Nuclear Science References (NSR)

NUCLEAR REACTIONS ¹H(e, π⁰X), E=high; analyzed data; deduced resonance production associated helicity amplitudes, Q² dependence. Unitary isobar model.

doi: 10.1140/epjad/s2004-03-009-9
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2003GI01 Phys.Lett. 552B, 149 (2003)

M.M.Giannini, E.Santopinto, A.Vassallo, M.Vanderhaeghen

Quark model predictions for the SU(6)-breaking ratio of the proton momentum distributions

NUCLEAR STRUCTURE ¹n, ¹H; calculated parton distribution features, relative anomalous magnetic moments. Constituent quark model.

doi: 10.1016/S0370-2693(02)03158-1
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2002GI03 Nucl.Phys. A699, 308c (2002)

M.M.Giannini, E.Santopinto, A.Vassallo

The Hypercentral Constituent Quark Model

doi: 10.1016/S0375-9474(01)01508-1
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2001GI18 Eur.Phys.J. A 12, 447 (2001)

M.M.Giannini, E.Santopinto, A.Vassallo

Hypercentral Constituent Quark Model and Isospin Dependence

doi: 10.1007/s10050-001-8668-y
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2000DE40 Phys.Rev. C62, 025208 (2000)

M.De Sanctis, M.M.Giannini, L.Repetto, E.Santopinto

Proton Form Factors in the Hypercentral Constituent Quark Model

NUCLEAR STRUCTURE ¹H; calculated charge, magnetic form factors.

doi: 10.1103/PhysRevC.62.025208
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2000DR09 Phys.Lett. 484B, 236 (2000)

D.Drechsel, M.Vanderhaeghen, M.M.Giannini, E.Santopinto

Inelastic Photon Scattering and the Magnetic Moment of the Δ (1232) Resonance

NUCLEAR REACTIONS ¹H(γ, γπ⁰), E=286 MeV; calculated σ, σ(E, θ). Constituent quark model, effective Lagrangian procedure.

doi: 10.1016/S0370-2693(00)00654-7
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2000GI03 Nucl.Phys. A666-667, 321c (2000)

M.M.Giannini

Models of the Nucleon

doi: 10.1016/S0375-9474(00)00045-2
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1998AI01 J.Phys.(London) G24, 753 (1998)

M.Aiello, M.M.Giannini, E.Santopinto

Electromagnetic Transition Form Factors of Negative Parity Nucleon Resonances

doi: 10.1088/0954-3899/24/4/007
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1998DE08 Eur.Phys.J. A 1, 187 (1998)

M.De Sanctis, E.Santopinto, M.M.Giannini

A Relativistic Study of the Nucleon Form Factors

NUCLEAR STRUCTURE ¹n, ¹H; calculated charge, magnetic form factors; deduced relativistic effects. Constituent quark models. Comparison with data.

doi: 10.1007/s100500050047
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1998DE45 Eur.Phys.J. A 2, 403 (1998)

M.De Sanctis, E.Santopinto, M.M.Giannini

A Relativistic Study of the Nucleon Helicity Amplitudes

NUCLEAR STRUCTURE ¹n, ¹H; calculated nucleon resonances form factors. Constituent quark model.

doi: 10.1007/s100500050137
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1998SA11 Eur.Phys.J. A 1, 307 (1998)

E.Santopinto, F.Iachello, M.M.Giannini

Nucleon Form Factors in a Simple Three-Body Quark Model

doi: 10.1007/s100500050065
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1997GI04 Int.J.Mod.Phys. E6, 65 (1997)

M.M.Giannini, E.Trovatore

Nucleon Resonances in Nuclei and Quark Levels

doi: 10.1142/S0218301397000044
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1997SA49 Nucl.Phys. A623, 100c (1997)

E.Santopinto, F.Iachello, M.M.Giannini

Exactly Solvable Models of Baryon Spectroscopy

doi: 10.1016/S0375-9474(97)00427-2
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1996AI06 Phys.Lett. 387B, 215 (1996)

M.Aiello, M.Ferraris, M.M.Giannini, M.Pizzo, E.Santopinto

A Three-Body Force Model for the Electromagnetic Excitation of the Nucleon

doi: 10.1016/0370-2693(96)00986-0
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1995MO35 Int.J.Mod.Phys. E4, 607 (1995)

V.I.Mokeev, E.Santopinto, M.M.Giannini, G.Ricco

The Influence of the Nuclear Medium on the Baryon Resonance Excitation

NUCLEAR REACTIONS ¹H(γ, X), E ≈ 0.5-4 GeV; ²H(γ, X), E ≈ 1.05-2 GeV; calculated photoabsorption σ(E). ⁹Be, ¹²C(γ, X), E=0.2-1.6 GeV; calculated per nucleon photoabsorption σ(E); deduced nuclear medium role.

doi: 10.1142/S0218301395000237
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1994AN07 Phys.Rev. C49, 3275 (1994)

V.V.Anisovich, L.G.Dakhno, M.M.Giannini

Color Transparency in the Deuteron

NUCLEAR REACTIONS ²H(e, X), E not given; calculated color transparency factor vs Reid soft core wave function parameter.

doi: 10.1103/PhysRevC.49.3275
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1994AN27 Yad.Fiz. 57, No 6, 1071 (1994); Phys.Atomic Nuclei 57, 1010 (1994)

V.V.Anisovich, L.G.Dakhno, M.M.Giannini

Electrodisintegration of the Deuteron and Color Transparency

NUCLEAR REACTIONS ²H(e, X), E not given; analyzed color transparency factor energy dependence following ²H disintegration. Multiple scattering theory.

1994GI02 Phys.Rev. C49, R1258 (1994)

M.M.Giannini, E.Santopinto

Nucleon Resonances in Nuclei and Quark Exchange

doi: 10.1103/PhysRevC.49.R1258
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1994GI16 Few-Body Systems 17, 21 (1994)

M.M.Giannini, L.Kondratyuk, P.Saracco

Relativistic Light-Cone Approach to Elastic Electron-Deuteron Scattering

NUCLEAR REACTIONS ²H(e, e), E not given; calculated charge, magnetic form factor. Relativistic light cone approach.

NUCLEAR STRUCTURE ²H; calculated structure functions. Relativistic light cone approach.

doi: 10.1007/BF01075352
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1993DR10 Few-Body Systems 15, 99 (1993)

D.Drechsel, M.M.Giannini

The Drell-Hearn-Gerasimov Sum Rule and the Constituent Quark Model

doi: 10.1007/BF01076427
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1991BO29 Nucl.Phys. A533, 441 (1991)

S.Boffi, M.M.Giannini

Distortion in Two-Nucleon Photoemission

NUCLEAR REACTIONS ¹⁶O(γ, np), E=200 MeV; calculated σ(θ₁, θ₂, E₁); deduced distortions role. Final state interactions, factorized approximation.

doi: 10.1016/0375-9474(91)90527-D
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1989BO28 J.Phys.(London) G15, 1605 (1989)

L.Boato, M.M.Giannini

Two-Nucleon Photoemission and Nuclear Correlations

NUCLEAR REACTIONS ¹⁶O(γ, n), (γ, p), (γ, np), (γ, X), E ≈ 40-140 MeV; calculated reaction, total σ(E). Correlations, meson exchange currents.

doi: 10.1088/0954-3899/15/10/010
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1988CO10 Nucl.Phys. A483, 9 (1988)

P.Corvisiero, M.Anghinolfi, M.M.Giannini, G.Ricco, M.Sanzone, M.Taiuti

Proton and Deuteron Radiative Capture in Light Nuclei

NUCLEAR REACTIONS, ICPND ¹⁶O(p, γ), E=30 MeV; ¹⁵N(d, γ), E=16 MeV; measured capture σ, σ(θ); deduced A₀, a₁ coefficients. ¹⁷F, ¹⁷O deduced GDR excitation mechanism. Gas targets, large anticoincidence NaI detector.

doi: 10.1016/0375-9474(88)90062-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0539.

1985AR05 Nucl.Phys. A436, 699 (1985)

H.Arenhovel, M.M.Giannini

Energy-Weighted M1 Sum Rule with Explicit Δ Degrees of Freedom

NUCLEAR STRUCTURE ²H, ⁴He; deduced M1 transition EWSR; deduced isobar degrees of freedom role.

doi: 10.1016/0375-9474(85)90555-X
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1983BE08 Phys.Lett. 122B, 1 (1983)

M.Beyer, D.Drechsel, M.M.Giannini

The Pair Current in the Constituent Quark Model

NUCLEAR STRUCTURE ³He, ³H; calculated charge form factors. Quark model, relativistic pair current.

doi: 10.1016/0370-2693(83)91156-5
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1983CI13 Nuovo Cim. 76A, 225 (1983)

C.Ciofi Degli Atti, M.M.Giannini, G.Salme

Antisymmetry and Orthogonality Effects in Single-Particle Models of (γ, p) Reactions

NUCLEAR REACTIONS ¹⁶O(γ, p), E=50-200 MeV; calculated σ(θ) vs E. Single particle model, antisymmetry, orthogonality effects.

1983GI11 Nuovo Cim. 76A, 455 (1983)

M.M.Giannini

Electromagnetic Form Factors and Quark Model

NUCLEAR STRUCTURE ¹H, ¹n, ³He; calculated charge form factors. Quark model.

doi: 10.1007/BF02833741
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1982DR01 Phys.Lett. 108B, 159 (1982)

D.Drechsel, L.Tiator, M.Beyer, M.M.Giannini

Nucleon Polarization and the Nuclear Charge Operator

NUCLEAR STRUCTURE ³He; calculated charge form factor. Impulse approximation, two-body contributions.

doi: 10.1016/0370-2693(82)91165-0
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1981HA07 Nucl.Phys. A352, 413 (1981)

Ch.Hajduk, P.U.Sauer, H.Arenhovel, D.Drechsel, M.M.Giannini

On the Contribution of the Δ -Isobar to the Charge Form Factor of ³He

NUCLEAR STRUCTURE ³He; calculated charge form factor. Faddeev equations, Δ-isobar.

doi: 10.1016/0375-9474(81)90420-6
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1979GI08 Phys.Lett. 88B, 13 (1979)

M.M.Giannini, D.Drechsel, H.Arenhovel, V.Tornow

The Charge Form Factor of Three-Nucleon Systems and the Polarization of the Bound Nucleon

NUCLEAR STRUCTURE ³H, ³He; calculated charge form factor. Impulse approximation, diagonal, nondiagonal isobar contributions, meson exchange effects.

doi: 10.1016/0370-2693(79)90102-3
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1978CE01 Nuovo Cim. 43A, 513 (1978)

R.Cenni, G.Dillon, M.M.Giannini

On the Δ-Resonance in the Two-Nucleon System

NUCLEAR REACTIONS ^1,2H(π⁺, X), E ≤ 240 MeV; calculated σ(E).

doi: 10.1007/BF02730446
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