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NSR database version of April 11, 2024.

Search: Author = B.Julia-Diaz

Found 32 matches.

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2023PE17      Eur.Phys.J. A 59, 240 (2023)

A.Perez-Obiol, S.Masot-Llima, A.M.Romero, J.Menendez, A.Rios, A.Garcia-Saez, B.Julia-Diaz

Quantum entanglement patterns in the structure of atomic nuclei within the nuclear shell model

NUCLEAR STRUCTURE ^8,10,12Be, ^{18,20,22,24,26}O, ^{20,22,24,26,28}Ne, ^{42,44,46,48,50}Ca; analyzed available data; deduced single-orbital entropies, mutual information, Von Neumann entanglement entropies for the proton–neutron and opposite partitions.

doi: 10.1140/epja/s10050-023-01151-z
Citations: PlumX Metrics

2016PE12      Nucl.Phys. A954, 213 (2016)

A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno

Next-to-leading order effective field theory ΛN → NN potential in coordinate space

doi: 10.1016/j.nuclphysa.2016.04.039
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2013PE05      Phys.Rev. C 87, 044614 (2013)

A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno

One-loop contributions in the effective field theory for the ΛN → NN transition

doi: 10.1103/PhysRevC.87.044614
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2013PE17      Nucl.Phys. A914, 199c (2013)

A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno

Higher order contributions to the weak ΛN → NN interaction in effective field theory

doi: 10.1016/j.nuclphysa.2013.12.122
Citations: PlumX Metrics

2011PE19      Phys.Rev. C 84, 024606 (2011)

A.Perez-Obiol, A.Parreno, B.Julia-Diaz

Constraints on effective field theory parameters for the ΛN → N N transition

doi: 10.1103/PhysRevC.84.024606
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2010SU01      Phys.Rev.Lett. 104, 042302 (2010)

N.Suzuki, B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato

Disentangling the Dynamical Origin of P₁₁ Nucleon Resonances

doi: 10.1103/PhysRevLett.104.042302
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2009JU04      Phys.Rev. C 80, 025207 (2009)

B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato, N.Suzuki

Dynamical coupled-channels analysis of ¹H(e, e'π)N reactions

doi: 10.1103/PhysRevC.80.025207
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2009KA08      Phys.Rev. C 79, 025206 (2009)

H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato

Dynamical coupled-channels study of πN → ππN reactions

doi: 10.1103/PhysRevC.79.025206
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2009KA39      Phys.Rev. C 80, 065203 (2009)

H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato

Double and single pion photoproduction within a dynamical coupled-channels model

doi: 10.1103/PhysRevC.80.065203
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2008DU17      Phys.Rev. C 78, 025204 (2008)

J.Durand, B.Julia-Diaz, T.-S.H.Lee, B.Saghai, T.Sato

Coupled-channels study of the π^- p → ηn process

doi: 10.1103/PhysRevC.78.025204
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2008JU04      Phys.Rev. C 77, 045205 (2008)

B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato, L.C.Smith

Dynamical coupled-channels effects on pion photoproduction

NUCLEAR REACTIONS p(γ, p)π⁰, E=1154-1632 MeV; calculated cross sections, angular distributions using dynamical coupled-channel model. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.045205
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2007JU01      Phys.Rev. C 75, 015205 (2007)

B.Julia-Diaz, T.-S.H.Lee, T.Sato, L.C.Smith

Extraction and interpretation of γN → Δ form factors within a dynamical model

NUCLEAR REACTIONS ¹H(e, e'π⁰), E=high; analyzed σ(θ), related data; deduced form factors.

doi: 10.1103/PhysRevC.75.015205
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2007JU07      Phys.Rev. C 76, 065201 (2007)

B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato

Dynamical coupled-channels model of πN scattering in the W ≤ 2 GeV nucleon resonance region

NUCLEAR REACTIONS p(π^-, π^-), (π^-, π⁰), E<2 GeV; analyzed pion-nucleon scattering using dynamical coupled-channel model.

doi: 10.1103/PhysRevC.76.065201
Citations: PlumX Metrics

2007SA19      Eur.Phys.J. A 31, 512 (2007)

B.Saghai, J.-C.David, B.Julia-Diaz, T.-S.H.Lee

Search for missing baryon resonances via associated strangeness photoproduction

NUCLEAR REACTIONS ¹H(γ, K⁺X), E ≈ 1.1, 1.3 GeV; analyzed hyperon production σ(θ), polarization observables.

doi: 10.1140/epja/i2006-10226-2
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2006JU02      Phys.Rev. C 73, 055204 (2006)

B.Julia-Diaz, B.Saghai, T.-S.H.Lee, F.Tabakin

Dynamical coupled-channels approach to hadronic and electromagnetic kaon-hyperon production on the proton

NUCLEAR REACTIONS ¹H(π^-, K⁰X), (γ, K⁺X), E(cm) ≈ 1.6-2.3 GeV; calculated hyperon production associated σ(θ), recoil polarization asymmetry, excitation functions. Dynamical coupled-channels approach, comparison with data.

doi: 10.1103/PhysRevC.73.055204
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2006JU04      Nucl.Phys. A780, 175 (2006)

B.Julia-Diaz, D.O.Riska

The role of qqqq(q-bar) components in the nucleon and the N(1440) resonance

doi: 10.1016/j.nuclphysa.2006.09.016
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2005FR05      Nucl.Phys. A750, 337 (2005)

F.Fromel, B.Julia-Diaz, D.O.Riska

Bound states of heavy flavor hyperons

doi: 10.1016/j.nuclphysa.2005.01.022
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2005HE17      Eur.Phys.J. A 24, 411 (2005)

J.He, B.Julia-Diaz, Y.Dong

Electroweak properties of the π, K and K^* (892) in the three forms of relativistic kinematics

doi: 10.1140/epja/i2005-10013-7
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2005JU07      Nucl.Phys. A755, 431c (2005)

B.Julia-Diaz, D.O.Riska

Nuclei of Double-Charm Hyperons

doi: 10.1016/j.nuclphysa.2005.03.050
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2005JU08      Nucl.Phys. A755, 463c (2005)

B.Julia-Diaz, B.Saghai, F.Tabakin, W.-T.Chiang, T.-S.H.Lee, Z.Li

Dynamical coupled-channel study of K⁺Λ photoproduction

NUCLEAR REACTIONS ¹H(γ, K⁺X), E(cm) ≈ 1.6-2.3 GeV; calculated hyperon production σ(θ), excitation functions. Constituent quark model, coupled-channels approach, comparison with data.

doi: 10.1016/j.nuclphysa.2005.03.056
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2005JU10      Nucl.Phys. A757, 441 (2005)

B.Julia-Diaz, D.O.Riska

D-state configurations in the electromagnetic form factors of the nucleon and the Δ(1232) resonance

NUCLEAR STRUCTURE ¹n, ¹H; calculated electromagnetic form factors, Δ-N form factors, effect of D-state admixtures.

doi: 10.1016/j.nuclphysa.2005.04.008
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2004JU01      Eur.Phys.J. A 19, Supplement 1, 99 (2004)

B.Julia-Diaz, A.Valcarce, P.Gonzalez, F.Fernandez

A microscopic NN → NN^*(1440) potential

doi: 10.1140/epjad/s2004-03-017-9
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2004JU02      Phys.Rev. C 69, 035212 (2004); Erratum Phys.Rev. C 75, 069902 (2007)

B.Julia-Diaz, D.O.Riska, F.Coester

Baryon form factors of relativistic constituent-quark models

NUCLEAR STRUCTURE ¹n, ¹H; calculated electromagnetic and axial form factors. Constituent-quark models.

2004JU04      Nucl.Phys. A739, 69 (2004)

B.Julia-Diaz, D.O.Riska

Baryon magnetic moments in relativistic quark models

doi: 10.1016/j.nuclphysa.2004.03.078
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2004JU07      Phys.Rev. C 70, 045204 (2004)

B.Julia-Diaz, D.O.Riska, F.Coester

Axial transition form factors and pion decay of baryon resonances

doi: 10.1103/PhysRevC.70.045204
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2004JU09      Fizika(Zagreb) B 13, 347 (2004)

B.Julia-Diaz, A.Valcarce, F.Fernandez

The p(d, d') reaction and the σNN^*(1440) coupling constant

NUCLEAR REACTIONS ¹H(d, d'), E=2.3 GeV; calculated σ(E, θ), Roper resonance contribution.

2003JU05      Mod.Phys.Lett. A 18, 200 (2003)

B.Julia-Diaz, T.-S.H.Lee

Quark-exchange mechanism of γd → np reaction at 2-6 GeV

NUCLEAR REACTIONS ²H(γ, n), E=2-6 GeV; calculated σ(θ), role of quark-exchange mechanism.

doi: 10.1142/S0217732303010247
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2002JU02      Phys.Rev. C65, 034001 (2002)

B.Julia-Diaz, J.Haidenbauer, A.Valcarce, F.Fernandez

Quark-Model Based Study of the Triton Binding Energy

NUCLEAR STRUCTURE ³H; calculated binding energy. Quark model, nonlocal NN potential, five-channel Fadeev calculation.

doi: 10.1103/PhysRevC.65.034001
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2002JU09      Phys.Rev. C66, 024005 (2002)

B.Julia-Diaz, A.Valcarce, P.Gonzalez, F.Fernandez

Microscopic NN →NN*(1440) transition potential: Determination of πNN*(1440) and σNN*(1440) coupling constants

doi: 10.1103/PhysRevC.66.024005
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2002JU11      Phys.Rev. C66, 047002 (2002)

B.Julia-Diaz, D.R.Entem, A.Valcarce, F.Fernandez

Deuteron NN^*(1440) components from a chiral quark model

NUCLEAR STRUCTURE ²H; calculated resonance components. Chiral quark model.

doi: 10.1103/PhysRevC.66.047002
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2001JU01      Phys.Rev. C63, 024006 (2001)

B.Julia-Diaz, F.Fernandez, P.Gonzalez, A.Valcarce

Microscopic Derivation of the NN^*(1440) Potential

doi: 10.1103/PhysRevC.63.024006
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2001JU11      Nucl.Phys. A689, 331c (2001)

B.Julia, F.Fernandez, A.Valcarce, P.Gonzalez

Quark-Model Description of the NN^*(1440) Potential

doi: 10.1016/S0375-9474(01)00848-X
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