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.

1994DI08 Nuovo Cim. 107A, 1293 (1994)

P.Di Giacomo, M.Giannini, D.Prosperi

Pair Currents and Constituent Quark Models

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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1970CE01 Nucl.Phys. A141, 561 (1970)

R.Cesareo, M.Giannini, P.R.Oliva, D.Prosperi, M.C.Ramorino

The ²⁰⁵Tl Level Scheme as Investigated by Nuclear Resonant Scattering of 7646 keV γ-Rays

NUCLEAR REACTIONS ²⁰⁵Tl(γ, γ'), E=7646 keV; measured resonance fluorescence, σ(Eγ', θ). ²⁰⁵Tl deduced levels, J. Natural targets, Ge(Li), NaI(Tl) detectors.

doi: 10.1016/0375-9474(70)90987-5
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1969AQ01 Nuovo Cimento 62B, 20 (1969)

A.Aquili, R.Cesareo, M.Giannini

Gamma-Ray Transitions and Gamma-Gamma Angular Correlations in ¹⁵²Sm

RADIOACTIVITY ¹⁵²Eu; measured Eγ, Iγ, γγ-coin, γγ(θ). ¹⁵²Sm deduced levels, J, π, γ-mixing, γ-multipolarity. Ge(Li) detector.

doi: 10.1007/BF02712462
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1969CE02 Nucl.Phys. A132, 512 (1969)

R.Cesareo, M.Giannini, P.Oliva, D.Prosperi, M.C.Ramorino

Nuclear Resonant Scattering of Gamma Rays in Ni, Cd, Sn and Bi

NUCLEAR REACTIONS ⁶²Ni(γ, γ'), E=7646 keV; ¹¹²Cd(γ, γ'), E=7632 keV; ¹¹⁸Sn(γ, γ'), E=6988 keV; ²⁰⁹Bi(γ, γ'), E=7637 keV; measured resonant fluorescence σ(Eγ', θ). ⁶²Ni, ¹¹²Cd, ¹¹⁸Sn, ²⁰⁹Bi deduced levels, J. Natural targets, Ge(Li), NaI(Tl) detectors.

doi: 10.1016/0375-9474(69)90715-5
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1969FU02 Nuovo Cimento Lett. 1, 467 (1969)

A.Fubini, M.Giannini, D.Prosperi, V.Rado

M1 Transitions Following the Slow-Neutron Capture in ¹¹⁵In

NUCLEAR REACTIONS ¹¹⁵In(n, γ)¹¹⁶In, E= thermal; measured Eγ, Iγ; deduced Q. ¹¹⁶In deduced levels, γ-multipolarity. Ge(Li) detector.

doi: 10.1007/BF02752589
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1967GI15 Nucl.Phys A101, 145 (1967)

M.Giannini, P.Oliva, D.Prosperi, G.Toumbev

Nuclear Resonant Scattering of Gamma Rays in Cu, Sn and Bi

NUCLEAR REACTIONS ^63,65Cu, ¹¹⁷Sn, ²⁰⁸Pb, ²⁰⁹Bi(γ, γ'), E= resonance; measured Eγ, Iγ; ⁶²Ni, ¹¹⁴Cd(γ, γ'), analyzed data. ⁶²Ni, ^63,65Cu, ¹¹⁴Cd, ¹¹⁷Sn, ²⁰⁸Pb, ²⁰⁹Bi levels deduced γ-width.