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NSR database version of April 11, 2024.

Search: Author = H.Garcilazo

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2019GA02      Phys.Rev. C 99, 014001 (2019)

H.Garcilazo, A.Valcarce

ΩNN and ΩΩN states

doi: 10.1103/PhysRevC.99.014001
Citations: PlumX Metrics


2019GA09      Phys.Lett. B 791, 48 (2019)

A.Gal, H.Garcilazo

Towards resolving the 3ΛH lifetime puzzle

NUCLEAR STRUCTURE 3H; analyzed available data; deduced hypernuclei T1/2.

doi: 10.1016/j.physletb.2019.02.014
Citations: PlumX Metrics


2018GA05      Phys.Rev. C 97, 024002 (2018)

H.Garcilazo

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
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2018GA24      Phys.Rev. C 98, 024002 (2018)

H.Garcilazo, A.Valcarce

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
Citations: PlumX Metrics


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
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2016GA03      Phys.Rev. C 93, 024001 (2016)

H.Garcilazo

Strangeness-2 (I, JP) = (1/2, 1/2+) tribaryon resonance

doi: 10.1103/PhysRevC.93.024001
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2016GA08      Phys.Rev. C 93, 034001 (2016)

H.Garcilazo, A.Valcarce

Deeply bound Ξ tribaryon

doi: 10.1103/PhysRevC.93.034001
Citations: PlumX Metrics


2016GA22      Phys.Rev. C 93, 064003 (2016)

H.Garcilazo, A.Valcarce

D*ΞN bound state in strange three-body systems

doi: 10.1103/PhysRevC.93.064003
Citations: PlumX Metrics


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
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2015GA20      Phys.Rev. C 92, 014004 (2015)

H.Garcilazo, A.Valcarce

Light Ξ hypernuclei

doi: 10.1103/PhysRevC.92.014004
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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
Citations: PlumX Metrics


2014GA12      Phys.Rev. C 89, 057001 (2014)

H.Garcilazo, A.Valcarce

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
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2014GA16      Nucl.Phys. A928, 73 (2014)

A.Gal, H.Garcilazo

Three-body model calculations of NΔ and ΔΔ dibaryon resonances

doi: 10.1016/j.nuclphysa.2014.02.019
Citations: PlumX Metrics


2013GA02      Phys.Rev.Lett. 110, 012503 (2013)

H.Garcilazo, A.Valcarce

Strangeness -2 Hypertriton

NUCLEAR STRUCTURE 3H; calculated binding energy for strange hypertriton. Fadeev equations, comparison with available data.

doi: 10.1103/PhysRevLett.110.012503
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2013GA03      Nucl.Phys. A897, 167 (2013)

H.Garcilazo, A.Gal

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
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2013GA43      Phys.Rev.Lett. 111, 172301 (2013)

A.Gal, H.Garcilazo

Three Body Calculation of the δδ Dibaryon Candidate D03 (2370)

doi: 10.1103/PhysRevLett.111.172301
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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
Citations: PlumX Metrics


2012GA01      Phys.Rev. C 85, 014002 (2012)

H.Garcilazo

Exclusive π+ d → ηpp process

doi: 10.1103/PhysRevC.85.014002
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2011GA38      Nucl.Phys. A864, 153 (2011)

A.Gal, H.Garcilazo

Coupled channel Faddeev calculations of a (K-bar)Nπ quasibound state

NUCLEAR REACTIONS 1H(K-, π00, E at 60-250 MeV/c; calculated σ; deduced interaction parameters.

doi: 10.1016/j.nuclphysa.2011.06.022
Citations: PlumX Metrics


2010GA10      Phys.Rev. C 81, 055205 (2010)

H.Garcilazo, A.Gal

Coupled channels calculation of a πΛN quasibound state

doi: 10.1103/PhysRevC.81.055205
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2008GA30      Eur.Phys.J. A 38, 209 (2008)

H.Garcilazo, M.T.Pena

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
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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
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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
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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
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2007GA55      Phys.Rev. C 76, 057002 (2007)

H.Garcilazo, A.Valcarce

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
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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
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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
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2006FE02      Phys.Rev. C 73, 034004 (2006)

T.Fernandez-Carames, A.Valcarce, H.Garcilazo, P.Gonzalez

Strange tribaryons

doi: 10.1103/PhysRevC.73.034004
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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
Citations: PlumX Metrics


2006PE19      Acta Phys.Slovaca 56, 261 (2006)

M.T.Pena, H.Garcilazo

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)

H.Garcilazo

Relativistic spin effects in the baryon spectrum

doi: 10.1103/PhysRevC.71.045204
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2005GA13      Phys.Rev. C 71, 048201 (2005)

H.Garcilazo

Relativistic treatment of the quasivirtual ηNN state

doi: 10.1103/PhysRevC.71.048201
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2005GA27      Phys.Rev. C 72, 014003 (2005)

H.Garcilazo, M.T.Pena

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
Citations: PlumX Metrics


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
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2003GA14      Phys.Rev. C 67, 055203 (2003)

H.Garcilazo

Momentum-space Faddeev calculations for confining potentials

doi: 10.1103/PhysRevC.67.055203
Citations: PlumX Metrics


2003GA17      Phys.Rev. C 67, 067001 (2003)

H.Garcilazo

ηd Effective-range formula

doi: 10.1103/PhysRevC.67.067001
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2003GA25      Phys.Rev. C 68, 035207 (2003)

H.Garcilazo, A.Valcarce

Chiral quark model with relativistic kinematics

doi: 10.1103/PhysRevC.68.035207
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2002GA36      Phys.Rev. C66, 034606 (2002)

H.Garcilazo, M.T.Pena

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
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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
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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
Citations: PlumX Metrics


2001GA06      Phys.Rev. C63, 021001 (2001)

H.Garcilazo, M.T.Pena

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
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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
Citations: PlumX Metrics


2001GA43      Nucl.Phys. A689, 193c (2001)

H.Garcilazo

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
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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
Citations: PlumX Metrics


2001MA60      Nucl.Phys. A689, 410c (2001)

L.Mathelitsch, H.Garcilazo

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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2000GA28      Phys.Rev. C61, 064010 (2000)

H.Garcilazo, M.T.Pena

ηd Scattering in the Region of the S11 Resonance

doi: 10.1103/PhysRevC.61.064010
Citations: PlumX Metrics


2000GA29      Phys.Rev. C62, 011002 (2000)

H.Garcilazo, M.T.Pena

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
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1999GA14      Phys.Rev. C59, 2389 (1999)

H.Garcilazo, M.T.Pena

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
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1999GA29      Phys.Rev. C60, 027001 (1999)

H.Garcilazo, L.Mathelitsch

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
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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
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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
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1998MA19      Nucl.Phys. A631, 529c (1998)

L.Mathelitsch, H.Garcilazo

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
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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
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1997GA20      Phys.Rev. C56, 1751 (1997)

H.Garcilazo

The Isospin 0 J(P) = 0- πNN Resonance

doi: 10.1103/PhysRevC.56.1751
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1997GA28      Phys.Rev. C56, 3384 (1997)

H.Garcilazo, A.Queijeiro

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
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1996GA01      Phys.Rev. C53, R20 (1996)

H.Garcilazo

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
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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
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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
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1995GA17      Phys.Rev. C52, 49 (1995)

H.Garcilazo, E.Moya de Guerra

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
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1995GA21      Phys.Rev. C52, 1126 (1995)

H.Garcilazo

Stability of Bound States of Negative Pions and Neutrons

doi: 10.1103/PhysRevC.52.1126
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1995GA26      Nucl.Phys. A591, 639 (1995)

H.Garcilazo, L.Mathelitsch

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
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1995GA36      J.Phys.(London) G21, 1231 (1995)

H.Garcilazo

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
Citations: PlumX Metrics


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
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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
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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
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1994GA03      Phys.Rev. C49, R601 (1994)

H.Garcilazo, E.Moya de Guerra

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
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1994GA17      Phys.Rev.Lett. 72, 2971 (1994)

H.Garcilazo, L.Mathelitsch

Comment on ' Signature of a πNN Resonance in Pionic Double Charge Exchange at Low Energies '

doi: 10.1103/PhysRevLett.72.2971
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1994GA48      Few-Body Systems 17, 5 (1994)

H.Garcilazo, L.Mathelitsch

Three-Pion Resonances

doi: 10.1007/BF01075351
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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
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1993GA04      Phys.Rev. C47, 957 (1993)

H.Garcilazo

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
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1993GA21      Nucl.Phys. A562, 521 (1993)

H.Garcilazo, E.Moya de Guerra

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
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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
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1991GA19      Phys.Rev. C44, 966 (1991)

H.Garcilazo

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
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1991MA01      Phys.Rev. C43, 1038 (1991)

L.Mathelitsch, H.Garcilazo

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
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1990GA14      Phys.Rev.Lett. 65, 293 (1990)

H.Garcilazo

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
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1990GA21      Phys.Rev. C42, 2334 (1990)

H.Garcilazo

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
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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
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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
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1989GA02      Phys.Rev. C39, 717 (1989)

H.Garcilazo, L.Mathelitsch

Pionic Components of the Deuteron Wave Function

NUCLEAR STRUCTURE 2H; calculated wave function pionic components. Three-body model.

doi: 10.1103/PhysRevC.39.717
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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
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1988GA06      Phys.Rev. C37, 2022 (1988)

H.Garcilazo

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
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1988GA15      Phys.Rev.Lett. 61, 1457 (1988)

H.Garcilazo

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
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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
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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
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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
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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
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1987GA06      Phys.Rev. C35, 1804 (1987)

H.Garcilazo

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
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1987GA07      Phys.Rev. C35, 1820 (1987)

H.Garcilazo

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
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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
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1986GA17      Phys.Rev. C34, 1425 (1986)

H.Garcilazo, L.Mathelitsch

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
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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
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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
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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
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1984GA18      Phys.Rev.Lett. 53, 652 (1984)

H.Garcilazo

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
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1983GA08      Phys.Rev. C27, 2405 (1983)

H.Garcilazo

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
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1982GA07      Phys.Rev. C25, 1649 (1982)

H.Garcilazo

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
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1982GA13      Phys.Rev. C25, 2596 (1982)

H.Garcilazo, G.Mercado

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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