NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Garcilazo Found 112 matches. Showing 1 to 100. [Next]2019GA02 Phys.Rev. C 99, 014001 (2019) ΩNN and ΩΩN states
doi: 10.1103/PhysRevC.99.014001
2019GA09 Phys.Lett. B 791, 48 (2019) Towards resolving the 3ΛH lifetime puzzle NUCLEAR STRUCTURE 3H; analyzed available data; deduced hypernuclei T1/2.
doi: 10.1016/j.physletb.2019.02.014
2018GA05 Phys.Rev. C 97, 024002 (2018) Inclusive π+d → p(ηp) process and the ηN scattering length NUCLEAR REACTIONS 2H(π+, pηp), at momentum=898.47 MeV/c; calculated cross section of the inclusive process as a function of ηp invariant mass with the detected proton moving in the forward direction, ηN scattering length using three models of the ηN amplitude.
doi: 10.1103/PhysRevC.97.024002
2018GA24 Phys.Rev. C 98, 024002 (2018) Ωd bound state NUCLEAR STRUCTURE 2H; calculated binding energy of Ω-deuteron bound state, and wave function of the ΩNN state.
doi: 10.1103/PhysRevC.98.024002
2017GA11 Chin.Phys.C 41, 074102 (2017) H.Garcilazo, A.Valcarce, J.Vijande 4ΛΛn system NUCLEAR STRUCTURE 4NN; calculated hypernuclei phase shifts, binding energy. Local central Yukawa-type Malfliet-Tjon interactions.
doi: 10.1088/1674-1137/41/7/074102
2016GA03 Phys.Rev. C 93, 024001 (2016) Strangeness-2 (I, JP) = (1/2, 1/2+) tribaryon resonance
doi: 10.1103/PhysRevC.93.024001
2016GA08 Phys.Rev. C 93, 034001 (2016) Deeply bound Ξ tribaryon
doi: 10.1103/PhysRevC.93.034001
2016GA22 Phys.Rev. C 93, 064003 (2016) D*ΞN bound state in strange three-body systems
doi: 10.1103/PhysRevC.93.064003
2016GA31 Phys.Rev. C 94, 024002 (2016) H.Garcilazo, A.Valcarce, J.Vijande Maximal isospin few-body systems of nucleons and Ξ hyperons
doi: 10.1103/PhysRevC.94.024002
2015GA20 Phys.Rev. C 92, 014004 (2015) Light Ξ hypernuclei
doi: 10.1103/PhysRevC.92.014004
2015GA25 Phys.Rev. C 92, 024006 (2015) H.Garcilazo, A.Valcarce, T.F.Carames J= 3/2 charmed hypertriton NUCLEAR STRUCTURE 3H; calculated binding energy and Fredholm determinants for charmed hypernucleus. Solution of Faddeev equations for the three-baryon system with charm quantum number=+1.
doi: 10.1103/PhysRevC.92.024006
2014GA12 Phys.Rev. C 89, 057001 (2014) Nonexistence of a Λnn bound state NUCLEAR STRUCTURE 3n; analyzed existence of bound state of Λnn hypernuclear system by full Faddeev calculation of the Λnn system using the interactions from the constituent quark cluster model; deduced no evidence for a bound Λnn system attributed in the analysis of 6Li+12C, E=2 GeV/nucleon experiment in 2013 by HypHI Collaboration.
doi: 10.1103/PhysRevC.89.057001
2014GA16 Nucl.Phys. A928, 73 (2014) Three-body model calculations of NΔ and ΔΔ dibaryon resonances
doi: 10.1016/j.nuclphysa.2014.02.019
2013GA02 Phys.Rev.Lett. 110, 012503 (2013) Strangeness -2 Hypertriton NUCLEAR STRUCTURE 3H; calculated binding energy for strange hypertriton. Fadeev equations, comparison with available data.
doi: 10.1103/PhysRevLett.110.012503
2013GA03 Nucl.Phys. A897, 167 (2013) Relativistic three-body calculations of a Y = 1, I =3over2, JP = 2+ π Λ N-πΣN dibaryon
doi: 10.1016/j.nuclphysa.2012.11.006
2013GA43 Phys.Rev.Lett. 111, 172301 (2013) Three Body Calculation of the δδ Dibaryon Candidate D03 (2370)
doi: 10.1103/PhysRevLett.111.172301
2013VI04 Nucl.Phys. A914, 472c (2013) J.Vijande, A.Valcarce, T.F.Carames, H.Garcilazo Heavy hadron spectroscopy: A quark model perspective
doi: 10.1016/j.nuclphysa.2012.12.096
2012GA01 Phys.Rev. C 85, 014002 (2012) Exclusive π+ d → ηpp process
doi: 10.1103/PhysRevC.85.014002
2011GA38 Nucl.Phys. A864, 153 (2011) Coupled channel Faddeev calculations of a (K-bar)Nπ quasibound state NUCLEAR REACTIONS 1H(K-, π0)Σ0, E at 60-250 MeV/c; calculated σ; deduced interaction parameters.
doi: 10.1016/j.nuclphysa.2011.06.022
2010GA10 Phys.Rev. C 81, 055205 (2010) Coupled channels calculation of a πΛN quasibound state
doi: 10.1103/PhysRevC.81.055205
2008GA30 Eur.Phys.J. A 38, 209 (2008) np → ηd near threshold and the s-wave ηN amplitude NUCLEAR REACTIONS 1H(n, dX), E(cm)=0-60 MeV; calculated η-meson production σ. Relativistic three-body model.
doi: 10.1140/epja/i2008-10662-x
2008VA09 Eur.Phys.J. A 37, 217 (2008) A.Valcarce, H.Garcilazo, J.Vijande Towards an understanding of heavy baryon spectroscopy
doi: 10.1140/epja/i2008-10616-4
2007GA12 Phys.Rev. C 75, 034002 (2007) H.Garcilazo, T.Fernandez-Carames, A.Valcarce ΛNN and ΣNN systems at threshold NUCLEAR STRUCTURE 3H; calculated hypernucleus binding energy. Hyperon-deuteron scattering discussed.
doi: 10.1103/PhysRevC.75.034002
2007GA42 Phys.Rev. C 76, 034001 (2007) H.Garcilazo, A.Valcarce, T.Fernandez-Carames ΛNN and ΣNN systems at threshold. II. The effect of D waves
doi: 10.1103/PhysRevC.76.034001
2007GA55 Phys.Rev. C 76, 057002 (2007) nd scattering lengths from a quark-model based NN interaction NUCLEAR REACTIONS n(d, d), E=not given; calculated scattering lengths.
doi: 10.1103/PhysRevC.76.057002
2007GO10 Eur.Phys.J. A 31, 515 (2007) P.Gonzalez, J.Vijande, A.Valcarce, H.Garcilazo A SU(4) (x) O(3) scheme for nonstrange baryons
doi: 10.1140/epja/i2006-10190-9
2007GO30 Nucl.Phys. A790, 550c (2007) P.Gonzalez, J.Vijande, A.Valcarce, H.Garcilazo Symmetry patterns in the (N, Δ) spectrum
doi: 10.1016/j.nuclphysa.2007.03.093
2006FE02 Phys.Rev. C 73, 034004 (2006) T.Fernandez-Carames, A.Valcarce, H.Garcilazo, P.Gonzalez Strange tribaryons
doi: 10.1103/PhysRevC.73.034004
2006GO29 Eur.Phys.J. A 29, 235 (2006) P.Gonzalez, J.Vijande, A.Valcarce, H.Garcilazo Spectral patterns in the nonstrange-baryon spectrum
doi: 10.1140/epja/i2006-10081-1
2006PE19 Acta Phys.Slovaca 56, 261 (2006) Study of the np → ηd reaction within a three-body model NUCLEAR REACTIONS 1H(n, dX), E ≈ threshold; calculated η-meson production σ. Three-body model.
2005GA12 Phys.Rev. C 71, 045204 (2005) Relativistic spin effects in the baryon spectrum
doi: 10.1103/PhysRevC.71.045204
2005GA13 Phys.Rev. C 71, 048201 (2005) Relativistic treatment of the quasivirtual ηNN state
doi: 10.1103/PhysRevC.71.048201
2005GA27 Phys.Rev. C 72, 014003 (2005) Relativistic description of the np → ηd reaction near threshold NUCLEAR REACTIONS 1H(n, dX), E(cm)=0-120 MeV; calculated η-meson production σ; deduced role of final state interaction, relativistic effects, related features. Comparisons with data.
doi: 10.1103/PhysRevC.72.014003
2005VA28 Phys.Rev. C 72, 025206 (2005) A.Valcarce, H.Garcilazo, J.Vijande Constituent quark model study of light- and strange-baryon spectra
doi: 10.1103/PhysRevC.72.025206
2003GA14 Phys.Rev. C 67, 055203 (2003) Momentum-space Faddeev calculations for confining potentials
doi: 10.1103/PhysRevC.67.055203
2003GA17 Phys.Rev. C 67, 067001 (2003) ηd Effective-range formula
doi: 10.1103/PhysRevC.67.067001
2003GA25 Phys.Rev. C 68, 035207 (2003) Chiral quark model with relativistic kinematics
doi: 10.1103/PhysRevC.68.035207
2002GA36 Phys.Rev. C66, 034606 (2002) The Reaction np → ηd Near Threshold NUCLEAR REACTIONS 1H(n, X)2H, E(cm)=0-120 MeV; calculated η meson production σ; deduced reaction mechanism features. Comparison with data.
doi: 10.1103/PhysRevC.66.034606
2002MO08 Phys.Rev. C65, 034006 (2002) R.D.Mota, A.Valcarce, F.Fernandez, D.R.Entem, H.Garcilazo Nonlocal Calculation for Nonstrange Dibaryons and Tribaryons NUCLEAR STRUCTURE A=2-3; calculated two- and three-baryon systems binding energies. Chiral quark cluster model, nonlocal potentials, resonating group method.
doi: 10.1103/PhysRevC.65.034006
2002SU20 Phys.Rev. C66, 034003 (2002) G.Suft, W.Kretschmer, E.Boschitz, R.Meier, B.Brinkmoller, B.van den Brandt, P.Hautle, J.A.Konter, S.Mango, L.Mathelitsch, H.Garcilazo, W.Gruebler Polarization Transfer Observables in πd Elastic Scattering NUCLEAR REACTIONS 2H(π+, π+), E=134, 180 MeV; measured analyzing powers, polarization transfer observables. Polarized target, comparisons with previous results and model predictions.
doi: 10.1103/PhysRevC.66.034003
2001GA06 Phys.Rev. C63, 021001 (2001) Nonexistence of a ηNN Quasibound State NUCLEAR STRUCTURE 2H; calculated η meson elastic scattering σ, scattering lengths; deduced no quasibound state. Solution of Fadeev equations.
doi: 10.1103/PhysRevC.63.021001
2001GA13 Phys.Rev. C63, 035207 (2001) H.Garcilazo, A.Valcarce, F.Fernandez Baryon Spectrum in the Chiral Constituent Quark Model
doi: 10.1103/PhysRevC.63.035207
2001GA43 Nucl.Phys. A689, 193c (2001) Pion and Eta Production Mechanisms NUCLEAR REACTIONS 1H(p, X), (n, X), E ≈ threshold; 2H(π-, X), E ≈ threshold; analyzed pion and eta production σ, reaction mechanism features.
doi: 10.1016/S0375-9474(01)00834-X
2001GA62 Phys.Rev. C64, 058201 (2001) H.Garcilazo, A.Valcarce, F.Fernandez Effect of Higher Orbital Angular Momenta in the Baryon Spectrum
doi: 10.1103/PhysRevC.64.058201
2001MA60 Nucl.Phys. A689, 410c (2001) The Interplay of πN States in Elastic πd Scattering NUCLEAR REACTIONS 2H(π, π), E=134, 180 MeV; calculated σ(θ), spin transfer coefficient; deduced partial wave contributions. Relativistic three-body calculation, comparison with data.
doi: 10.1016/S0375-9474(01)00867-3
2001PE03 Nucl.Phys. A683, 322 (2001) M.T.Pena, H.Garcilazo, D.O.Riska The Reaction pp → ppη and the eta-Nucleon and Nucleon-Nucleon Interactions NUCLEAR REACTIONS 1H(p, pX), E=1260-1340 MeV; calculated η meson production σ, meson exchange contributions; deduced coupling constant. Comparison with data.
doi: 10.1016/S0375-9474(00)00449-8
2001SU13 Nucl.Phys. A689, 406c (2001) G.Suft, W.Beulertz, A.Bock, M.Frank, A.Glombik, J.Hey, B.Kowalzik, W.Kretschmer, S.Merz, H.Meyer, L.Sozuer, R.Weidmann, E.Boschitz, B.Brinkmoller, R.Meier, G.Mertens, B.van den Brandt, P.Hautle, J.A.Konter, S.Mango, L.Mathelitsch, H.Garcilazo, R.Tacik, P.Armaudruz, W.Gruebler Measurement of Polarization Transfer in Pion-Deutron Elastic Scattering NUCLEAR REACTIONS 2H(π+, π+), E=134, 180 MeV; measured polarization transfer observables. Polarized target, comparisons with model predictions.
doi: 10.1016/S0375-9474(01)00866-1
2001VA03 J.Phys.(London) G27, L1 (2001) A.Valcarce, H.Garcilazo, R.D.Mota, F.Fernandez ΔΔ and ΔΔΔ Bound States
doi: 10.1088/0954-3899/27/1/101
2000GA28 Phys.Rev. C61, 064010 (2000) ηd Scattering in the Region of the S11 Resonance
doi: 10.1103/PhysRevC.61.064010
2000GA29 Phys.Rev. C62, 011002 (2000) πd → ηNN Reaction Near Threshold NUCLEAR REACTIONS 2H(π, nX), (π, pX), E at 630-746 MeV/c; calculated η production associated σ, σ(θ); deduced no quasibound state. Comparisons with data.
doi: 10.1103/PhysRevC.62.011002
1999GA14 Phys.Rev. C59, 2389 (1999) Pion-Induced η Production in the Deuteron NUCLEAR REACTIONS 2H(π-, 2nX), E=threshold-1500 MeV; calculated η production σ, σ(θ); deduced reaction mechanism features. Fully covariant formalism. Comparison with data.
doi: 10.1103/PhysRevC.59.2389
1999GA29 Phys.Rev. C60, 027001 (1999) Backward Pion-Deuteron Scattering at High Momentum NUCLEAR REACTIONS 2H(π, π), E at 0.8-3.2 GeV/c; calculated σ(θ=180°); deduced model dependence, cutoff parameter dependence. Relativistic model with single- and double-scattering terms. Comparison with data.
doi: 10.1103/PhysRevC.60.027001
1999GA42 Phys.Rev. C60, 044002 (1999) H.Garcilazo, A.Valcarce, F.Fernandez Bound-State Problem of the NNΔ, NNN, and NN Systems
doi: 10.1103/PhysRevC.60.044002
1999MO01 Phys.Rev. C59, 46 (1999) R.D.Mota, A.Valcarce, F.Fernandez, H.Garcilazo Bound-State Problem of the NΔ and NΔΔ Systems
doi: 10.1103/PhysRevC.59.46
1998MA19 Nucl.Phys. A631, 529c (1998) Deuteron Wave Functions, πN Off-Shell Behavior and πd Polarization Observables NUCLEAR REACTIONS 2H(π, π), E=256 MeV; calculated σ(θ), tensor analyzing power; deduced off-shell effects role. Comparison with data.
doi: 10.1016/S0375-9474(98)00061-X
1997GA15 Phys.Rev. C56, 84 (1997) H.Garcilazo, F.Fernandez, A.Valcarce, R.D.Mota Bound States of ΔΔ and ΔΔΔ Systems
doi: 10.1103/PhysRevC.56.84
1997GA20 Phys.Rev. C56, 1751 (1997) The Isospin 0 J(P) = 0- πNN Resonance
doi: 10.1103/PhysRevC.56.1751
1997GA28 Phys.Rev. C56, 3384 (1997) Lifetime of Bound States of Negative Pions and Neutrons NUCLEAR STRUCTURE 5,6,7n; calculated pion-neutron systems T1/2, decay modes.
doi: 10.1103/PhysRevC.56.3384
1996GA01 Phys.Rev. C53, R20 (1996) Pion Charge Exchange in the Deuteron NUCLEAR REACTIONS 2H(π-, π0), E=164-500 MeV; analyzed σ(θ). Extended three-body model.
doi: 10.1103/PhysRevC.53.R20
1996MO17 Phys.Rev. C54, 2085 (1996) E.Moro, A.Valcarce, H.Garcilazo, F.Fernandez Does the Quark Cluster Model Predict a J(P) = 0- Isospin-2 Dibaryon Resonance ( Question )
doi: 10.1103/PhysRevC.54.2085
1996VA13 Phys.Rev. C54, 1010 (1996) A.Valcarce, H.Garcilazo, F.Fernandez Mass and Width of the d' Resonance in Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 120Sn; calculated d' resonance mass, width. Nucleon-Δ model, Δ-self energy, NΔ-propogators included.
doi: 10.1103/PhysRevC.54.1010
1995GA17 Phys.Rev. C52, 49 (1995) Pion Photoproduction on the Deuteron: The reaction γd → π0d NUCLEAR REACTIONS 2H(γ, π0), (polarized γ, π0), E ≈ 200-1000 MeV; analyzed σ(θ), other polarization observables data. Spectator-on-mass shell, Feynmann diagrams.
doi: 10.1103/PhysRevC.52.49
1995GA21 Phys.Rev. C52, 1126 (1995) Stability of Bound States of Negative Pions and Neutrons
doi: 10.1103/PhysRevC.52.1126
1995GA26 Nucl.Phys. A591, 639 (1995) Theoretical Description of πd Scattering up to 2 GeV/c Incident Momentum NUCLEAR REACTIONS 2H(π, π), E at 0.5-2 GeV/c; analyzed σ(θ). Full three-body calculation, impulse approximation.
doi: 10.1016/0375-9474(95)00295-C
1995GA36 J.Phys.(London) G21, 1231 (1995) πd Scattering Above the 3, 3 Resonance NUCLEAR REACTIONS 2H(π, π), E=294-417 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Relativistic three-body model.
doi: 10.1088/0954-3899/21/9/009
1995VA19 Phys.Rev. C52, 539 (1995) A.Valcarce, H.Garcilazo, F.Fernandez Quark Cluster Model Study of Isospin-2 Dibaryons
doi: 10.1103/PhysRevC.52.539
1995WE05 Phys.Rev. C51, 2575 (1995) M.Wessler, E.Boschitz, B.Brinkmoller, J.Buhler, H.Garcilazo, W.Gyles, W.List, R.Meier, S.Ritt, R.Tacik, J.A.Konter, D.Gill, S.Mango, D.Renker, B.van den Brandt, G.Wait, V.A.Efimovykh, A.I.Kovalev, A.N.Prokofiev, W.Thiel, B.Blankleider Polarization Observables in πd(pol) Elastic Scattering: Analyzing powers τ22 and iT11 in the Forward Hemisphere NUCLEAR REACTIONS 2H(π+, π+), E=100-294 MeV; measured analyzing powers, other observables. Polarized target, two different methods. Model comparison.
doi: 10.1103/PhysRevC.51.2575
1995YE02 Phys.Rev. C52, 2526 (1995) D.M.Yeomans, E.L.Mathie, G.M.Huber, G.J.Lolos, S.I.H.Naqvi, V.Pafilis, G.Jones, M.Sevior, R.P.Trelle, P.Weber, R.Tacik, D.Healey, D.F.Ottewell, G.R.Smith, G.Wait, H.Garcilazo, D.L.Humphrey Analyzing Power Measurements in Pion-Deuteron Breakup at Intermediate Energies NUCLEAR REACTIONS 2H(π+, pπ+), E=80-300 MeV; measured iT11(θ) vs proton momentum following breakup. Polarized target. Relativistic Faddeev calculations comparison.
doi: 10.1103/PhysRevC.52.2526
1994GA03 Phys.Rev. C49, R601 (1994) Reaction γd → π0d and the Small Components of the Deuteron Wave Function NUCLEAR REACTIONS 2H(γ, π0), E < 1 GeV; calculated σ(θ), photon asymmetry. Spectator-on-mass-shell approximation, latest γN → πN amplitude model, fully relativistic approach.
doi: 10.1103/PhysRevC.49.R601
1994GA17 Phys.Rev.Lett. 72, 2971 (1994) Comment on ' Signature of a πNN Resonance in Pionic Double Charge Exchange at Low Energies '
doi: 10.1103/PhysRevLett.72.2971
1994GA48 Few-Body Systems 17, 5 (1994) Three-Pion Resonances
doi: 10.1007/BF01075351
1994VA03 Phys.Rev. C49, 1799 (1994) A.Valcarce, F.Fernandez, H.Garcilazo, M.T.Pena, P.U.Sauer Effects of a Quark-Model-Based Nucleon-Δ Potential on the Two-Nucleon System Above Pion Threshold NUCLEAR REACTIONS 1H(p, X), (p, π+), E=300-900 MeV; 2H(π+, π+), E ≤ 300 MeV; analyzed σ(E). 1H(p, π+), (polarized p, π+), E=578, 800 MeV; 2H(π+, π+), E=140, 256 MeV; analyzed σ(θ), polarization data. Nonrelativistic quark model, nucleon-Δ potential.
doi: 10.1103/PhysRevC.49.1799
1993GA04 Phys.Rev. C47, 957 (1993) Inclusive πd Breakup Reactions NUCLEAR REACTIONS 2H(π+, π+X), (π-, π0X), (π+, pX), (π-, pX), E=96.5 MeV; calculated σ(θ), σ(θ(π), E(π)), σ(θp, Ep). Relativistic three-body model.
doi: 10.1103/PhysRevC.47.957
1993GA21 Nucl.Phys. A562, 521 (1993) A Model for Pion Electro- and Photo-Production from Threshold up to 1 GeV NUCLEAR REACTIONS 1H(γ, π+), (γ, π0), 1n(γ, π-), 1n(γ, π0), E=200-1000 MeV; calculated total σ(E), σ(θ), asymmetry. Generalized Peccei model.
doi: 10.1016/0375-9474(93)90129-L
1992PE03 Phys.Rev. C45, 1487 (1992) M.T.Pena, H.Garcilazo, U.Oelfke, P.U.Sauer Effect of the NΔ Interaction on Observables of the πNN and γNN Systems NUCLEAR REACTIONS 1H(polarized p, π), E=578, 800 MeV; calculated analyzing power, iT11, other polarization observables vs θ. 2H(γ, π0), E=300 MeV; calculated σ(θ), asymmetry, polarization observables vs θ; deduced NΔ-interaction role.
doi: 10.1103/PhysRevC.45.1487
1991GA19 Phys.Rev. C44, 966 (1991) Three-Body K+d Reaction NUCLEAR REACTIONS 2H(K+, K+X), (K+, K0X), (K+, K+), E at 342-587 MeV/c; calculated σ(θ), elastic scattering, target breakup. Relativistic Faddeev calculation.
doi: 10.1103/PhysRevC.44.966
1991MA01 Phys.Rev. C43, 1038 (1991) Origin of Phase Patterns in πd Elastic Scattering NUCLEAR REACTIONS 2H(π, π), E=180-600 MeV; calculated scattering amplitudes; deduced structure origin.
doi: 10.1103/PhysRevC.43.1038
1990GA14 Phys.Rev.Lett. 65, 293 (1990) Inclusive πd Charge Exchange and Breakup NUCLEAR REACTIONS 2H(π-, π0X), E=164.1 MeV; 2H(π+, π+X), E=96.5 MeV; calculated σ(θ(π), E(π)), σ(θ). Relativistic three-body model.
doi: 10.1103/PhysRevLett.65.293
1990GA21 Phys.Rev. C42, 2334 (1990) NΔ Interaction in πd Breakup NUCLEAR REACTIONS 2H(π, π), E=228, 294 MeV; calculated σ(θ), iT11(θ), σ(θp, θ(π)) vs proton momentum; deduced n-Δ interaction role in d-breakup.
doi: 10.1103/PhysRevC.42.2334
1990MA02 Phys.Rev. C41, 193 (1990) E.L.Mathie, V.Pafilis, G.M.Huber, G.J.Lolos, S.I.H.Naqvi, Z.Papandreou, D.M.Yeomans, M.Sevior, R.P.Trelle, D.Ottewell, G.R.Smith, D.Healey, H.Garcilazo Pion-Deuteron Breakup Reaction at 228 MeV NUCLEAR REACTIONS 2H(π, πp), E=228 MeV; measured σ(θ(π), θp) vs proton momentum; deduced possible quark contribution role.
doi: 10.1103/PhysRevC.41.193
1990TA25 Phys.Rev. C42, 1846 (1990) R.Tacik, E.T.Boschitz, W.Gyles, C.R.Ottermann, M.Wessler, U.Wiedner, H.Garcilazo, R.R.Johnson Kinematically Complete Measurement of the π+d → π0pp Charge-Exchange Reaction NUCLEAR REACTIONS 2H(π+, π0p), E=228, 294 MeV; measured σ(θp1, θp2) vs proton momentum. Relativistic Faddeev formalism.
doi: 10.1103/PhysRevC.42.1846
1989GA02 Phys.Rev. C39, 717 (1989) Pionic Components of the Deuteron Wave Function NUCLEAR STRUCTURE 2H; calculated wave function pionic components. Three-body model.
doi: 10.1103/PhysRevC.39.717
1989GA03 Phys.Rev. C39, 942 (1989) H.Garcilazo, E.T.Boschitz, W.Gyles, W.List, C.R.Ottermann, R.Tacik, M.Wessler Polarization Observables in πd(pol) Elastic Scattering: Amplitude analysis NUCLEAR REACTIONS 2H(π, π), E=254, 294 MeV; analyzed polarization observables data; deduced πd helicity amplitudes. Polarized targets, amplitude analysis.
doi: 10.1103/PhysRevC.39.942
1988GA06 Phys.Rev. C37, 2022 (1988) Relativistic Faddeev Calculation of K+d Scattering NUCLEAR REACTIONS 2H(K+, K+), E at 1.5 GeV/c; calculated total, inelastic σ, σ(θ) vs momentum. Relativistic Faddeev calculations.
doi: 10.1103/PhysRevC.37.2022
1988GA15 Phys.Rev.Lett. 61, 1457 (1988) Determination of the Pion-Deuteron Scattering Amplitude NUCLEAR REACTIONS 2H(π, π), E=256, 294 MeV; analyzed σ(θ), analyzing power data; deduced pion-deuteron scattering amplitude.
doi: 10.1103/PhysRevLett.61.1457
1988LI08 Phys.Rev. C37, 1587 (1988) W.List, E.T.Boschitz, H.Garcilazo, W.Gyles, C.R.Ottermann, R.Tacik, M.Wessler, U.Wiedner, R.R.Johnson Neutron-Proton Final-State Interaction in πd Breakup: Differential cross section NUCLEAR REACTIONS 2H(π+, np), E=294 MeV; measured σ(θ(π), θp) vs proton momentum; deduced np-final state interaction role. Kinematically complete experiment.
doi: 10.1103/PhysRevC.37.1587
1988LI09 Phys.Rev. C37, 1594 (1988) W.List, E.T.Boschitz, H.Garcilazo, W.Gyles, C.R.Ottermann, R.Tacik, S.Mango, J.A.Konter, B.van den Brandt, G.R.Smith Neutron-Proton Final-State Interaction in πd Breakup: Vector analyzing power NUCLEAR REACTIONS 2H(π+, np), E=134-228 MeV; measured iT11(θ) following breakup; deduced final state interaction role. Polarized target.
doi: 10.1103/PhysRevC.37.1594
1988OT07 Phys.Rev. C38, 2310 (1988) C.R.Ottermann, E.T.Boschitz, H.Garcilazo, W.Gyles, W.List, R.Tacik, M.Wessler, S.Mango, B.van den Brandt, J.A.Konter, E.L.Mathie Polarization Observables in πd(pol) Elastic Scattering: Analyzing powers τ22 and iT11 NUCLEAR REACTIONS 2H(π, π), E=134-294 MeV; measured iT11, T20, T21, T22 vs θ, other observables. Polarized target, frozen spin mode.
doi: 10.1103/PhysRevC.38.2310
1988PA22 Phys.Rev. C38, 2716 (1988) P.V.Pancella, G.S.Mutchler, S.D.Baker, J.W.Kruk, I.M.Duck, M.D.Corcoran, G.C.Phillips, J.M.Clement, J.A.Buchanan, B.W.Mayes, L.S.Pinsky, W.von Witsch, E.Andrade, H.Garcilazo, J.M.Laget Measurement of π+d → Δ++n at Intermediate Energy NUCLEAR REACTIONS 2H(π+, π+p), E at 312-600 MeV/c; measured σ(θ(π), θ(p)) vs pion momentum; deduced σ(θ) for reaction 2H(π+, Δ++).
doi: 10.1103/PhysRevC.38.2716
1987GA06 Phys.Rev. C35, 1804 (1987) Relativistic Faddeev Theory of the πNN System with Application to πd Scattering NUCLEAR REACTIONS 2H(π, π), E=82-325 MeV; calculated σ(E), σ(θ), iT11(θ), T20(θ). Faddeev theory, polarized target.
doi: 10.1103/PhysRevC.35.1804
1987GA07 Phys.Rev. C35, 1820 (1987) Polarized Pion-Deuteron Breakup in the Region of the 3, 3 Resonance NUCLEAR REACTIONS 2H(π+, π+p), E=180, 228, 294 MeV; calculated vector analyzing power vs θ. Faddeev theory, polarized target breakup.
doi: 10.1103/PhysRevC.35.1820
1986BE25 Nuovo Cim. 93A, 89 (1986) G.H.Berthold, H.Zankel, L.Mathelitsch, H.Garcilazo Momentum Space Calculation of 3He Bound-State Energies NUCLEAR STRUCTURE 3He, 3H; calculated binding energies. 2H; calculated binding energy, quadrupole moment, D-state propability. Momentum space Faddeev equations.
doi: 10.1007/BF02773444
1986GA17 Phys.Rev. C34, 1425 (1986) Applications of the πNN Bound-State Problem: The deuteron and the 4, 4 Resonance NUCLEAR STRUCTURE 2H; calculated binding energy; deduced (4, 4) resonance role. Pion-nulceon-nulceon bound state problem.
doi: 10.1103/PhysRevC.34.1425
1986GY01 Phys.Rev. C33, 583 (1986) W.Gyles, E.T.Boschitz, H.Garcilazo, W.List, E.L.Mathie, C.R.Ottermann, G.R.Smith, R.Tacik, R.R.Johnson π+d → π+pn Reaction as a Test of Relativistic Faddeev Theories: Differential cross section NUCLEAR REACTIONS 2H(π+, π+p), E=228, 294 MeV; measured σ(θπ, θp) vs proton momentum; deduced nonconventional dynamics insignificance. Faddeev method.
doi: 10.1103/PhysRevC.33.583
1986GY02 Phys.Rev. C33, 595 (1986) W.Gyles, E.T.Boschitz, H.Garcilazo, E.L.Mathie, C.R.Ottermann, G.R.Smith, S.Mango, J.A.Konter, R.R.Johnson π+d → π+pn Reaction as a Test of Relativistic Faddeev Theories: Vector analyzing power NUCLEAR REACTIONS 2H(π+, π+p), E=180, 228, 294 MeV; measured vector analysing power iT11(θπ, θp), σ(θπ, θp) vs proton momentum. Relativistic Faddeev method.
doi: 10.1103/PhysRevC.33.595
1985GA10 Phys.Rev. C32, 264 (1985) H.Garcilazo, L.Mathelitsch, H.Zankel Relativistic Effects in the Neutron-Deuteron Scattering Lengths NUCLEAR REACTIONS 2H(n, n), E=low; calculated doublet, quartet scattering lengths; deduced relativistic corrections size. Relativistic, nonrelativistic Faddeev equations, local, nonlocal potentials.
doi: 10.1103/PhysRevC.32.264
1984GA18 Phys.Rev.Lett. 53, 652 (1984) Understanding Polarization Observables in Pion-Deuteron Scattering NUCLEAR REACTIONS 2H(π, π), E=219-325 MeV; calculated polarization observables vs θ, E. Relativistic three-body theory, spin variables inclusion.
doi: 10.1103/PhysRevLett.53.652
1983GA08 Phys.Rev. C27, 2405 (1983) Pion-Deuteron Scattering and the Range of the Pion-Nucleon Amplitude NUCLEAR REACTIONS 2H(π, π), E=50-350 MeV; calculated σ(E); deduced form factor range. Relativistic three-body theory, momentum space.
doi: 10.1103/PhysRevC.27.2405
1982GA07 Phys.Rev. C25, 1649 (1982) Effect of Reflections in Pion-Deuteron Scattering NUCLEAR REACTIONS 2H(π, π), E=142, 181, 228 MeV; calculated σ(θ). Faddeev equations, reflection terms.
doi: 10.1103/PhysRevC.25.1649
1982GA13 Phys.Rev. C25, 2596 (1982) Pion-Deuteron Scattering and the Optical Potential NUCLEAR REACTIONS 2H(π, π), E=100-300 MeV; calculated σ(θ), σ(total), σ(elastic). Optical model.
doi: 10.1103/PhysRevC.25.2596
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