NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Xie Found 47 matches. 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
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
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
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
2021AC08 Eur.Phys.J. A 57, 261 (2021) A.Accardi, A.Afanasev, I.Albayrak, S.F.Ali, M.Amaryan, J.R.M.Annand, J.Arrington, A.Asaturyan, H.Atac, H.Avakian, T.Averett, C.Ayerbe Gayoso, X.Bai, L.Barion, M.Battaglieri, V.Bellini, R.Beminiwattha, F.Benmokhtar, V.V.Berdnikov, J.C.Bernauer, V.Bertone, A.Bianconi, A.Biselli, P.Bisio, P.Blunden, M.Boer, M.Bondi, K.-T.Brinkmann, W.J.Briscoe, V.Burkert, T.Cao, A.Camsonne, R.Capobianco, L.Cardman, M.Carmignotto, M.Caudron, L.Causse, A.Celentano, P.Chatagnon, J.-P.Chen, T.Chetry, G.Ciullo, E.Cline, P.L.Cole, M.Contalbrigo, G.Costantini, A.D'Angelo, L.Darme, D.Day, M.Defurne, M.De Napoli, A.Deur, R.De Vita, N.D'Hose, S.Diehl, M.Diefenthaler, B.Dongwi, R.Dupre, H.Dutrieux, D.Dutta, M.Ehrhart, L.El Fassi, L.Elouadrhiri, R.Ent, J.Erler, I.P.Fernando, A.Filippi, D.Flay, T.Forest, E.Fuchey, S.Fucini, Y.Furletova, H.Gao, D.Gaskell, A.Gasparian, T.Gautam, F.-X.Girod, K.Gnanvo, J.Grames, G.N.Grauvogel, P.Gueye, M.Guidal, S.Habet, T.J.Hague, D.J.Hamilton, O.Hansen, D.Hasell, M.Hattawy, D.W.Higinbotham, A.Hobart, T.Horn, C.E.Hyde, H.Ibrahim, A.Ilyichev, A.Italiano, K.Joo, S.J.Joosten, V.Khachatryan, N.Kalantarians, G.Kalicy, B.Karky, D.Keller, C.Keppel, M.Kerver, M.Khandaker, A.Kim, J.Kim, P.M.King, E.Kinney, V.Klimenko, H.-S.Ko, M.Kohl, V.Kozhuharov, B.T.Kriesten, G.Krnjaic, V.Kubarovsky, T.Kutz, L.Lanza, M.Leali, P.Lenisa, N.Liyanage, Q.Liu, S.Liuti, J.Mammei, S.Mantry, D.Marchand, P.Markowitz, L.Marsicano, V.Mascagna, M.Mazouz, M.McCaughan, B.McKinnon, D.McNulty, W.Melnitchouk, A.Metz, Z.-E.Meziani, S.Migliorati, M.Mihovilovic, R.Milner, A.Mkrtchyan, H.Mkrtchyan, A.Movsisyan, H.Moutarde, M.Muhoza, C.Munoz Camacho, J.Murphy, P.Nadel-Turonski, E.Nardi, J.Nazeer, S.Niccolai, G.Niculescu, R.Novotny, J.F.Owens, M.Paolone, L.Pappalardo, R.Paremuzyan, B.Pasquini, E.Pasyuk, T.Patel, I.Pegg, C.Peng, D.Perera, M.Poelker, K.Price, A.J.R.Puckett, M.Raggi, N.Randazzo, M.N.H.Rashad, M.Rathnayake, B.Raue, P.E.Reimer, M.Rinaldi, A.Rizzo, Y.Roblin, J.Roche, O.Rondon-Aramayo, F.Sabatie, G.Salme, E.Santopinto, R.Santos Estrada, B.Sawatzky, A.Schmidt, P.Schweitzer, S.Scopetta, V.Sergeyeva, M.Shabestari, A.Shahinyan, Y.Sharabian, S.Sirca, E.S.Smith, D.Sokhan, A.Somov, N.Sparveris, M.Spata, H.Spiesberger, M.Spreafico, S.Stepanyan, P.Stoler, I.Strakovsky, R.Suleiman, M.Suresh, P.Sznajder, H.Szumila-Vance, V.Tadevosyan, A.S.Tadepalli, A.W.Thomas, M.Tiefenback, R.Trotta, M.Ungaro, P.Valente, M.Vanderhaeghen, L.Venturelli, H.Voskanyan, E.Voutier, B.Wojtsekhowski, M.H.Wood, S.Wood, J.Xie, W.Xiong, Z.Ye, M.Yurov, H.-G.Zaunick, S.Zhamkochyan, J.Zhang, S.Zhang, S.Zhao, Z.W.Zhao, X.Zheng, J.Zhou, C.Zorn An experimental program with high duty-cycle polarized and unpolarized positron beams at Jefferson Lab
doi: 10.1140/epja/s10050-021-00564-y
2019XI03 Eur.Phys.J. A 55, 6 (2019) 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
2018AN13 Phys.Rev. C 98, 045201 (2018) Decay patterns of low-lying Nss-bar states via strangeness channels
doi: 10.1103/PhysRevC.98.045201
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
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
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
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
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
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
2016XI02 Phys.Rev. C 93, 025202 (2016) Photoproduction of the f'2(1525), a2(1320) and k*2(1430)
doi: 10.1103/PhysRevC.93.025202
2016XI03 Phys.Rev. C 93, 035206 (2016) K(pol) induced formation of the f0(980) and α0(980) resonances on proton targets
doi: 10.1103/PhysRevC.93.035206
2015GA31 Phys.Rev. C 92, 035201 (2015) 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
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
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
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
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
2015XI03 Eur.Phys.J. A 51, 111 (2015) 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
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
2015XI08 Phys.Rev. C 92, 065203 (2015) The K-p → f1 (1285) Λ reaction within an effective Lagrangian approach
doi: 10.1103/PhysRevC.92.065203
2014LU10 Phys.Rev. C 90, 034002 (2014) Nucleon pole contribution in the pp → ppK+K- reaction below the φ meson threshold
doi: 10.1103/PhysRevC.90.034002
2014WA52 Phys.Rev. C 90, 065203 (2014) Regge signatures from CLAS Λ(1520) photoproduction data at forward angles
doi: 10.1103/PhysRevC.90.065203
2014XI01 Phys.Rev. C 89, 015203 (2014) Re-analysis of the Λ(1520) photoproduction reaction
doi: 10.1103/PhysRevC.89.015203
2014XI06 Phys.Rev. C 90, 025207 (2014) Role of the Δ* (1940) in the π+p → K+Σ+ (1385) and pp → nK+Σ+ (1385)
doi: 10.1103/PhysRevC.90.025207
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
2014XI09 Phys.Rev. C 90, 055204 (2014) Role of the possible Σ* (1/2-) state in the Λp → Λpπ0 reaction
doi: 10.1103/PhysRevC.90.055204
2013GA17 Phys.Rev. C 87, 055204 (2013) Case in favor of the N*(1700)(3/2-)
doi: 10.1103/PhysRevC.87.055204
2013XI03 Phys.Rev. C 87, 045210 (2013) Role of the N*(2080) in pp → K+Λ(1520) and π-p → K0Λ(1520) reactions
doi: 10.1103/PhysRevC.87.045210
2013XI07 Phys.Rev. C 88, 015203 (2013) Coupling constant for Λ(1405)K(bar)N
doi: 10.1103/PhysRevC.88.015203
2012LI20 Phys.Rev. C 85, 038201 (2012) The K-p → ηΛ reaction in an effective Lagrangian model
doi: 10.1103/PhysRevC.85.038201
2012LI49 Phys.Rev. C 86, 055202 (2012) Evidence for a narrow D03 state in K- p → ηΛ near threshold
doi: 10.1103/PhysRevC.86.055202
2012XI04 Eur.Phys.J. A 48, 146 (2012) The DN, πΣc interaction in finite volume and the Λc(2595) resonance
doi: 10.1140/epja/i2012-12146-x
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
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
2011XI08 Phys.Rev. C 84, 034004 (2011) The pp → pΛK+ and pp → pΣ0 K+ reactions with chiral dynamics
doi: 10.1103/PhysRevC.84.034004
2010XI03 Phys.Rev. C 82, 025210 (2010) Associated strangeness production in the pp → pK++K-p and pp → pK++π0Σ0reactions
doi: 10.1103/PhysRevC.82.025210
2010XI05 Phys.Rev. C 82, 045205 (2010) Role of the N*(2080) resonance in the ψ(pol)p → K+Λ(1520) reaction
doi: 10.1103/PhysRevC.82.045205
2010ZO04 Nucl.Phys. A834, 544c (2010) Strangeness production from pp collisions
doi: 10.1016/j.nuclphysa.2010.01.086
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
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
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
2008XI04 Phys.Rev. C 77, 058202 (2008) Coupling constant for N*(1535)Nρ
doi: 10.1103/PhysRevC.77.058202
2007XI02 Phys.Lett. B 649, 405 (2007) The role of Δ++*(1620) resonances in pp → nK+Σ+ reaction and its important implications
doi: 10.1016/j.physletb.2007.04.035
2005XI04 Chin.Phys.Lett. 22, 2215 (2005) 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
Back to query form Note: The following list of authors and aliases matches the search parameter J.Xie: , J.J.XIE, J.X.XIE |