NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = T.Gutsche Found 46 matches. 2022WO03 Prog.Theor.Exp.Phys. 2022, 083C01 (2022) R.L.Workman, V.D.Burkert, V.Crede, E.Klempt, U.Thoma, L.Tiator, K.Agashe, G.Aielli, B.C.Allanach, C.Amsler, M.Antonelli, E.C.Aschenauer, D.M.Asner, H.Baer, Sw.Banerjee, R.M.Barnett, L.Baudis, C.W.Bauer, J.J.Beatty, V.I.Belousov, J.Beringer, A.Bettini, O.Biebel, K.M.Black, E.Blucher, R.Bonventre, V.V.Bryzgalov, O.Buchmuller, M.A.Bychkov, R.N.Cahn, M.Carena, A.Ceccucci, A.Cerri, R.S.Chivukula, G.Cowan, K.Cranmer, O.Cremonesi, G.D'Ambrosio, T.Damour, D.de Florian, A.de Gouvea, T.DeGrand, P.de Jong, S.Demers, B.A.Dobrescu, M.D'Onofrio, M.Doser, H.K.Dreiner, P.Eerola, U.Egede, S.Eidelman, A.X.El-Khadra, J.Ellis, S.C.Eno, J.Erler, V.V.Ezhela, W.Fetscher, B.D.Fields, A.Freitas, H.Gallagher, Y.Gershtein, T.Gherghetta, M.C.Gonzalez-Garcia, M.Goodman, C.Grab, A.V.Gritsan, C.Grojean, D.E.Groom, M.Grunewald, A.Gurtu, T.Gutsche, H.E.Haber, M.Hamel, C.Hanhart, S.Hashimoto, Y.Hayato, A.Hebecker, S.Heinemeyer, J.J.Hernandez-Rey, K.Hikasa, J.Hisano, A.Hocker, J.Holder, L.Hsu, J.Huston, T.Hyodo, A.Ianni, M.Kado, M.Karliner, U.F.Katz, M.Kenzie, V.A.Khoze, S.R.Klein, F.Krauss, M.Kreps, P.Krizan, B.Krusche, Y.Kwon, O.Lahav, J.Laiho, L.P.Lellouch, J.Lesgourgues, A.R.Liddle, Z.Ligeti, C.-J.Lin, C.Lippmann, T.M.Liss, L.Littenberg, C.Lourenco, K.S.Lugovsky, S.B.Lugovsky, A.Lusiani, Y.Makida, F.Maltoni, T.Mannel, A.V.Manohar, W.J.Marciano, A.Masoni, J.Matthews, U.-G.Meissner, I.-A.Melzer-Pellmann, M.Mikhasenko, D.J.Miller, D.Milstead, R.E.Mitchell, K.Monig, P.Molaro, F.Moortgat, M.Moskovic, K.Nakamura, M.Narain, P.Nason, S.Navas, A.Nelles, M.Neubert, P.Nevski, Y.Nir, K.A.Olive, C.Patrignani, J.A.Peacock, V.A.Petrov, E.Pianori, A.Pich, A.Piepke, F.Pietropaolo, A.Pomarol, S.Pordes, S.Profumo, A.Quadt, K.Rabbertz, J.Rademacker, G.Raffelt, M.Ramsey-Musolf, B.N.Ratcliff, P.Richardson, A.Ringwald, D.J.Robinson, S.Roesler, S.Rolli, A.Romaniouk, L.J.Rosenberg, J.L.Rosner, G.Rybka, M.G.Ryskin, R.A.Ryutin, Y.Sakai, S.Sarkar, F.Sauli, O.Schneider, S.Schonert, K.Scholberg, A.J.Schwartz, J.Schwiening, D.Scott, F.Sefkow, U.Seljak, V.Sharma, S.R.Sharpe, V.Shiltsev, G.Signorelli, M.Silari, F.Simon, T.Sjostrand, P.Skands, T.Skwarnicki, G.F.Smoot, A.Soffer, M.S.Sozzi, S.Spanier, C.Spiering, A.Stahl, S.L.Stone, Y.Sumino, M.J.Syphers, F.Takahashi, M.Tanabashi, J.Tanaka, M.Tasevsky, K.Terao, K.Terashi, J.Terning, R.S.Thorne, M.Titov, N.P.Tkachenko, D.R.Tovey, K.Trabelsi, P.Urquijo, G.Valencia, R.Van de Water, N.Varelas, G.Venanzoni, L.Verde, I.Vivarelli, P.Vogel, W.Vogelsang, V.Vorobyev, S.P.Wakely, W.Walkowiak, C.W.Walter, D.Wands, D.H.Weinberg, E.J.Weinberg, N.Wermes, M.White, L.R.Wiencke, S.Willocq, C.G.Wohl, C.L.Woody, W.-M.Yao, M.Yokoyama, R.Yoshida, G.Zanderighi, G.P.Zeller, O.V.Zenin, R.-Y.Zhu, Sh.-L.Zhu, F.Zimmermann, P.A.Zyla, for the PDG collaboration Review of Particle Physics
doi: 10.1093/ptep/ptac097
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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