NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Hosaka Found 74 matches. 2022SA13 Eur.Phys.J. A 58, 32 (2022) T.Sangkhakrit, S.Shim, Y.Yan, A.Hosaka Charmed baryon pair production in proton-antiproton collisions in effective Lagrangian and Regge approaches
doi: 10.1140/epja/s10050-022-00678-x
2020IS04 Phys.Rev. C 101, 052201 (2020) T.Ishikawa, H.Fujimura, H.Fukasawa, R.Hashimoto, Q.He, Y.Honda, A.Hosaka, T.Iwata, S.Kaida, J.Kasagi, A.Kawano, S.Kuwasaki, K.Maeda, S.Masumoto, M.Miyabe, F.Miyahara, K.Mochizuki, N.Muramatsu, A.Nakamura, S.X.Nakamura, K.Nawa, S.Ogushi, Y.Okada, K.Okamura, Y.Onodera, K.Ozawa, Y.Sakamoto, M.Sato, T.Sato, H.Shimizu, H.Sugai, K.Suzuki, Y.Tajima, S.Takahashi, Y.Taniguchi, Y.Tsuchikawa, H.Yamazaki, R.Yamazaki, H.Y.Yoshida wN scattering length from w photoproduction on the proton near the reaction threshold NUCLEAR REACTIONS 1H(γ, ω), E=1.09-1.15 GeV; measured Eγ, Iγ, differential σ(θ), and total σ(Eγ) using the FOREST detector at the Research Center for Electron Photon Science of Tohoku University; deduced scattering parameters, spin-averaged scattering length, and effective range. Comparison with other experimental results and with theoretical predictions.
doi: 10.1103/PhysRevC.101.052201
2019NA14 Phys.Rev. C 100, 015205 (2019) Photoproduction and electroproduction of Λ(1405) via γ(*)p → K*+π0Σ0 NUCLEAR REACTIONS 1H(γ, K+π0Σ0), E not given; calculated invariant-mass plots, electromagnetic form factors, and beam asymmetries using effective Lagrangian method. Investigated vector K*-meson coupling constant with Λ(1405) and discussed experimental method for determining the coupling.
doi: 10.1103/PhysRevC.100.015205
2018HI12 Phys.Rev. C 98, 045208 (2018) E.Hiyama, A.Hosaka, M.Oka, J.-M.Richard Quark model estimate of hidden-charm pentaquark resonances
doi: 10.1103/PhysRevC.98.045208
2017SA23 Phys.Rev. C 95, 045206 (2017) Effect of the final state interaction of η'N on the η' photoproduction off the nucleon
doi: 10.1103/PhysRevC.95.045206
2016DM01 Phys.Rev. C 93, 065208 (2016) V.Dmitrasinovic, H.-X.Chen, A.Hosaka Baryon fields with UΛ (3) x UR(3) chiral symmetry. V. Pion-nucleon and kaon-nucleon Σ terms
doi: 10.1103/PhysRevC.93.065208
2016HO12 Nucl.Phys. A954, 341 (2016) A.Hosaka, E.Hiyama, S.H.Kim, H.-C.Kim, H.Nagahiro, H.Noumi, M.Oka, K.Shirotori, T.Yoshida, S.Yasui Production and decay of charmed baryons
doi: 10.1016/j.nuclphysa.2016.05.009
2014KI10 Few-Body Systems 55, 783 (2014) H.-Ch.Kim, H.-Y.Ryu, A.Titov, A.Hosaka φN photoproduction coupled with the K Λ* channel
doi: 10.1007/s00601-014-0883-6
2014NA39 Phys.Rev. C 90, 065201 (2014) Elementarity of composite systems
doi: 10.1103/PhysRevC.90.065201
2014YA12 Nucl.Phys. A927, 110 (2014) Y.Yamaguchi, S.Yasui, A.Hosaka Exotic dibaryons with a heavy antiquark NUCLEAR STRUCTURE 2H; calculated exotic dibaryons binding energy, mass excess, levels, J, π; deduced bound states potential parameters.
doi: 10.1016/j.nuclphysa.2014.04.002
2013KH12 Nucl.Phys. A914, 300c (2013) K.P.Khemchandani, A.Martinez Torres, H.Nagahiro, A.Hosaka Λ and Σ resonances coupled to vector and pseudoscalar mesons
doi: 10.1016/j.nuclphysa.2012.12.095
2013NA35 Phys.Rev. C 88, 055203 (2013) Composite and elementary nature of a resonance in the σ model
doi: 10.1103/PhysRevC.88.055203
2012CH23 Phys.Rev. C 85, 055205 (2012) H.-X.Chen, V.Dmitrasinovic, A.Hosaka Baryon fields with UL (3)xUR(3) chiral symmetry. IV. Interactions with chiral (8, 1)(+)(1, 8) vector and axial-vector mesons and anomalous magnetic moments
doi: 10.1103/PhysRevC.85.055205
2012HY01 Phys.Rev. C 85, 015201 (2012) Compositeness of dynamically generated states in a chiral unitary approach
doi: 10.1103/PhysRevC.85.015201
2012KA20 Eur.Phys.J. A 48, 56 (2012) H.Kaneko, A.Hosaka, O.Scholten A hidden local symmetry approach to rho-meson photoproduction
doi: 10.1140/epja/i2012-12056-y
2010HY04 Nucl.Phys. A835, 402c (2010) Meson-baryon nature of the Λ(1405) in chiral dynamics
doi: 10.1016/j.nuclphysa.2010.01.229
2010OZ01 Phys.Rev. C 81, 035206 (2010) Charged K* photoproduction in a Regge model
doi: 10.1103/PhysRevC.81.035206
2010OZ03 Nucl.Phys. A835, 321c (2010) S.Ozaki, H.Nagahiro, A.Hosaka, O.Scholten Φ Photoproduction in a Coupled-Channel Approach
doi: 10.1016/j.nuclphysa.2010.01.209
2009HU02 Phys.Rev. C 79, 024305 (2009) J.Hu, Y.Ogawa, H.Toki, A.Hosaka, H.Shen Extended relativistic chiral mean field model for nuclear matter
doi: 10.1103/PhysRevC.79.024305
2009OZ01 Phys.Rev. C 80, 035201 (2009), Erratum Phys.Rev. C 81, 059901 (2010) S.Ozaki, A.Hosaka, H.Nagahiro, O.Scholten Coupled-channel analysis for φ photoproduction with Λ(1520)
doi: 10.1103/PhysRevC.80.035201
2008HY02 Phys.Rev. C 78, 025203 (2008) Origin of resonances in the chiral unitary approach
doi: 10.1103/PhysRevC.78.025203
2006CH21 Phys.Lett. B 636, 253 (2006) K.-S.Choi, S.-I.Nam, A.Hosaka, H.-C.Kim A new N*(1675) resonance in the γN → ηN reaction NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm)=1.4-1.9 GeV; calculated η production σ, resonance features. Effective Lagrangians and Born approximation, comparison with data.
doi: 10.1016/j.physletb.2006.03.058
2006HI05 Few-Body Systems 38, 91 (2006) E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro Five-Body Calculation of Resonance and Scattering States of the uudd(s-bar) System
doi: 10.1007/s00601-005-0143-x
2006HY01 Phys.Rev. C 73, 035209 (2006); Erratum Phys.Rev. C 75, 029901 (2007) T.Hyodo, S.Sarkar, A.Hosaka, E.Oset Coupling of (K-bar)* N to the Λ(1520)
doi: 10.1103/PhysRevC.73.035209
2006NA04 Phys.Lett. B 633, 483 (2006) Suppression of Θ+(JP = 3/2±)-photoproduction from the proton NUCLEAR REACTIONS 1n, 1H(γ, X), E=1.73-2.10 GeV; calculated pentaquark production σ, σ(E, θ). Effective Langrangians, comparison with data.
doi: 10.1016/j.physletb.2005.12.059
2006NA15 J.Phys.(London) G32, 777 (2006) Two nucleon states in a chiral quark-diquark model
doi: 10.1088/0954-3899/32/6/003
2006NA24 Phys.Rev. C 74, 025204 (2006) Pentaquark Θ+ production via γ N → (K-bar)*Θ+(3/2±) NUCLEAR REACTIONS 1n, 1H(γ, X), E=2.5-3.5 GeV; calculated pentaquark production σ, σ(θ), asymmetry.
doi: 10.1103/PhysRevC.74.025204
2006NA35 J.Korean Phys.Soc. 49, 1928 (2006) Photo-Production of the Pentaquark Θ+ with Positive and Negative Parities NUCLEAR REACTIONS 1n, 1H(γ, X), E=1.7-2.6 GeV; calculated pentaquark production σ. 1n, 1H(γ, X), E(cm)=2.1 GeV; calculated pentaquark production σ(θ).
2005BO41 Part. and Nucl., Lett. 128, 9 (2005) S.G.Bondarenko, V.V.Burov, N.Hamamoto, A.Hosaka, Y.Manabe, H.Toki One- and two-rank separable kernels of the two-nucleon system in the Bethe-Salpeter approach
2005BO42 Part. and Nucl., Lett. 128, 17 (2005) S.G.Bondarenko, V.V.Burov, N.Hamamoto, A.Hosaka, Y.Manabe, H.Toki Elastic eD scattering in the Bethe-Salpeter approach for the deuteron with the positive- and negative-energy states NUCLEAR REACTIONS 2H(e, e), E not given; analyzed form factors, tensor polarization vs momentum transfer. Bethe-Salpeter approach.
2005HI14 Nucl.Phys. A755, 411c (2005) E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro Five-body calculation of resonance and continuum states of pentaquark baryons with quark-quark correlations
doi: 10.1016/j.nuclphysa.2005.03.047
2005HO13 Phys.Rev. C 71, 045205 (2005) A.Hosaka, T.Hyodo, F.J.Llanes-Estrada, E.Oset, J.R.Pelaez, M.J.Vicente Vacas Two-meson cloud contribution to the baryon antidecuplet binding
doi: 10.1103/PhysRevC.71.045205
2005HO20 Nucl.Phys. A755, 407c (2005) Decay of the Θ+ in a quark model
doi: 10.1016/j.nuclphysa.2005.03.046
2005HY03 Nucl.Phys. A755, 395c (2005) T.Hyodo, A.Hosaka, F.J.Llanes-Estrada, E.Oset, J.R.Pelaez, M.J.Vicente Vacas Two-meson cloud contribution to the baryon antidecuplet self-energy
doi: 10.1016/j.nuclphysa.2005.03.044
2005HY05 Phys.Rev. C 72, 055202 (2005); Erratum Phys.Rev. C 72, 069902 (2005) Phenomenological study of two-meson couplings of Θ+ NUCLEAR REACTIONS 1H(π-, K-X), E ≈ 1920 MeV; 1H(K+, π+X), E ≈ 1200 MeV; calculated pentaquark production σ, σ(θ), interference effects.
doi: 10.1103/PhysRevC.72.055202
2005MA79 J.Phys.(London) G31, 1183 (2005) Relationship between the separable and one-boson-exchange potential for the covariant Bethe-Salpeter equation
doi: 10.1088/0954-3899/31/11/005
2005NA24 Nucl.Phys. A755, 423c (2005) Determination of the parity of the pentaquark baryons : Θ+ and Ξ5 NUCLEAR REACTIONS 1H(polarized p, Σ+X), (K0, X), E(cm) ≈ 2.7-2.8 GeV; calculated pentaquark production σ, σ(θ), dependence on parity.
doi: 10.1016/j.nuclphysa.2005.03.049
2005NA34 Phys.Rev. C 72, 035208 (2005); Erratum Phys.Rev. C 73, 049903 (2006) K.Nagata, A.Hosaka, L.J.Abu-Raddad Mass of the nucleon in a chiral quark-diquark model NUCLEAR STRUCTURE A=1; calculated nucleon mass; deduced mixing angle, coupling constant. Chiral quark-diquark model.
doi: 10.1103/PhysRevC.72.035208
2004HY01 Phys.Lett. B 579, 290 (2004) Determining the Θ+ quantum numbers through the K+p → π+K+n reaction NUCLEAR REACTIONS 1H(K+, K+π+), E at 850 MeV/c; calculated invariant mass spectra, σ(θ), polarization observables, dependence on resonance quantum numbers.
doi: 10.1016/j.physletb.2003.11.026
2004HY02 Prog.Theor.Phys.(Kyoto) 112, 73 (2004) T.Hyodo, S.Nam, D.Jido, A.Hosaka Detailed Analysis of the Chiral Unitary Model for Meson-Baryon Scattering with Flavor SU(3) Breaking Effects
doi: 10.1143/PTP.112.73
2004NA18 Prog.Theor.Phys.(Kyoto) 111, 57 (2004) Structure of the Nuclear Force in a Chiral Quark-Diquark Model
2004NA31 Phys.Lett. B 602, 180 (2004) Threshold production of the Θ+ in a polarized proton reaction NUCLEAR REACTIONS 1H(polarized p, X), E(cm)=2.72-2.82 GeV; calculated pentaquark production σ, σ(θ), analyzing powers.
doi: 10.1016/j.physletb.2004.09.035
2004NA41 Phys.Rev. D 70, 114027 (2004) Production of the pentaquark Θ+ in np scattering NUCLEAR REACTIONS 1H(n, X), E(cm)=2.6-3.5 GeV; calculated hyperon, pentaquark production σ, σ(θ). Effective chiral Langrangians.
doi: 10.1103/PhysRevD.70.114027
2004OG04 Prog.Theor.Phys.(Kyoto) 111, 75 (2004) Y.Ogawa, H.Toki, S.Tamenaga, H.Shen, A.Hosaka, S.Sugimoto, K.Ikeda Chiral Sigma Model with Pion Mean Field in Finite Nuclei NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn, 64Ge, 68Se; calculated single-particle level energies, pion mean-field features.
doi: 10.1143/PTP.111.75
2004TI05 Phys.Rev. C 70, 042202 (2004) A.I.Titov, A.Hosaka, S.Date, Y.Ohashi Θ+ production at high energy
doi: 10.1103/PhysRevC.70.042202
2003BO34 Nucl.Phys. A721, 413c (2003) S.G.Bondarenko, V.V.Burov, N.Hamamoto, A.Hosaka, Y.Manabe, H.Toki Separable kernel of nucleon-nucleon interaction in the Bethe-Salpeter approach for J = 0, 1
doi: 10.1016/S0375-9474(03)01085-6
2003HO27 Nucl.Phys. A721, 705c (2003) Chiral Symmetry of Baryons NUCLEAR REACTIONS 1n, 1H(γ, X), (π, X), E ≈ threshold; calculated pion and η meson production σ, chiral symmetry effects.
doi: 10.1016/S0375-9474(03)01162-X
2003HY03 Phys.Rev. C 68, 018201 (2003) T.Hyodo, S.I.Nam, D.Jido, A.Hosaka Flavor SU(3) breaking effects in the chiral unitary model for meson-baryon scatterings NUCLEAR REACTIONS 1H(K-, X), E at 50-300 MeV/c; analyzed σ, branching ratios, symmetry breaking effects. Chiral unitary model.
doi: 10.1103/PhysRevC.68.018201
2003HY05 Phys.Rev. C 68, 065203 (2003) T.Hyodo, A.Hosaka, E.Oset, A.Ramos, M.J.Vicente Vacas Λ(1405) production in the π-p → K0πΣ reaction NUCLEAR REACTIONS 1H(π-, K0X), E=1690 MeV; calculated hyperon production associated invariant mass spectra, total σ; deduced reaction mechanism features. Comparison with data.
doi: 10.1103/PhysRevC.68.065203
2003KO61 Nucl.Phys. A721, 616c (2003) M.Koma Takayama, A.Hosaka, H.Toki Flavor independent systematics of excited baryons and intra-band transition
doi: 10.1016/S0375-9474(03)01136-9
2003YA15 Nucl.Phys. A721, 735c (2003) Proton - proton bremsstrahlung at the threshold region of the pion production
doi: 10.1016/S0375-9474(03)01169-2
2002AB17 Phys.Rev. C66, 025206 (2002) L.J.Abu-Raddad, A.Hosaka, D.Ebert, H.Toki Path-integral hadronization for the nucleon and its interactions NUCLEAR STRUCTURE 1n, 1H; calculated radii, μ, electric and magnetic form factors, coupling constants. Path-integral hadronization.
doi: 10.1103/PhysRevC.66.025206
2002FI08 Phys.Rev. C66, 014004 (2002) J.O.Fiase, K.R.S.Devan, A.Hosaka Mass Dependence of M3Y-Type Interactions and the Effects of Tensor Correlations
doi: 10.1103/PhysRevC.66.014004
2002JI05 Phys.Rev. C66, 025203 (2002) D.Jido, A.Hosaka, J.C.Nacher, E.Oset, A.Ramos Magnetic moments of the Λ(1405) and Λ(1670) resonances
doi: 10.1103/PhysRevC.66.025203
2001HO04 Nucl.Phys. A680, 167c (2001) Excited Baryons in the Deformed Oscillator Quark Model
doi: 10.1016/S0375-9474(00)00410-3
2001JI07 Prog.Theor.Phys.(Kyoto) 106, 823 (2001) Probing Chiral Symmetry of Nucleons by Threshold ηπ Production NUCLEAR REACTIONS 1H(π-, π-X), E(cm) at 540-620 MeV/c; calculated η production σ, outgoing pion momentum and angular distributions; deduced role of nucleon chiral symmetry.
doi: 10.1143/PTP.106.823
2000HO11 Nucl.Phys. A663-664, 707c (2000) A.Hosaka, D.Jido, Y.Nemoto, M.Oka Chiral Symmetry for Baryons
doi: 10.1016/S0375-9474(99)00727-7
2000HO21 Nucl.Phys. A678, 147 (2000) Electromagnetic Transitions of Excited Baryons in a Deformed Oscillator Quark Model
doi: 10.1016/S0375-9474(00)00319-5
2000JI03 Nucl.Phys. A671, 471 (2000) D.Jido, Y.Nemoto, M.Oka, A.Hosaka Chiral Symmetry for Positive and Negative Parity Nucleons
doi: 10.1016/S0375-9474(99)00844-1
2000KI20 Phys.Rev. C62, 015206 (2000) M.Kimura, T.Miyakawa, A.Suzuki, M.Takayama, K.Tanaka, A.Hosaka Nature of Λ(1405) NUCLEAR REACTIONS 1H(K-, K-), E at 0-200 MeV/c; calculated σ; deduced parameters, Λ(1405) resonance features.
doi: 10.1103/PhysRevC.62.015206
2000NA29 Nucl.Phys. A678, 187 (2000) J.C.Nacher, A.Parreno, E.Oset, A.Ramos, A.Hosaka, M.Oka Chiral Unitary Approach to the πN*N*, νN*N* Couplings for the N*(1535) Resonance
doi: 10.1016/S0375-9474(00)00311-0
2000OS03 Nucl.Phys. A663-664, 497c (2000) E.Oset, A.Hosaka, J.C.Nacher, M.Oka, J.A.Oller, A.Parreno, J.R.Pelaez, A.Ramos, H.Toki SU(3) Chiral Approach to Meson and Baryon Dynamics
doi: 10.1016/S0375-9474(99)00640-5
2000TA08 Nucl.Phys. A663-664, 695c (2000) Systematics of Baryon Masses and Deformed Oscillator Quark Model
doi: 10.1016/S0375-9474(99)00724-1
1999TA32 Prog.Theor.Phys.(Kyoto) 101, 1271 (1999) Systematics of the SU(3) Baryon Spectra and Deformed Oscillator Quark Model
doi: 10.1143/PTP.101.1271
1998HO04 Nucl.Phys. A629, 160c (1998) Baryon Resonances in a Deformed Oscillator Quark Model
doi: 10.1016/S0375-9474(97)00681-7
1998JI01 Phys.Rev.Lett. 80, 448 (1998) Suppression of πNN(*) Coupling and Chiral Symmetry
doi: 10.1103/PhysRevLett.80.448
1998JI02 Nucl.Phys. A629, 156c (1998) Negative Parity Baryons in the QCD Sum Rule
doi: 10.1016/S0375-9474(97)00680-5
1998YO03 Int.J.Mod.Phys. E7, 231 (1998) Nuclear G-Matrix Elements from Nonlocal Potentials NUCLEAR STRUCTURE 16O; calculated G-matrix elements. Local, nonlocal potentials compared.
doi: 10.1142/S0218301398000099
1996HO32 Phys.Rep. 277, 65 (1996) Chiral Bag Model for the Nucleon
doi: 10.1016/S0370-1573(96)00013-0
1995HO06 Phys.Lett. 343B, 1 (1995) Higher Order Corrections to Spin-Isospin Quantities in the Chiral Bag Model
doi: 10.1016/0370-2693(94)01438-I
1995HO19 Phys.Lett. 358B, 184 (1995) The Large-N(c) Limit and the Behavior of (g(A))0 and g(A)
doi: 10.1016/0370-2693(95)01024-K
1990HO25 Z.Phys. A337, 447 (1990) A.Hosaka, T.Schafer, U.Kalmbach Spin Content of the Nucleon in a Non-Topological Chiral Soliton Model NUCLEAR STRUCTURE 1H; calculated spin content; deduced flavor singlet axial vector coupling constant. Nontopological chiral soliton model.
1985HO22 Nucl.Phys. A444, 76 (1985) G-Matrix Effective Interaction with the Paris Potential NUCLEAR STRUCTURE 16O, 40Ca, 90Zr; calculated G-matrix elements; deduced Landau-Migdal parameter. Effective interaction from Paris nucleon-nucleon force.
doi: 10.1016/0375-9474(85)90292-1
1985YA10 Prog.Theor.Phys.(Kyoto) 73, 1165 (1985) M.Yabe, A.Hosaka, K.-I.Kubo, H.Toki On the Central-Odd Components in the G-Matrix Interactions and the Low Energy (p, p') and (p, n) Reactions NUCLEAR REACTIONS 16O(p, n), E=35 MeV; calculated σ(θ). 48Ca(p, p'), E=65 MeV; calculated σ(θ). 58Ni(p, p'), (polarized p, p'), E=65 MeV; calculated σ(θ), analyzing power vs θ.
doi: 10.1143/PTP.73.1165
Back to query form |