu, H.-J.He, J.-T.Zhao, Q.Wang, K.-H.Fang, X.Meng, T.-S.Wang, J.Kasagi Deuterium depth distribution study in Yb NUCLEAR REACTIONS 2H(d, p), E=20 keV; measured reaction products, Ep, Ip; deduced proton yields, deuterium depth distribution for 20 keV deuterons implanted into Yb foil.
doi: 10.1088/1674-1137/41/5/054002
2017LU05 Phys.Rev. C 96, 015208 (2017) Y.Lu, C.Chen, C.D.Roberts, J.Segovia, S.-S.Xu, H.-S.Zong Parity partners in the baryon resonance spectrum
doi: 10.1103/PhysRevC.96.015208
2017WA42 Phys.Rev. C 96, 044620 (2017) Z.Wang, H.Bai, L.Zhang, H.Jiang, Y.Lu, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu Cross section measurement for the 10B (n, t2α) three-body reaction at 4.0, 4.5, and 5.0 MeV. I. Prediction of the experimental spectrum NUCLEAR REACTIONS 10B(n, t2α), E=4.0, 4.5, 5.0 MeV; calculated complete final-state phase space for the 7Li**, 8Be, and breakup channels, one-dimensional and two-dimensional experimental spectra using LUNF code, and as described in the experimental details of a companion article 2017Wa23.
doi: 10.1103/PhysRevC.96.044620
2017WA43 Phys.Rev. C 96, 044621 (2017) Z.Wang, H.Bai, L.Zhang, H.Jiang, Y.Lu, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu Cross section measurement for the 10B (n, t2α) three-body reaction at 4.0, 4.5, and 5.0 MeV. II. Experimental setup and results NUCLEAR REACTIONS 10B(n, t2α), E=4.0, 4.5, 5.0 MeV; 10B(n, α)7Li, E=thermal; measured particle spectra, grid-anode two-dimensional spectra using a twin gridded ionization chamber (GIC) and double-coincidence technique at the 4.5 MV Van de Graaff accelerator of Peking University; deduced σ(E). Comparison with previous measurements and evaluated libraries ENDF/B-VII.1, JENDL-4.0, and CN-RAC2016.
doi: 10.1103/PhysRevC.96.044621
2017XI15 Phys.Rev. C 96, 054303 (2017) S.Y.Xia, H.Tao, Y.Lu, Z.P.Li, T.Niksic, D.Vretenar Spectroscopy of reflection-asymmetric nuclei with relativistic energy density functionals NUCLEAR STRUCTURE 138,140,142,144,146,148,150,152,154Xe, 140,142,144,146,148,150,152,154,156Ba, 142,144,146,148,150,152,154,156,158Ce, 144,146,148,150,152,154,156,158,160Nd, 146,148,150,152,154,156,158,160,162Sm, 148,150,152,154,156,158,160,162,164Gd, 216,218,220,222,224,226,228,230,232,234,236,238Rn, 218,220,222,224,226,228,230,232,234,236,238,240Ra, 220,222,224,226,228,230,232,234,236,238,240,242Th, 222,224,226,228,230,232,234,236,238,240,242,244U, 224,226,228,230,232,234,236,238,240,242,244,246Pu, 226,228,230,232,234,236,238,240,242,244,246,248Cm, 228,230,232,234,236,238,240,242,244,246,248,250Cf, 230,232,234,236,238,240,242,244,246,248,250,252Fm; calculated levels, J, π, B(E1), B(E2), B(E3), electric dipole moments, deformation energy surface in (β2, β3) plane, other related features for 2+, 1-, 3- states of reflection-asymmetric nuclei using microscopic quadrupole-octupole collective Hamiltonian (QOCH) based on relativistic PC-PK1 energy density functional and δ-interaction pairing. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.054303
2016BA54 Phys.Rev. C 94, 044323 (2016) M.Bao, Y.Lu, Y.M.Zhao, A.Arima Simple relations between masses of mirror nuclei ATOMIC MASSES A=3-110; Z=2-56, N=1-54; deduced a relation between difference of neutron and proton separation energies, and difference of Coulomb energies between two mirror nuclei; deduced mass excesses of nuclei and compared with AME-2012 values.
doi: 10.1103/PhysRevC.94.044323
2016BA64 Phys.Rev. C 94, 064315 (2016) M.Bao, Y.Lu, Y.M.Zhao, A.Arima Predictions of nuclear charge radii NUCLEAR STRUCTURE Z=6-95, N=10-150; analyzed charge radii for nuclei using empirical formulas and CR1999, CR2004 and CR2013 databases for charge radii; predicted values for unknown charge radii of ground states of 1085 nuclei.
doi: 10.1103/PhysRevC.94.064315
2015LU01 Phys.Rev. C 91, 027301 (2015) Spin I ground state probabilities of integrable systems under random interactions
doi: 10.1103/PhysRevC.91.027301
2014LU03 Phys.Rev. C 89, 017301 (2014) Simple correction of nuclear mass models ATOMIC MASSES A=40-260; analyzed deviations of calculated masses by popular theoretical models such as the Skyrme-Hartree-Fock-Bogoliubov approach, the Duflo-Zuker model, the finite range droplet model, and the Weizsacker-Skyrme model from experimental and evaluated values in AME-2012. Odd-even staggering in deviations.
doi: 10.1103/PhysRevC.89.017301
2014LU15 Phys.Rev. C 90, 064313 (2014) Y.Lu, Y.M.Zhao, N.Yoshida, A.Arima Correlations between low-lying yrast states for sd bosons with random interactions
doi: 10.1103/PhysRevC.90.064313
2014SU20 Phys.Rev. C 90, 054318 (2014) B.H.Sun, Y.Lu, J.P.Peng, C.Y.Liu, Y.M.Zhao New charge radius relations for atomic nuclei NUCLEAR STRUCTURE A=20-225; analyzed rms charge radii for 296 stable isotopes; proposed simple relations for charge radii. Comparisons between predictions and experimental data, and with available theoretical calculations. Shape transition shape coexistence.
doi: 10.1103/PhysRevC.90.054318
2013BA60 Phys.Rev. C 88, 064325 (2013) M.Bao, Z.He, Y.Lu, Y.M.Zhao, A.Arima Generalized Garvey-Kelson mass relations ATOMIC MASSES A>16; analyzed Garvey-Kelson mass relations with deviations from experimental data with a different parity of proton and neutron numbers; deduced eight new generalized Garvey-Kelson mass relations; odd-even staggering.
doi: 10.1103/PhysRevC.88.064325
2009LU07 Nucl.Instrum.Methods Phys.Res. B267, 760 (2009) Y.F.Lu, L.Q.Shi, Z.J.He, L.Zhang, B.Zhang, R.Hutton Elastic scattering cross-section of proton from helium at the laboratory angle of 165 degrees NUCLEAR REACTIONS He(p, p), E=1.6-3.6 MeV; measured cross section.
doi: 10.1016/j.nimb.2009.01.011
2009WA26 Chin.Phys.C 33, 838 (2009) S.-Y.Wang, B.-T.Duan, X.-X.Zhu, X.-L.Ren, X.-L.Yang, J.Xi, F.-Z.Lu, D.-P.Sun, Y.-B.Lu, X.-J.Liu, H.Hua, Z.-Y.Li, S.-Q.Zhang, B.Qi, J.-M.Yao, L.-H.Zhu, X.-G.Wu, G.-S.Li, Y.Liu, X.-Q.Li, Y.Zheng, L.-L.Wang, L.Wang Structural evolution of the intruder band in 118Sn NUCLEAR REACTIONS 116Cd(7Li, 4np)118Sn, E=48 MeV; measured Eγ, Iγ, γγ-coin.; deduced energy levels, J, π, intruder band.
doi: 10.1088/1674-1137/33/10/004
2007CH60 Nucl.Instrum.Methods Phys.Res. B262, 161 (2007) X.M.Chen, Y.X.Lu, Z.M.Gao, Y.Cui, Y.W.Liu, J.Du Pure ionization cross section of helium and ionization mechanism
doi: 10.1016/j.nimb.2007.01.083
2007LI79 J.Phys.(London) G34, S1073 (2007) Elliptic flow in a hadron transport model
doi: 10.1088/0954-3899/34/8/S159
2006LU10 J.Phys.(London) G32, 1121 (2006) Y.Lu, M.Bleicher, F.Liu, Z.Liu, H.Petersen, P.Sorensen, H.Stocker, N.Xu, X.Zhu Anisotropic flow at RHIC: how unique is the number-of-constituent-quark scaling? NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated anisotropic flow, transverse momentum dependence. Transport models.
doi: 10.1088/0954-3899/32/8/004
2006XU13 J.Phys.(London) G32, S571 (2006) Z.Xu, Y.Chen, S.Kleinfelder, A.Koohi, S.Li, H.Huang, A.Tai, V.Kushpil, M.Sumbera, C.Colledani, W.Dulinski, A.Himmi, C.Hu, A.Shabetai, M.Szelezniak, I.Valin, M.Winter, M.Miller, B.Surrow, G.Van Nieuwenhuizen, L.Greiner, Y.Lu, H.S.Matis, M.Oldenburg, H.G.Ritter, F.Retiere, A.Rose, L.Ruan, K.Schweda, E.Sichtermann, J.H.Thomas, H.Wieman, N.Xu, Y.Zhang, I.Kotov Measurement of charm flow with the STAR Heavy Flavour Tracker
doi: 10.1088/0954-3899/32/12/S79
2005GU29 Nucl.Phys. A761, 162 (2005) B.Guo, Z.H.Li, W.P.Liu, X.X.Bai, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, J.Su, Y.Lu The 8Li(d, p)9Li reaction and astrophysical 8B(p, γ)9C reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E(cm)=7.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 8B(p, γ), E=low; calculated astrophysical S-factor. DWBA analysis, inverse kinematics, comparison with data.
doi: 10.1016/j.nuclphysa.2005.07.013
2005LI19 Phys.Rev. C 71, 052801 (2005) Z.H.Li, W.P.Liu, X.X.Bai, B.Guo, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, Y.Lu, J.Su, Y.S.Chen, K.S.Wu, N.C.Shu, T.Kajino The 8Li(d, p)9Li reaction and the astrophysical 8Li(n, γ)9Li reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E=39 MeV; measured particle spectra, σ(θ). 8Li(n, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.71.052801
2003LI51 Nucl.Phys. A728, 275 (2003) W.Liu, Z.Li, X.Bai, B.Guo, S.Zeng, Y.Chen, S.Yan, B.Wang, G.Lian, Y.Lu, K.Wu, N.Shu Determination of 11C(p, γ) 12N astrophysical S-factor via measurement of 11C(d, n)12N reaction NUCLEAR REACTIONS 2H(11C, 12N), E(cm)=9.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 11C(p, γ), E=low; deduced astrophysical S-factor, reaction mechanism features. DWBA analysis.
doi: 10.1016/j.nuclphysa.2003.08.017
1998LU02 Phys.Rev. C57, 1983 (1998) Nucleon-Antinucleon Interaction from the Skyrme Model. II. Beyond the Product Ansatz
doi: 10.1103/PhysRevC.57.1983
1996AM01 Z.Phys. A354, 209 (1996) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, Y.Lu, V.E.Markushin On the Relationship of the Scaled Phase Space and Skyrme-Coherent State Treatments of Proton Antiproton Annihilation at Rest NUCLEAR REACTIONS 1H(p-bar, X), E at rest; analyzed pion multiplicities, single pion spectra following (p-bar)p annihilation; deduced scaled phase space, Skyrme-coherent state treatments relationship.
doi: 10.1007/s002180050033
1996LU10 Phys.Rev. C54, 1566 (1996) Nucleon-Antinucleon Interaction from the Skyrme Model
doi: 10.1103/PhysRevC.54.1566
1995AM01 Phys.Rev. C51, 1587 (1995) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, Y.Lu Isospin Recoupling and Bose-Einstein Pion Correlations in (N-bar)N Annihilations
doi: 10.1103/PhysRevC.51.1587
1995LI46 J.Phys.(London) G21, 1199 (1995) The Collective Excitation Spectra of σ, ω Mesons in the Walecka Model of Nuclear Matter
doi: 10.1088/0954-3899/21/9/005
1995LO05 Z.Phys. A351, 83 (1995) Rescattering Mechanisms for (p-bar)p → φX and OZI Rule Re-Examined NUCLEAR REACTIONS 1H(p-bar, X), E at ≈ 2 GeV/c; calculated 2φ, π0φ, γφ production σ, branching ratios. Rescattering mechanism, OZI rule reexamined.
doi: 10.1007/BF01292789
1995LU13 Phys.Rev. C52, 2158 (1995) NN(bar) Annihilation in Large N(C) QCD with ρ and ω Mesons NUCLEAR REACTIONS 1H(p-bar, X), E at rest; calculated multi-pion production branching ratios following annihilation. Large number of colors QCD.
doi: 10.1103/PhysRevC.52.2158
1995LU14 Phys.Rev. C52, 2369 (1995) Pion Correlation from Skyrmion-Anti-Skyrmion Annihilation
doi: 10.1103/PhysRevC.52.2369
1994AL32 Z.Phys. A350, 131 (1994) C.Alexandrou, Y.Lu, R.Rosenfelder Nonperturbative Dressing of Nucleons by Mesons
doi: 10.1007/BF01290681
1994AM11 Phys.Lett. 339B, 201 (1994) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, Y.Lu Bose-Einstein Pion Correlations in (N-bar)N Annihilations
doi: 10.1016/0370-2693(94)91155-X
1994BA53 Phys.Rev. C50, 1300 (1994) M.Batinic, T.-S.H.Lee, M.P.Locher, Y.Lu, A.Svarc Off-Shell Effects for the Reaction pp → πd at High Energies NUCLEAR REACTIONS 1H(polarized p, π+), E=1.3-2.4 GeV; analyzed σ(θ), analyzing power data; deduced pp distortion role. Relativistic meson rescattering model.
doi: 10.1103/PhysRevC.50.1300
1994LO26 Z.Phys. A347, 281 (1994) Rates for the Reactions (p-bar)p → πφ and γφ NUCLEAR REACTIONS 1H(p-bar, X), E at rest; calculated rescattering contributions for πφ-, γφ-production following annihilation.
doi: 10.1007/BF01289796
1993LU05 Z.Phys. A346, 143 (1993) Regge Pole Model with K(*) - K(**) Exchange and Absorption for the(p-bar)p → (Lambda-bar)Lambda Reaction NUCLEAR REACTIONS 1H(p-bar, X), E at 1.436-1.918 MeV/c; calculated σ(θ), polarization, spin correlation parameters in strangeness production. Regge pole model.
doi: 10.1007/BF01294630
1991TA16 Phys.Rev. C44, 1749 (1991) F.Tabakin, R.A.Eisenstein, Y.Lu Spin Observables at Threshold for the Reaction (p-bar)p → (Lambda-bar)Lambda NUCLEAR REACTIONS 1H(p-bar, X), E at 1.435-1.697 GeV/c; analyzed σ, polarization, spin-correlation data for (Lambda)(Lambda-bar) production; deduced partial wave amplitudes.
doi: 10.1103/PhysRevC.44.1749
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