NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Bayar Found 15 matches. 2018BA13 Phys.Rev. C 97, 035203 (2018) M.Bayar, R.Pavao, S.Sakai, E.Oset Role of the triangle singularity in Λ (1405) production in the π-p → K0πΣ and pp → pK+ πK+ πΣ processes NUCLEAR REACTIONS 1H(π-, πK0Σ), 1H(p, pπK+Σ), at Minv=2000-2230 MeV; calculated mass distributions, cross sections by considering mechanism that develops a triangle singularity; evaluated the real part, the imaginary part, and the absolute value of the amplitude; deduced a peak of singularity around 2140 MeV.
doi: 10.1103/PhysRevC.97.035203
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
2016BA21 Eur.Phys.J. A 52, 106 (2016) M.Bayar, P.Fernandez-Soler, Z.-F.Sun, E.Oset States of ρB*B-bar* with J = 3 within the fixed center approximation to Faddeev equations
doi: 10.1140/epja/i2016-16106-2
2015BA15 Eur.Phys.J. A 51, 61 (2015) States of ρD*D*-bar within the fixed center approximation to the Faddeev equations
doi: 10.1140/epja/i2015-15061-8
2014AC02 Eur.Phys.J. A 50, 103 (2014) F.Aceti, M.Bayar, J.M.Dias, E.Oset Prediction of a Zc(4000) D*(D*bar) state and relationship with the claimed Zc(4025)
doi: 10.1140/epja/i2014-14103-1
2014BA08 Eur.Phys.J. A 50, 67 (2014) M.Bayar, W.H.Liang, T.Uchino, C.W.Xiao Description of ρ(1700) as a ρK(K-bar)system with the fixed-center approximation
doi: 10.1140/epja/i2014-14067-0
2013BA46 Nucl.Phys. A914, 349c (2013) The K(bar)NN system revisited including absorption
doi: 10.1016/j.nuclphysa.2013.02.005
2013BA50 Phys.Rev. C 88, 044003 (2013) K(bar)NN absorption within the framework of the fixed-center approximation to Faddeev equations
doi: 10.1103/PhysRevC.88.044003
2013DO19 Nucl.Phys. A914, 499c (2013) A.Dote, M.Bayar, C.W.Xiao, T.Hyodo, M.Oka, E.Oset A narrow quasi-bound state of the DNN system
doi: 10.1016/j.nuclphysa.2013.02.090
2013XI02 Eur.Phys.J. A 49, 22 (2013) The small Kπ component in the K* wave functions
doi: 10.1140/epja/i2013-13022-y
2012BA19 Nucl.Phys. A883, 57 (2012) Improved fixed center approximation of the Faddeev equations for the (K-bar) N N system with S=0
doi: 10.1016/j.nuclphysa.2012.04.005
2012BA49 Phys.Rev. C 86, 044004 (2012) M.Bayar, C.W.Xiao, T.Hyodo, A.Dote, M.Oka, E.Oset Energy and width of a narrow I=1/2 DNN quasibound state
doi: 10.1103/PhysRevC.86.044004
2012MA51 Phys.Rev. C 86, 055201 (2012) A.Martinez Torres, M.Bayar, D.Jido, E.Oset Strategy to find the two Λ(1405) states from lattice QCD simulations
doi: 10.1103/PhysRevC.86.055201
2012OS03 Nucl.Phys. A881, 127 (2012) E.Oset, D.Jido, T.Sekihara, A.Martinez Torres, K.P.Khemchandani, M.Bayar, J.Yamagata-Sekihara A new perspective on the Faddeev equations and the (K-bar)NN system from chiral dynamics and unitarity in coupled channels
doi: 10.1016/j.nuclphysa.2012.02.005
2011BA26 Phys.Rev. C 84, 015209 (2011) M.Bayar, J.Yamagata-Sekihara, E.Oset (K-bar)NN system with chiral dynamics
doi: 10.1103/PhysRevC.84.015209
Back to query form |