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NSR database version of April 27, 2024.

Search: Author = E.Oset

Found 353 matches.

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2024AB04      Eur.Phys.J. A 60, (2024)

L.M.Abreu, J.Song, P.C.S.Brandao, E.Oset

A note on the tensor and vector exchange contributions to KK-bar KK-bar, DD-bar → DD-bar and π⁺π^- → π⁺π^- reactions

doi: 10.1140/epja/s10050-024-01300-y
Citations: PlumX Metrics

2023MA11      Phys.Rev. C 107, 025202 (2023)

A.Martinez Torres, K.P.Khemchandani, E.Oset

Theoretical study of the γd → π⁰ηd reaction

NUCLEAR REACTIONS ²H(γ, π⁰η), E=950-1150 MeV; calculated differential s(θ, E), contribution from rescattering of pion and Δ-wave component of the deuteron wave function. Comparison to available experimental data.

doi: 10.1103/PhysRevC.107.025202
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2022SO08      Eur.Phys.J. A 58, 133 (2022)

J.Song, L.R.Dai, E.Oset

How much is the compositeness of a bound state constrained by α and r₀? The role of the interaction range

doi: 10.1140/epja/s10050-022-00753-3
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2021IK01      Phys.Rev. C 104, 014614 (2021)

N.Ikeno, R.Molina, E.Oset

Triangle singularity mechanism for the pp → π⁺d fusion reaction

NUCLEAR REACTIONS ¹H(p, dπ⁺), E=400-850 MeV; calculated σ(E) as function of incident proton energy and in terms of contribution of the different spin transitions, differential σ(θ, E) for E(p)=570, 616, 660 MeV using a model based on triangle singularity mechanism. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.014614
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2021WA11      Eur.Phys.J. A 57, 38 (2021)

E.Wang, W.-H.Liang, E.Oset

Analysis of the e⁺e^- → J/ψ D D-bar reaction close to the threshold concerning claims of x_c0(2P) state

doi: 10.1140/epja/s10050-021-00351-9
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2020DA06      Eur.Phys.J. A 56, 154 (2020)

L.R.Dai, E.Oset

Helicity amplitudes in the B-bar → D^*ν-bat_tt decay with V-A breaking in the quark sector

doi: 10.1140/epja/s10050-020-00160-6
Citations: PlumX Metrics

2020IK01      Eur.Phys.J. A 56, 73 (2020)

N.Ikeno, L.Dai, E.Oset

Meson exchange between initial and final state and the R_D ratio in the B-bar → Dν-barℓ((n-bar_tt) reactions

doi: 10.1140/epja/s10050-020-00079-y
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2020MO27      Eur.Phys.J. A 56, 173 (2020)

R.Molina, L.R.Dai, L.S.Geng, E.Oset

J/ψ decay into φ(w) and vector-vector molecular states

doi: 10.1140/epja/s10050-020-00176-y
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2019DA04      Eur.Phys.J. A 55, 20 (2019)

L.R.Dai, R.Pavao, S.Sakai, E.Oset

τ^- → ν_τ M₁M₂, with M₁, M₂ pseudoscalar or vector mesons

doi: 10.1140/epja/i2019-12690-9
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2019DA08      Eur.Phys.J. A 55, 36 (2019)

L.R.Dai, G.Y.Wang, X.Chen, E.Wang, E.Oset, D.M.Li

The B⁺ → J/ψωK⁺ reaction and D^*D-bar^* molecular states

doi: 10.1140/epja/i2019-12706-6
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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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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 M_inv=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
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2018DA22      Eur.Phys.J. A 54, 219 (2018)

L.R.Dai, E.Oset

Polarization amplitudes τ^- → ν_τ decay beyond the Standard Model

doi: 10.1140/epja/i2018-12654-7
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2018PA27      Phys.Rev. C 98, 015201 (2018)

R.Pavao, S.Sakai, E.Oset

Production of N^* (1535) and N^* (1650) in Λ_c → L-bar⁰ ηp (πN) decay

doi: 10.1103/PhysRevC.98.015201
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2018SA11      Eur.Phys.J. A 54, 10 (2018)

S.Sakai, E.Oset, A.Ramos

Triangle singularities in B^- → K^-π^-D⁺_s0 and B^- → K^-π^-D⁺_s1

doi: 10.1140/epja/i2018-12450-5
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2017DE23      Phys.Rev. C 96, 025201 (2017)

V.R.Debastiani, S.Sakai, E.Oset

Role of a triangle singularity in the πN(1535) contribution to γp → pπ⁰η

NUCLEAR REACTIONS ¹H(γ, pπ⁰η), E=930-1410 MeV; analyzed total σ(E) taking into account two mechanisms: γ+p -> Δ(1700) -> ηΔ(1232) -> ηπ⁰p and γ+p -> Δ(1700) -> pN(1535). Role of triangular singularities. Comparison with experimental data.

doi: 10.1103/PhysRevC.96.025201
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2017MI03      Phys.Rev. C 95, 035212 (2017)

K.Miyahara, T.Hyodo, M.Oka, J.Nieves, E.Oset

Theoretical study of the Ξ(1620) and Ξ(1690) resonances in Ξ_c → π⁺ MB decays

doi: 10.1103/PhysRevC.95.035212
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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
Citations: PlumX Metrics

2017RO15      Phys.Rev. C 95, 065211 (2017)

L.Roca, E.Oset

Role of a triangle singularity in the πΔ decay N (1700) (3/2)

doi: 10.1103/PhysRevC.95.065211
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2017SA55      Phys.Rev. C 96, 035202 (2017)

D.Samart, W.-H.Liang, E.Oset

Triangle mechanisms in the build up and decay of the N^* (1875)

doi: 10.1103/PhysRevC.96.035202
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2017SE18      Acta Phys.Pol. B48, 1869 (2017)

T.Sekihara, E.Oset, A.Ramos

What Makes the Peak Structure of the Λp Invariant-mass Spectrum in the K^-3He → Λpn Reaction?

doi: 10.5506/APhysPolB.48.1869
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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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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
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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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2016KA26      Nucl.Phys. A954, 41 (2016)

Y.Kamiya, K.Miyahara, S.Ohnishi, Y.Ikeda, T.Hyodo, E.Oset, W.Weise

Antikaon-nucleon interaction and Λ(1405) in chiral SU(3) dynamics

NUCLEAR REACTIONS ²H(K^-, πΣ), E at 1 GeV/c; calculated σ(M_πΣ), invariant mass distribution of Λ⁺_c decay.

doi: 10.1016/j.nuclphysa.2016.04.013
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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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2016SE17      Prog.Theor.Exp.Phys. 2016, 123D03 (2016)

T.Sekihara, E.Oset, A.Ramos

On the structure observed in the in-flight ³He(K^-, Λp)n reaction at J-PARC

NUCLEAR REACTIONS ³He(K^-, Λp), E=1 GeV; calculated σ, mass spectrum. Faddeev equation.

doi: 10.1093/ptep/ptw166
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2016UC01      Eur.Phys.J. A 52, 43 (2016)

T.Uchino, W.-H.Liang, E.Oset

Baryon states with hidden charm in the extended local hidden gauge approach

doi: 10.1140/epja/i2016-16043-0
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2015AC02      Eur.Phys.J. A 51, 48 (2015)

F.Aceti, J.M.Dias, E.Oset

f₁(1285) decays into a₀(980)π⁰, f₀(980)π⁰ and isospin breaking

doi: 10.1140/epja/i2015-15048-5
Citations: PlumX Metrics

2015BA15      Eur.Phys.J. A 51, 61 (2015)

M.Bayar, X.-L.Ren, E.Oset

States of ρD^*D^*-bar within the fixed center approximation to the Faddeev equations

doi: 10.1140/epja/i2015-15061-8
Citations: PlumX Metrics

2015GA06      Phys.Rev. C 91, 025201 (2015)

E.J.Garzon, E.Oset

Mixing of pseudoscalar-baryon and vector-baryon in the J^P=1/2^- sector and the N^* (1535) and N^* (1650) resonances

doi: 10.1103/PhysRevC.91.025201
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2015LI06      Eur.Phys.J. A 51, 16 (2015)

W.H.Liang, T.Uchino, C.W.Xiao, E.Oset

Baryon states with open charm in the extended local hidden gauge approach

doi: 10.1140/epja/i2015-15016-1
Citations: PlumX Metrics

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 B⁰_s-bar → φX(YZ) with X(4160), Y(3940), Z(3930)

doi: 10.1140/epja/i2015-15058-3
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2015MI19      Phys.Rev. C 92, 055204 (2015)

K.Miyahara, T.Hyodo, E.Oset

Weak decay of Λ⁺_c for the study of Λ(1405) and Λ(1670)

doi: 10.1103/PhysRevC.92.055204
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2015RE02      Phys.Rev. C 91, 045201 (2015)

X.-L.Ren, E.Oset, L.Alvarez-Ruso, M.J.V.Vicente Vacas

Antineutrino induced Λ(1405) production off the proton

doi: 10.1103/PhysRevC.91.045201
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2014AC02      Eur.Phys.J. A 50, 103 (2014)

F.Aceti, M.Bayar, J.M.Dias, E.Oset

Prediction of a Z_c(4000) D^*(D^*bar) state and relationship with the claimed Zc(4025)

doi: 10.1140/epja/i2014-14103-1
Citations: PlumX Metrics

2014AC03      Phys.Rev. C 90, 025208 (2014)

F.Aceti, E.Oset, L.Roca

Composite nature of the Λ(1520) resonance

doi: 10.1103/PhysRevC.90.025208
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2014NI07      Eur.Phys.J. A 50, 57 (2014)

F.Aceti, L.R.Dai, L.S.Geng, E.Oset, Y.Zhang

Meson-baryon components in the states of the baryon decuplet

doi: 10.1140/epja/i2014-14057-2
Citations: PlumX Metrics

2014RE10      Eur.Phys.J. A 50, 133 (2014)

X.-L.Ren, L.-S.Geng, E.Oset, J.Meng

Tes of h₁(1830) made of K^*K^*-bar with the η_c → φK^*K^*-bar decay

doi: 10.1140/epja/i2014-14133-7
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2013AL12      Phys.Rev. C 88, 014006 (2013)

M.Albaladejo, E.Oset

Combined analysis of the pn → dπ⁺π^- and pn → π⁺π^- cross sections and implications for the interpretation of the pn → dπ⁺ π^- data

doi: 10.1103/PhysRevC.88.014006
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2013BA46      Nucl.Phys. A914, 349c (2013)

M.Bayar, E.Oset

The K(bar)NN system revisited including absorption

doi: 10.1016/j.nuclphysa.2013.02.005
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2013BA50      Phys.Rev. C 88, 044003 (2013)

M.Bayar, E.Oset

K(bar)NN absorption within the framework of the fixed-center approximation to Faddeev equations

doi: 10.1103/PhysRevC.88.044003
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2013DA17      Eur.Phys.J. A 49, 130 (2013)

L.Dai, E.Oset

Tests on the molecular structure of f₂(1270), f'₂(1525) from ψ(nS) and Υ(nS) decays

doi: 10.1140/epja/i2013-13130-8
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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
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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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2013JI10      Eur.Phys.J. A 49, 95 (2013)

D.Jido, E.Oset, T.Sekihara

The K^-d → πΣn reaction revisited

doi: 10.1140/epja/i2013-13095-6
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2013MA63      Nucl.Phys. A914, 280c (2013)

A.Martinez Torres, K.P.Khemchandani, D.Jido, Y.Kanada-Enyo, E.Oset

Three-body hadron systems with strangeness

doi: 10.1016/j.nuclphysa.2013.01.026
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2013OS02      Eur.Phys.J. A 49, 32 (2013)

E.Oset

On the ambiguities of sign determination of the S-matrix from energy levels in a finite box

doi: 10.1140/epja/i2013-13032-9
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2013RA30      Eur.Phys.J. A 49, 148 (2013)

A.Ramos, L.Tolos, R.Molina, E.Oset

The width of the ω meson in the nuclear medium

doi: 10.1140/epja/i2013-13148-x
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2013RO11      Phys.Rev. C 87, 055201 (2013)

L.Roca, E.Oset

Λ(1405) poles obtained from π⁰Σ⁰ photoproduction data

doi: 10.1103/PhysRevC.87.055201
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2013RO32      Phys.Rev. C 88, 055206 (2013)

L.Roca, E.Oset

Isospin 0 and 1 resonances from πΣ photoproduction data

doi: 10.1103/PhysRevC.88.055206
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2013TO14      Nucl.Phys. A914, 461c (2013)

L.Tolos, D.Cabrera, C.Garcia-Recio, R.Molina, J.Nieves, E.Oset, A.Ramos, O.Romanets, L.L.Salcedo

Strangeness and charm in nuclear matter

doi: 10.1016/j.nuclphysa.2013.01.018
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2013XI04      Eur.Phys.J. A 49, 52 (2013)

C.W.Xiao, E.Oset

Three methods to detect the predicted D(D-bar) scalar meson X(3700) at 1.76 A GeV

doi: 10.1140/epja/i2013-13052-5
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2013XI12      Eur.Phys.J. A 49, 139 (2013)

C.W.Xiao, E.Oset

Hidden beauty baryon states in the local hidden gauge approach with heavy quark spin symmetry

doi: 10.1140/epja/i2013-13139-y
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2012BA19      Nucl.Phys. A883, 57 (2012)

M.Bayar, E.Oset

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
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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
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2012DO09      Eur.Phys.J. A 48, 114 (2012)

M.Doring, U.-G.Meissner, E.Oset, A.Rusetsky

Coherent investigation of nuclear data at CEA DAM: Theoretical models, experiments and evaluated data

doi: 10.1140/epja/i2012-12114-6
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2012GA05      Eur.Phys.J. A 48, 5 (2012)

E.J.Garzon, E.Oset

Effects of pseudoscalar-baryon channels in the dynamically generated vector-baryon resonances

doi: 10.1140/epja/i2012-12005-x
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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
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2012MO18      Phys.Rev. C 86, 014604 (2012)

R.Molina, C.W.Xiao, E.Oset

J/ψ reaction mechanisms and suppression in the nuclear medium

doi: 10.1103/PhysRevC.86.014604
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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
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2012SE01      Eur.Phys.J. A 48, 10 (2012)

T.Sekihara, A.Martinez Torres, D.Jido, E.Oset

Theoretical study of incoherent φ photoproduction on a deuteron target

NUCLEAR REACTIONS ¹H(γ, φ), ²H(γ, nφ), E=1.6, 1.8, 2.0, 2.2 GeV; calculated various dσ with special attention to Fermi motion of the bound proton.

doi: 10.1140/epja/i2012-12010-1
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2012TO04      Nucl.Phys. A881, 169 (2012)

L.Tolos, R.Molina, E.Oset, A.Ramos

Nuclear medium effects on the (K-bar)^* meson

doi: 10.1016/j.nuclphysa.2011.12.011
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2012XI04      Eur.Phys.J. A 48, 146 (2012)

J.-J.Xie, E.Oset

The DN, πΣ_c interaction in finite volume and the Λ_c(2595) resonance

doi: 10.1140/epja/i2012-12146-x
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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
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2011DO16      Eur.Phys.J. A 47, 139 (2011)

M.Doring, U.-G.Meissner, E.Oset, A.Rusetsky

Unitarized Chiral Perturbation Theory in a finite volume: Scalar meson sector

doi: 10.1140/epja/i2011-11139-7
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2011JI13      Eur.Phys.J. A 47, 42 (2011)

D.Jido, E.Oset, T.Sekihara

Kaon-induced Λ(1405) production on a deuteron target at DAFNE

NUCLEAR REACTIONS ²H(K^-, Λ), (Κ^-, π^-Σ⁺), (Κ^-, π⁺Σ^-), (Κ^-, π⁰Σ⁰), E at 80, 100, 130 MeV/c; measured invariant mass spectra; calculated invariant mass spectra at DAFNE; deduced resonances.

doi: 10.1140/epja/i2011-11042-3
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2011SU25      Eur.Phys.J. A 47, 127 (2011)

B.-X.Sun, H.-X.Chen, E.Oset

ρρN and ρρΔ molecules with J^P = 5/2⁺ and J^P = 7/2⁺

doi: 10.1140/epja/i2011-11127-y
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2011WU05      Phys.Rev. C 84, 015202 (2011)

J.Wu, R.Molina, E.Oset, B.S.Zou

Dynamically generated N^* and Λ^* resonances in the hidden charm sector around 4.3 GeV

doi: 10.1103/PhysRevC.84.015202
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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 Δ_5/2+(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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2010DO15      Eur.Phys.J. A 45, 319 (2010)

M.Doring, D.Jido, E.Oset

Helicity amplitudes of the Λ(1670) and two Λ(1405) as dynamically generated resonances

doi: 10.1140/epja/i2010-11015-0
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2010DO17      Eur.Phys.J. A 46, 315 (2010)

M.Doring, E.Oset, U.-G.Meissner

Evaluation of the polarization observables I^S and I^C in the reaction gp ^(R)p⁰hp

doi: 10.1140/epja/i2010-11047-4
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2010GE03      Eur.Phys.J. A 44, 305 (2010)

L.S.Geng, F.K.Guo, C.Hanhart, R.Molina, E.Oset, B.S.Zou

Study of the f₂(1270), f₂'(1525), f₀(1370) and f₀(1710) in the J/ψ radiative decays

doi: 10.1140/epja/i2010-10971-5
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2010JI17      Nucl.Phys. A835, 59c (2010)

D.Jido, T.Sekihara, Y.Ikeda, T.Hyodo, Y.Kanada-Enyo, E.Oset

The nature of Λ(1405) hyperon resonance in chiral dynamics

doi: 10.1016/j.nuclphysa.2010.01.175
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2010KA37      Eur.Phys.J. A 46, 223 (2010)

M.Kaskulov, E.Hernandez, E.Oset

On the background in the gp ^(R)w(p⁰g)p reaction and mixed event simulation

doi: 10.1140/epja/i2010-11033-x
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2010LI40      Eur.Phys.J. A 44, 479 (2010)

W.H.Liang, R.Molina, E.Oset

Radiative open charm decay of the Y(3940), Z(3930), X(4160) resonances

doi: 10.1140/epja/i2010-10972-4
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2010MA11      Phys.Rev. C 81, 024609 (2010)

V.K.Magas, J.Yamagata-Sekihara, S.Hirenzaki, E.Oset, A.Ramos

Proton emission off nuclei induced by kaons in flight

doi: 10.1103/PhysRevC.81.024609
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2010MA25      Phys.Rev. C 81, 055202 (2010)

A.Martinez Torres, E.Oset

The γd → K⁺K^-np reaction and an alternative explanation for the "Θ⁺(1540) pentaquark" peak

doi: 10.1103/PhysRevC.81.055202
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2010OS03      Eur.Phys.J. A 44, 445 (2010)

E.Oset, A.Ramos

Dynamically generated resonances from the vector octet-baryon octet interaction

doi: 10.1140/epja/i2010-10957-3
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2010OS05      Nucl.Phys. A835, 271c (2010)

E.Oset, S.Sarkar, B.X.Sun, M.J.Vicente Vacas, A.Ramos, P.Gonzalez, J.Vijande, A.Martinez Torres, K.Khemchandani

Baryon Resonances

doi: 10.1016/j.nuclphysa.2010.01.202
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2010RA24      Nucl.Phys. A835, 382c (2010)

A.Ramos, V.K.Magas, J.Yamagata-Sekihara, S.Hirenzaki, E.Oset

The (K^-, p) reaction on nuclei with in-flight kaons

doi: 10.1016/j.nuclphysa.2010.01.224
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2010SA31      Eur.Phys.J. A 44, 431 (2010)

S.Sarkar, B.-X.Sun, E.Oset, M.J.Vicente Vacas

Dynamically generated resonances from the vector octet-baryon decuplet interaction

doi: 10.1140/epja/i2010-10956-4
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2010TO08      Phys.Rev. C 82, 045210 (2010)

L.Tolos, R.Molina, E.Oset, A.Ramos

(K-bar)^* mesons in dense matter

doi: 10.1103/PhysRevC.82.045210
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2009GA36      Eur.Phys.J. A 41, 85 (2009)

D.Gamermann, E.Oset, B.S.Zou

The radiative decay of ψ(3770) into the predicted scalar state X(3700)

doi: 10.1140/epja/i2009-10767-8
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2009GE03      Phys.Rev. C 79, 025203 (2009)

L.S.Geng, E.Oset, B.S.Zou, M.Doring

Role of the N^*(1535) in the J/ψ → p(bar)ηp and J/ψ → p(bar)K⁺ Λ reactions

doi: 10.1103/PhysRevC.79.025203
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2009GE05      Eur.Phys.J. A 39, 81 (2009)

L.S.Geng, E.Oset, J.R.Pelaez, L.Roca

Nature of the axial-vector mesons from their N_c behavior within the chiral unitary approach

doi: 10.1140/epja/i2008-10689-y
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2009GO07      Phys.Rev. C 79, 025209 (2009)

P.Gonzalez, E.Oset, J.Vijande

Explanation of the Δ_5/2^-(1930) as a ρΔ bound state

doi: 10.1103/PhysRevC.79.025209
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2009JI11      Eur.Phys.J. A 42, 257 (2009)

D.Jido, E.Oset, T.Sekihara

Kaonic production of Λ(1405) off deuteron target in chiral dynamics

doi: 10.1140/epja/i2009-10875-5
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2009MA34      Phys.Rev. C 79, 065207 (2009)

A.Martinez Torres, K.P.Khemchandani, E.Oset

Solution to Faddeev equations with two-body experimental amplitudes as input and application to J^P=1/2⁺, S=0 baryon resonances

doi: 10.1103/PhysRevC.79.065207
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2009MA67      Eur.Phys.J. A 41, 361 (2009)

A.Martinez Torres, K.P.Khemchandani, U.-G.Meissner, E.Oset

Searching for signatures around 1920 MeV of a Nstate of three hadron nature

doi: 10.1140/epja/i2009-10834-2
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2009MO41      Eur.Phys.J. A 42, 31 (2009)

R.Molina, D.Gamermann, E.Oset, L.Tolos

Charm and hidden charm scalar mesons in the nuclear medium

doi: 10.1140/epja/i2009-10853-y
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2009OS02      Nucl.Phys. A827, 255c (2009)

E.Oset, L.S.Geng, D.Gamermann, R.Molina, D.Nicmorus, J.Yamagata-Sekihara, H.Nagahiro, S.Hirenzaki, D.Jido, M.Doring, A.Ramos

Meson and Baryon resonances

doi: 10.1016/j.nuclphysa.2009.05.050
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2009TO09      Nucl.Phys. A827, 249c (2009)

L.Tolos, R.Molina, D.Gamermann, E.Oset

Charm and Hidden Charm Scalar Resonances in Nuclear Matter

doi: 10.1016/j.nuclphysa.2009.05.049
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2008DO04      Phys.Rev. C 77, 024602 (2008)

M.Doring, E.Oset

s-wave pion-nucleus optical potential

doi: 10.1103/PhysRevC.77.024602
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