NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = T.Gutsche Found 45 matches. 2010BR11 Phys.Rev. D 82, 054010 (2010) T.Branz, T.Gutsche, V.E.Lyubovitskij Two-photon decay of heavy hadron molecules
doi: 10.1103/PhysRevD.82.054010
2008BR19 Eur.Phys.J. A 37, 303 (2008) T.Branz, T.Gutsche, V.Lyubovitskij f0(980)-meson as a K(K-bar) molecule in a phenomenological Lagrangian approach
doi: 10.1140/epja/i2008-10635-1
2008DO21 Phys.Rev. C 78, 035205 (2008) Y.Dong, A.Faessler, T.Gutsche, V.E.Lyubovitskij Phenomenological Lagrangian approach to the electromagnetic deuteron form factors
doi: 10.1103/PhysRevC.78.035205
2007FA13 Phys.Rev. C 76, 025213 (2007) A.Faessler, T.Gutsche, V.E.Lyubovitskij, I.T.Obukhovsky Role of the ρ meson in the description of pion electroproduction experiments
doi: 10.1103/PhysRevC.76.025213
2007KH13 Nucl.Phys. A790, 518c (2007) K.Khosonthongkee, N.Supanam, Y.Yan, Th.Gutsche, A.Faessler N*(1440) decays in a hybrid baryon model
doi: 10.1016/j.nuclphysa.2007.03.087
2007KU03 Phys.Atomic Nuclei 70, 349 (2007) J.Kuckei, C.Dib, A.Faessler, T.Gutsche, S.G.Kovalenko, V.E.Lyubovitskij, K.Pumsa-ard Strong CP violation and the neutron electric dipole form factor NUCLEAR STRUCTURE 1n; calculated electric dipole form factor. Perturbative chiral quark model.
doi: 10.1134/S1063778807020160
2007TA24 Nucl.Phys. A790, 502c (2007) S.Takeuchi, V.E.Lyubovitskij, Th.Gutsche, A.Faessler X(3872): a q(q-bar)-c(c-bar) molecule with attractive diquarks
doi: 10.1016/j.nuclphysa.2007.03.085
2006DI03 J.Phys.(London) G32, 547 (2006) C.Dib, A.Faessler, T.Gutsche, S.Kovalenko, J.Kuckei, V.E.Lyubovitskij, K.Pumsa-ard The neutron electric dipole form factor in the perturbative chiral quark model NUCLEAR STRUCTURE 1n; calculated electric dipole moment; deduced constraints on CP-violating parameters. Perturbative chiral quark model.
doi: 10.1088/0954-3899/32/4/011
2006DO01 J.Phys.(London) G32, 203 (2006) Y.Dong, A.Faessler, Th.Gutsche, J.Kuckei, V.E.Lyubovitskij, K.Pumsa-ard, P.Shen Nucleon polarizabilities in the perturbative chiral quark model NUCLEAR STRUCTURE 1n, 1H; calculated polarizabilities, meson-cloud effects. Perturbative chiral quark model.
doi: 10.1088/0954-3899/32/2/011
2006OB02 Phys.Lett. B 634, 220 (2006) I.T.Obukhovsky, D.Fedorov, A.Faessler, Th.Gutsche, V.E.Lyubovitskij Quark model description of quasi-elastic pion knockout from the proton at JLAB NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated σ(E) for quasielastic pion knockout. Constituent quark model.
doi: 10.1016/j.physletb.2006.01.038
2005BI21 Phys.Rev. D 72, 053015 (2005) S.M.Bilenky, A.Faessler, T.Gutsche, F.Simkovic Neutrinoless double beta-decay and neutrino mass hierarchies RADIOACTIVITY 76Ge, 82Se, 100Mo, 116Cd, 130Te, 136Xe(2β-); calculated 0νββ-decay T1/2, neutrino mass dependence.
doi: 10.1103/PhysRevD.72.053015
2005FA15 Phys.Rev. D 72, 075006 (2005) A.Faessler, T.Gutsche, S.Kovalenko, V.E.Lyubovitskij, I.Schmidt Scalar meson mediated nuclear μ- - e- conversion NUCLEAR REACTIONS 27Al, 48Ti, 197Au(μ-, e-), E not given; analyzed upper limits for muon-electron conversion branching ratio; deduced mass scale lower limits. Effective Lagrangian approach.
doi: 10.1103/PhysRevD.72.075006
2005GI04 Phys.Rev. C 71, 025202 (2005) F.Giacosa, T.Gutsche, A.Faessler Covariant constituent quark-gluon model for the glueball-quarkonia content of scalar-isoscalar mesons
doi: 10.1103/PhysRevC.71.025202
2005YA04 Phys.Rev. C 71, 025204 (2005) Y.Yan, C.Kobdaj, P.Suebka, Y.M.Zheng, A.Faessler, Th.Gutsche, V.E.Lyubovitskij Electron-positron annihilation into hadron-antihadron pairs
doi: 10.1103/PhysRevC.71.025204
2004CH21 Eur.Phys.J. A 20, 317 (2004) S.Cheedket, V.E.Lyubovitskij, Th.Gutsche, A.Faessler, K.Pumsa-ard, Y.Yan Electromagnetic form factors of the baryon octet in the perturbative chiral quark model NUCLEAR STRUCTURE 1n, 1H; calculated μ, radii, form factors. Perturbative chiral quark model.
doi: 10.1140/epja/i2003-10165-4
2004DR07 Phys.Rev. C 69, 065210 (2004) E.G.Drukarev, M.G.Ryskin, V.A.Sadovnikova, Th.Gutsche, A.Faessler Nucleon QCD sum rules in nuclear matter including four-quark condensates
doi: 10.1103/PhysRevC.69.065210
2004FA12 Phys.Lett. B 590, 57 (2004) A.Faessler, Th.Gutsche, S.Kovalenko, V.E.Lyubovitskij, I.Schmidt, F.Simkovic Vector mesons in nuclear μ- - e- conversion NUCLEAR REACTIONS 48Ti(μ-, e-), E=low; analyzed muon-electron conversion data; deduced lepton flavor violation parameter limits.
doi: 10.1016/j.physletb.2004.03.068
2004IN02 Phys.Rev. C 69, 035207 (2004) T.Inoue, V.E.Lyubovitskij, Th.Gutsche, A.Faessler Updated analysis of meson-nucleon σ terms in the perturbative chiral quark model
doi: 10.1103/PhysRevC.69.035207
2004KH08 J.Phys.(London) G30, 793 (2004) K.Khosonthongkee, V.E.Lyubovitskij, Th.Gutsche, A.Faessler, K.Pumsa-ard, S.Cheedket, Y.Yan Axial form factor of the nucleon in the perturbative chiral quark model NUCLEAR STRUCTURE 1n, 1H; calculated axial form factor. Perturbative chiral quark model, comparison with data.
doi: 10.1088/0954-3899/30/6/009
2004WA19 Phys.Rev. C 70, 015202 (2004) P.Wang, V E.Lyubovitskij, Th.Gutsche, A.Faessler Chiral symmetry restoration in strange hadronic matter
doi: 10.1103/PhysRevC.70.015202
2003DR05 Phys.Rev. D 68, 054021 (2003) E.G.Drukarev, M.G.Ryskin, V.A.Sadovnikova, V.E.Lyubovitskij, Th.Gutsche, A.Faessler Expectation values of four-quark operators in the nucleon
doi: 10.1103/PhysRevD.68.054021
2003PU05 Phys.Rev. C 68, 015205 (2003) K.Pumsa-ard, V.E.Lyubovitskij, Th.Gutsche, A.Faessler, S.Cheedket Electromagnetic nucleon-delta transition in the perturbative chiral quark model
doi: 10.1103/PhysRevC.68.015205
2003WA04 Phys.Rev. C 67, 015210 (2003) P.Wang, V.E.Lyubovitskij, Th.Gutsche, A.Faessler Strange quark matter in a chiral SU(3) quark mean field model
doi: 10.1103/PhysRevC.67.015210
2003YA07 Int.J.Mod.Phys. E12, 367 (2003) Y.Yan, K.Pumsa-ard, R.Tegen, T.Gutsche, V.E.Lyubovitskij, A.Faessler Nucleon-Nucleon High-Energy Scattering NUCLEAR REACTIONS 1H(p, p), (n, p), E(cm) ≈ 7-20 GeV; analyzed σ(t). Effective hadron model, comparison with data.
doi: 10.1142/S0218301303001302
2002LY01 Phys.Rev. C65, 025202 (2002) V.E.Lyubovitskij, Th.Gutsche, A.Faessler, R.Vinh Mau Electromagnetic Couplings of the Chiral Perturbation Theory Lagrangian From the Perturbative Chiral Quark Model
doi: 10.1103/PhysRevC.65.025202
2002LY02 Phys.Rev. C 66, 055204 (2002) V.E.Lyubovitskij, P.Wang, T.Gutsche, A.Faessler Strange nucleon form factors in the perturbative chiral quark model NUCLEAR STRUCTURE 1n, 1H; calculated strange form factors. Perturbative chiral quark model.
doi: 10.1103/PhysRevC.66.055204
2002SI23 Phys.Lett. 544B, 121 (2002) F.Simkovic, V.E.Lyubovitskij, T.Gutsche, A.Faessler, S.Kovalenko New aspects of muon-electron nuclear conversion NUCLEAR REACTIONS 27Al, 48Ti, 197Au(μ-, e-), E not given; calculated matrix elements for muon-electron conversion, tree-level contribution from neutrino exchange.
doi: 10.1016/S0370-2693(02)02466-8
2001GU15 Nucl.Phys. A684, 345c (2001) T.Gutsche, M.Strohmeier-Presicek, R.Vinh Mau, A.Faessler Possible Glueball-Configuration in the Scalar-Isoscalar Meson Sector
doi: 10.1016/S0375-9474(01)00441-9
2001KU14 Nucl.Phys. A689, 327c (2001) V.I.Kukulin, I.T.Obukhovsky, T.Gutsche, V.E.Lyubovitsky, A.Faessler Dressed Six-Quark Bags at Short and Intermediate NN Ranges
doi: 10.1016/S0375-9474(01)00847-8
2001LY01 Phys.Lett. 520B, 204 (2001) V.E.Lyubovitsky, Th.Gutsche, A.Faessler, R.Vinh Mau πN Scattering and Electromagnetic Corrections in the Perturbative Chiral Quark Model
doi: 10.1016/S0370-2693(01)01142-X
2001LY02 Phys.Rev. C64, 065203 (2001) V.E.Lyubovitsky, Th.Gutsche, A.Faessler Electromagnetic Structure of the Nucleon in the Perturbative Chiral Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated μ, radii, form factors. Perturbative chiral quark model. NUCLEAR MOMENTS 1n, 1H; calculated μ, radii, form factors. Perturbative chiral quark model.
doi: 10.1103/PhysRevC.64.065203
2000HO22 Eur.Phys.J. C 16, 677 (2000) R.Hofmann, M.Schumann, T.Gutsche, R.D.Viollier Vacuum Structure of a Modified MIT Bag
doi: 10.1007/s100520000445
1999GU03 Phys.Rev. C59, 630 (1999) T.Gutsche, R.Vinh Mau, M.Strohmeier-Presicek, A.Faessler Radiative Proton-Antiproton Annihilation and Isospin Mixing in Protonium NUCLEAR REACTIONS 1H(p-bar, γX), E at rest; calculated radiative annihilation branching ratios; deduced isospin dependence features. Two-step process, vector dominance model.
doi: 10.1103/PhysRevC.59.630
1999HO12 J.Phys.(London) G25, 1043 (1999) R.Hofmann, A.Faessler, Th.Gutsche Can One Directly Test the Scalar-Vector Lorentz Structure of the Nucleon- and Antinucleon-Nucleus Potential ? NUCLEAR REACTIONS 208Pb(γ, pp-bar), E ≈ 1035-1095 MeV; calculated inclusive pair production σ, σ(θ); deduced nucleon-nucleus potential features. Feasibility for measurement discussed.
doi: 10.1088/0954-3899/25/5/308
1999KE13 J.Phys.(London) G25, 2271 (1999) A.Kercek, T.Gutsche, A.Faessler Protonium Annihilation into Two Mesons in the Quark Annihilation Model NUCLEAR REACTIONS 1H(p-bar, X), E at rest; calculated two-meson branching ratios. Quark annihilation model.
doi: 10.1088/0954-3899/25/11/308
1998ST22 Phys.Lett. 438B, 21 (1998) M.Strohmeier-Presicek, T.Gutsche, A.Faessler, R.Vinh Mau 4π Decay Modes of the f0(1500) Resoonance
doi: 10.1016/S0370-2693(98)01044-2
1997DO16 Nucl.Phys. A625, 1 (1997) C.B.Dover, P.Fishbane, T.Gutsche On Threshold Proton-Antiproton Annihilation to K+-K--Meson States NUCLEAR REACTIONS 1H(p-bar, K+K-X), E not given; calculated φ, ω production σ ratios.
doi: 10.1016/S0375-9474(97)00488-0
1997YA09 Phys.Rev. C56, 1596 (1997) Y.Yan, R.Tegen, T.Gutsche, A.Faessler Sturmian Function Approach and (N-bar)N Bound States
doi: 10.1103/PhysRevC.56.1596
1996BA73 Phys.Lett. 386B, 50 (1996) E.Bauer, T.Gutsche, A.Muhm, R.Thierauf, Y.Yan, A.Faessler, R.Vinh Mau The rho Parameter of Low Energy Proton-Antiproton Scattering in the 3P0 Quark Model NUCLEAR REACTIONS 1H(p-bar, p-bar), E at 0.1-6 GeV/c; analyzed data; deduced model parameter. Nucleon-antinucleon potential model, effective 3P0 quark-antiquark operator.
doi: 10.1016/0370-2693(96)00974-4
1996MU02 Nucl.Phys. A598, 285 (1996) A.Muhm, T.Gutsche, R.Thierauf, Y.Yan, A.Faessler P(P-bar)-Annihilation into Two Mesons in the Quark Annihilation Model Including Final State Interaction NUCLEAR REACTIONS 1H(p-bar, X), E at 500 MeV/c; analyzed partial annihilation σ vs momentum for π+π-, K+K- production. Nonrelativistic A2 quark model.
doi: 10.1016/0375-9474(95)00427-0
1995TH01 Nucl.Phys. A588, 783 (1995) R.Thierauf, T.Gutsche, Y.Yan, A.Muhm, A.Faessler Low-Energy Proton-Antiproton Scattering in the Non-Relativistic 3P0 Quark Model NUCLEAR REACTIONS 1H(p-bar, p-bar), (p-bar, X), (p-bar, n-bar), E at ≤ 0.6 GeV/c; analyzed σ(E), σ(θ). Potential, nonrelativistic model, 3P0 quark model.
doi: 10.1016/0375-9474(95)00079-G
1994GU12 Phys.Lett. 331B, 8 (1994) T.Gutsche, R.D.Viollier, A.Faessler Coupling the Scalar-Isoscalar ' q2(q-bar)2 Meson ' to the Nucleon
doi: 10.1016/0370-2693(94)90935-0
1992DO01 Phys.Lett. 277B, 23 (1992) C.B.Dover, T.Gutsche, A.Faessler, R.Vinh Mau Production of Q(Q-bar)g Hybrid Mesons in (N-bar)N Annihilation NUCLEAR REACTIONS 1H(p-bar, X), E=low; calculated hybrid meson production rate.
doi: 10.1016/0370-2693(92)90950-9
1991DO02 Phys.Rev. C43, 379 (1991) C.B.Dover, T.Gutsche, A.Faessler Case for Quasinuclear N(Bar)N Bound States NUCLEAR REACTIONS 1H(p-bar, X), (n-bar, X), E not given; calculated (π+π-) mass spectrum following annihilation; deduced (N-bar)N bound states role.
doi: 10.1103/PhysRevC.43.379
1989GU18 Nucl.Phys. A503, 737 (1989) T.Gutsche, M.Maruyama, A.Faessler Proton-Antiproton Annihilation into Three Mesons in Flight in the 3P0 Model with a Planar Quark Diagram Topology NUCLEAR REACTIONS 1H(p-bar, X), E not given; calculated multi-pion production σ following annihilation.
doi: 10.1016/0375-9474(89)90438-7
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