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NSR database version of April 27, 2024.

Search: Author = J.J.Xie

Found 46 matches.

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2023LI14      Phys.Rev. C 107, 025205 (2023)

J.-F.Li, C.Chen, G.Li, C.-S.An, C.-R.Deng, J.-J.Xie

Quark orbital angular momentum of ground-state octet baryons

doi: 10.1103/PhysRevC.107.025205
Citations: PlumX Metrics

2023XI12      Phys.Rev. C 108, 065204 (2023)

J.-X.Xie, J.-F.Li, Ch.-Sh.An, Ch.-R.Deng, G.Li, J.-J.Xie

Intrinsic sea content of the ground state decuplet baryons in the extended chiral constituent quark model

doi: 10.1103/PhysRevC.108.065204
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2022QI02      Phys.Rev. C 105, 065204 (2022)

R.Qi, J.-B.Wang, G.Li, C.-S.An, C.-R.Deng, J.-J.Xie

Investigations on the flavor-dependent axial charges of the octet baryons

doi: 10.1103/PhysRevC.105.065204
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2022ZH12      Eur.Phys.J. A 58, 20 (2022)

X.Zhang, C.Hanhart, U.-G.Meissner, J.-J.Xie

Remarks on non-perturbative three-body dynamics and its application to the KKK-bar system

doi: 10.1140/epja/s10050-021-00661-y
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2019XI03      Eur.Phys.J. A 55, 6 (2019)

J.-J.Xie, W.-H.Liang, E.Oset

η-4He interaction from the dd → η4He reaction near threshold

NUCLEAR REACTIONS 2H(d, η)4He, E≈threshold; compiled experimental data on total σ (12 data points together); calculated total σ using Bethe-Salpeter Equation (BSE), three-parameter fit to the data; deduced potential, poles of the T matrix, other parameters.

doi: 10.1140/epja/i2019-12693-6
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2018AN13      Phys.Rev. C 98, 045201 (2018)

C.-S.An, J.-J.Xie, G.Li

Decay patterns of low-lying Nss-bar states via strangeness channels

doi: 10.1103/PhysRevC.98.045201
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2017OS05      Acta Phys.Pol. B48, 1793 (2017)

E.Oset, J.J.Xie, W.H.Liang, P.Moskal, M.Skurzok, C.Wilkin, M.Bayar, P.Fernandez-Soler, Z.F.Sun

The pd → η3He Reaction and η3He Bound State? The B*B-bar* - ρ System

NUCLEAR REACTIONS 2H(p, η)3He, E=threshold -threshold+12.5 MeV; analyzed σ and asymmetry data; calculated σ and asymmetry using optical model, η3He binding, Q, optical potential parameters.

doi: 10.5506/APhysPolB.48.1793
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2017WA06      Phys.Rev. C 95, 015205 (2017)

E.Wang, J.-Ju.Xie, W.-H.Liang, F.-K.Guo, E.Oset

Role of a triangle singularity in the γp → K+Λ (1405) reaction

NUCLEAR REACTIONS 1H(γ, Κ+Λ), E=2000, 2100, 2200 MeV; analyzed differential σ(θ) data for Κ+Λ(1405); deduced effects of a triangle singularity mechanism and formation of Λ(1405) resonance structure.

doi: 10.1103/PhysRevC.95.015205
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2017XI03      Phys.Rev. C 95, 015202 (2017)

J.-J.Xie, W.-H.Liang, E.Oset, P.Moskal, M.Skurzok, C.Wilkin

Determination of the η 3He threshold structure from the low energy pd → η 3He reaction

NUCLEAR REACTIONS 1H(d, η3He), E near threshold; analyzed experimental data for total cross sections and asymmetry parameter by an algorithm used in chiral unitary approach; evaluated η 3He scattering amplitude and local Breit-Wigner form of the η 3He amplitude T matrix, binding energy and width of the η 3He system.

doi: 10.1103/PhysRevC.95.015202
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2016CH26      Phys.Rev. C 93, 065203 (2016)

H.-X.Chen, L.-S.Geng, W.-H.Liang, E.Oset, E.Wang, J.-J.Xie

Looking for a hidden-charm pentaquark state with strangeness S = -1 from Ξ-b decay into J/ψ K-Λ

doi: 10.1103/PhysRevC.93.065203
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2016OS01      Nucl.Phys. A954, 371 (2016)

E.Oset, H.-X.Chen, A.Feijoo, L.-S.Geng, W.-H.Liang, D.-M.Li, J.-X.Lu, V.K.Magas, J.Nieves, A.Ramos, L.Roca, E.Wang, J.-J.Xie

Study of reactions disclosing hidden charm pentaquarks with or without strangeness

doi: 10.1016/j.nuclphysa.2016.04.038
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2016SH22      Nucl.Phys. A954, 393 (2016)

C.-W.Shen, F.-K.Guo, J.-J.Xie, B.-S.Zou

Disentangling the hadronic molecule nature of the Pc(4380) pentaquark-like structure

doi: 10.1016/j.nuclphysa.2016.04.034
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2016XI02      Phys.Rev. C 93, 025202 (2016)

J.-J.Xie, E.Oset, L.-S.Geng

Photoproduction of the f'2(1525), a2(1320) and k*2(1430)

doi: 10.1103/PhysRevC.93.025202
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2016XI03      Phys.Rev. C 93, 035206 (2016)

J.-J.Xie, W.-H.Liang, E.Oset

K(pol) induced formation of the f0(980) and α0(980) resonances on proton targets

doi: 10.1103/PhysRevC.93.035206
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2015GA31      Phys.Rev. C 92, 035201 (2015)

E.J.Garzon, J.-J.Xie

Effects of a N*cc(bar) resonance with hidden charm in the π-p → D-Σ+c reaction near threshold

doi: 10.1103/PhysRevC.92.035201
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2015HU06      Phys.Rev. C 91, 065202 (2015)

Y.Huang, J.He, X.-R.Chen, R.Wang, J.-J.Xie, H.-F.Zhang

Theoretical investigation of the decay of the N(2120) resonance to nucleon resonances near 1.7 GeV

doi: 10.1103/PhysRevC.91.065202
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2015LI16      Eur.Phys.J. A 51, 58 (2015)

W.-H.Liang, R.Molina, J.-J.Xie, M.Doring, E.Oset

Predictions for the B0-bar → K*0-bar X(YZ) and B0s-bar → φX(YZ) with X(4160), Y(3940), Z(3930)

doi: 10.1140/epja/i2015-15058-3
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2015LU06      Phys.Rev. C 91, 035204 (2015)

Q.-F.Lu, R.Wang, J.-J.Xie, X.-R.Chen, D.-M.Li

Nucleon resonances in the γp → φK+Λ reaction near threshold

doi: 10.1103/PhysRevC.91.035204
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2015WA21      Phys.Rev. C 92, 015202 (2015)

X.-Y.Wang, X.Cao, J.-J.Xie, X.-R.Chen

Reexamination of the role of the Δ* resonances in the pp → nK+Σ+ reaction

doi: 10.1103/PhysRevC.92.015202
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2015XI03      Eur.Phys.J. A 51, 111 (2015)

J.-Ju.Xie, E.Oset

Photoproduction of the f2(1270) resonance

NUCLEAR REACTIONS 1H(γ, π+π-), E=2.15-4.0 GeV; calculated σ, σ(t) using local hidden gauge approach with incorporated vector meson dominance. Compared with available data.

doi: 10.1140/epja/i2015-15111-3
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2015XI05      Eur.Phys.J. A 51, 130 (2015)

L.-Y.Xiao, Q.-F.Lu, J.-J.Xie, X.-H.Zhong

Role of Λ(1670) in the γp → K+ ηΛ reaction near threshold

doi: 10.1140/epja/i2015-15130-0
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2015XI08      Phys.Rev. C 92, 065203 (2015)

J.-J.Xie

The K-p → f1 (1285) Λ reaction within an effective Lagrangian approach

doi: 10.1103/PhysRevC.92.065203
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2014LU10      Phys.Rev. C 90, 034002 (2014)

Q.-F.Lu, J.-J.Xie, D.-M.Li

Nucleon pole contribution in the pp → ppK+K- reaction below the φ meson threshold

doi: 10.1103/PhysRevC.90.034002
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2014WA52      Phys.Rev. C 90, 065203 (2014)

E.Wang, J.-J.Xie, J.Nieves

Regge signatures from CLAS Λ(1520) photoproduction data at forward angles

doi: 10.1103/PhysRevC.90.065203
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2014XI01      Phys.Rev. C 89, 015203 (2014)

J.-J.Xie, E.Wang, J.Nieves

Re-analysis of the Λ(1520) photoproduction reaction

doi: 10.1103/PhysRevC.89.015203
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2014XI06      Phys.Rev. C 90, 025207 (2014)

J.-J.Xie, E.Wang, B.-S.Zou

Role of the Δ* (1940) in the π+p → K+Σ+ (1385) and pp → nK+Σ+ (1385)

doi: 10.1103/PhysRevC.90.025207
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2014XI07      Phys.Rev. C 90, 048201 (2014)

J.-J.Xie, L.-S.Geng, X.-R.Chen

The p-bar p → φφ reaction in an effective Lagrangian approach

doi: 10.1103/PhysRevC.90.048201
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2014XI09      Phys.Rev. C 90, 055204 (2014)

J.-J.Xie, J.-J.Wu, B.-S.Zou

Role of the possible Σ* (1/2-) state in the Λp → Λpπ0 reaction

doi: 10.1103/PhysRevC.90.055204
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2013GA17      Phys.Rev. C 87, 055204 (2013)

E.J.Garzon, J.J.Xie, E.Oset

Case in favor of the N*(1700)(3/2-)

doi: 10.1103/PhysRevC.87.055204
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2013XI03      Phys.Rev. C 87, 045210 (2013)

J.-J.Xie, B.-C.Liu

Role of the N*(2080) in pp → K+Λ(1520) and π-p → K0Λ(1520) reactions

doi: 10.1103/PhysRevC.87.045210
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2013XI07      Phys.Rev. C 88, 015203 (2013)

J.-J.Xie, B.-C.Liu, C.-S.An

Coupling constant for Λ(1405)K(bar)N

doi: 10.1103/PhysRevC.88.015203
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2012LI20      Phys.Rev. C 85, 038201 (2012)

B.-C.Liu, J.-J.Xie

The K-p → ηΛ reaction in an effective Lagrangian model

doi: 10.1103/PhysRevC.85.038201
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2012LI49      Phys.Rev. C 86, 055202 (2012)

B.-C.Liu, J.-J.Xie

Evidence for a narrow D03 state in K- p → ηΛ near threshold

doi: 10.1103/PhysRevC.86.055202
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2012XI04      Eur.Phys.J. A 48, 146 (2012)

J.-J.Xie, E.Oset

The DN, πΣc interaction in finite volume and the Λc(2595) resonance

doi: 10.1140/epja/i2012-12146-x
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2011XI06      Phys.Rev. C 83, 055204 (2011)

J.-J.Xie, A.Martinez Torres, E.Oset, P.Gonzalez

Plausible explanation for the Δ5/2+(2000) puzzle

doi: 10.1103/PhysRevC.83.055204
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2011XI07      Phys.Rev. C 83, 065207 (2011)

J.-J.Xie, A.Martinez Torres, E.Oset

Faddeev fixed-center approximation to the N(K-bar)K system and the signature of a N*(1920)(1/2+) state

doi: 10.1103/PhysRevC.83.065207
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2011XI08      Phys.Rev. C 84, 034004 (2011)

J.-J.Xie, H.Chen, E.Oset

The pp → pΛK+ and pp → pΣ0 K+ reactions with chiral dynamics

doi: 10.1103/PhysRevC.84.034004
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2010XI03      Phys.Rev. C 82, 025210 (2010)

J.-J.Xie, C.Wilkin

Associated strangeness production in the pp → pK++K-p and pp → pK++π0Σ0reactions

doi: 10.1103/PhysRevC.82.025210
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2010XI05      Phys.Rev. C 82, 045205 (2010)

J.-J.Xie, J.Nieves

Role of the N*(2080) resonance in the ψ(pol)p → K+Λ(1520) reaction

doi: 10.1103/PhysRevC.82.045205
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2010ZO04      Nucl.Phys. A834, 544c (2010)

B.-S.Zou, J.-J.Xie

Strangeness production from pp collisions

doi: 10.1016/j.nuclphysa.2010.01.086
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2009CA19      Phys.Rev. C 80, 025203 (2009)

X.Cao, J.-J.Xie, B.-S.Zou, H.-S.Xu

Evidence of N*(1535) resonance contribution in the pn → dφ reaction

doi: 10.1103/PhysRevC.80.025203
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2009OU01      Nucl.Phys. A821, 220 (2009)

Z.Ouyang, J.-J.Xie, B.-S.Zou, H.-S.Xu

Role of the N*(1440) resonance in the pp → pnπ+ reaction

doi: 10.1016/j.nuclphysa.2009.02.010
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2008XI02      Phys.Rev. C 77, 015206 (2008)

J.-J.Xie, B.-S.Zou, H.-C.Chiang

Role of the N*(1535) in pp → ppφ and π- p → nφ reactions

doi: 10.1103/PhysRevC.77.015206
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2008XI04      Phys.Rev. C 77, 058202 (2008)

J.-J.Xie, C.Wilkin, B.-S.Zou

Coupling constant for N*(1535)Nρ

doi: 10.1103/PhysRevC.77.058202
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2007XI02      Phys.Lett. B 649, 405 (2007)

J.-J.Xie, B.-S.Zou

The role of Δ++*(1620) resonances in pp → nK+Σ+ reaction and its important implications

doi: 10.1016/j.physletb.2007.04.035
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2005XI04      Chin.Phys.Lett. 22, 2215 (2005)

J.-J.Xie, B.-S.Zou, B.-C.Liu

Theoretical Prediction with Monte Carlo Simulation for pp → nK+Σ+ through Δ++* Resonance Production

NUCLEAR REACTIONS 1H(p, K+Σ+), E=2-7 GeV; calculated σ, invariant mass spectra. Monte Carlo simulation.

doi: 10.1088/0256-307X/22/9/021
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