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Search: Author = A.Scalia

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1997SC19      Nucl.Phys. A621, 335c (1997)

A.Scalia, N.Arena, Seb.Cavallaro, R.Giordano

Fusion Process and Elastic Scattering at Low Energy for the p + ¹²C System

NUCLEAR REACTIONS ¹²C(p, X), E < 0.4 MeV; analyzed σ, astrophysical S-factor. Shadow model.

doi: 10.1016/S0375-9474(97)00267-4
Citations: PlumX Metrics

1994SC14      Phys.Rev. C49, 2847 (1994)

A.Scalia

Reply to ' Comment on ' Shadow Model for Sub-Barrier Fusion Applied to Light System ' '

NUCLEAR REACTIONS ³He(³He, 2p), E(cm) ≤ 350 keV; ⁷Be(p, γ), ³He(α, γ), E < 1.3 MeV; compiled, reviewed data analyses; deduced shadow model based analysis validity.

doi: 10.1103/PhysRevC.49.2847
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1993SC06      Phys.Rev. C47, 1247 (1993)

A.Scalia

' Shadow ' Properties in Sub-Barrier Fusion

NUCLEAR REACTIONS ²H(p, γ), (d, p), ³He(d, p), (³He, 2p), ⁷Li(p, α), E not given; analyzed fusion σ; deduced effective Coulomb potential role in anomalous behavior.

doi: 10.1103/PhysRevC.47.1247
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1992SC07      Nuovo Cim. 105A, 233 (1992)

A.Scalia

The < Shadow > Model for the Sub-Barrier Fusion

NUCLEAR STRUCTURE A=26-194; analyzed production σ by fusion reactions. Several reactions studied, shadow model for fusion.

doi: 10.1007/BF02826031
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1992SC22      Phys.Rev. C46, 2610 (1992)

A.Scalia, P.Figuera

' Shadow ' Model for Sub-Barrier Fusion Applied to Light Systems: Determination of the reaction rate

NUCLEAR REACTIONS, ICPND ²H(p, γ), E(cm) ≤ 1.25; ²H(d, p), (d, n), E(cm) ≤ 0.15 MeV; ³He(d, p), E(cm) ≤ 0.175 MeV; ⁷Li(p, α), E(cm) ≤ 0.9 MeV; ³He(³He, 2p), E(cm) ≤ 1.25 MeV; ⁷Be(p, γ), E(cm) ≤ 1.3 MeV; calculated fusion σ(E); deduced reaction rates, cross section factor. Shadow model, sub-barrier fusion.

doi: 10.1103/PhysRevC.46.2610
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1991SC12      Nuovo Cim. 104A, 563 (1991)

A.Scalia

The Extended Elastic Model III: The nuclear fusion for the reaction ⁷Li(p, α)⁴He

NUCLEAR REACTIONS, ICPND ²H(p, γ), E(cm) < 1.2 MeV; ²H(d, p), (d, n), E(cm) ≤ 160 keV; ³He(d, p), E(cm) ≤ 160 keV; ⁷Li(p, α), ³He(³He, 2p), E(cm) ≤ 1 MeV; analyzed σ(E). Extended elastic model.

doi: 10.1007/BF02813592
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1991SC23      Nuovo Cim. 104A, 691 (1991)

A.Scalia

A Simple Expression for the Cross-Section Factor in Nuclear Fusion

NUCLEAR REACTIONS ²H(p, γ), (d, p), (d, n), (α, γ), ³H(d, n), ³He(d, t), (³He, 2p), ³H(α, γ), E=sub-barrier; calculated fusion σ factor. Extended elastic model.

doi: 10.1007/BF02821777
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1991SC24      Nuovo Cim. 104A, 707 (1991)

A.Scalia

An Effective Coulomb Potential Obtained by Using the Extended Elastic Model III for the Sub-Barrier Fusion

NUCLEAR REACTIONS ²H(p, γ), (d, p), (d, n), ³He(³He, 2p), ⁷Li(p, α), E=sub-barrier; calculated σ(θ) maximum energy dependence. Extended elastic model.

doi: 10.1007/BF02821779
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1991SC25      Nuovo Cim. 104A, 713 (1991)

A.Scalia

An Effective Strong-Interaction Distance Obtained in the Framework of the Extended Elastic Model III for Sub-Barrier Fusion

NUCLEAR REACTIONS ²H(p, γ), (d, p), (d, n), ³He(³He, 2p), ⁷Li(p, α), E=sub-barrier; calculated fusion σ(E); deduced effective strong interaction range. Extended elastic model.

doi: 10.1007/BF02821780
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1991SC32      Nuovo Cim. 104A, 1441 (1991)

A.Scalia

Interaction Time for Sub-Barrier Fusion

NUCLEAR REACTIONS ²H(p, γ), E(cm) ≤ 1 MeV; ²H(d, p), (d, n), E(cm) < 200 keV; ³He(³He, 2p), E(cm) ≤ 1 MeV; ⁷Li(p, α), E(cm) ≤ 600 keV; calculated fusion interaction time interval vs E. Extended elastic model.

doi: 10.1007/BF02817426
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1990GI04      Nuovo Cim. 103A, 47 (1990)

R.Giordano, S.Sambataro, A.Scalia, F.Porto, P.Figuera, S.Pirrone

A New Approach to Heavy-Ion Fusion II. Systematic Comparison with Experimental Data

NUCLEAR REACTIONS, ICPND ^13,12C, ¹⁴N, ¹⁸O, ¹⁹F, ^24,26Mg, ²⁷Al, ^29,30,28Si, ³²S(¹²C, X), ¹⁶O, ²⁶Mg, ^28,29,30Si, ⁴⁰Ca(¹⁶O, X), ²⁴Mg, ²⁷Al, ²⁸Si(¹⁸O, X), ²⁷Al, ^28,30Si, ⁴⁰Ca(¹⁹F, X), ²⁶Mg, ²⁷Al(²⁰Ne, X), ^26,24Mg, ³²S(²⁴Mg, X), ^28,29,30Si, ²⁷Al(²⁸Si, X), ²⁴Mg, ²⁷Al, ³⁰Si, ⁴⁰Ca(³²S, X), ⁴⁸Ti, ⁵⁶Fe, ⁶²Ni, ⁹⁰Zr, ^116,120,124Sn(³⁵Cl, X), ^58,62Ni(⁴⁰Ca, X), ¹⁶⁵Ho, ¹⁹⁷Au(⁴⁰Ar, X), E not given; calculated fusion σ(E). Phenomenological approach.

doi: 10.1007/BF02902619
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1990SC15      Nuovo Cim. 103A, 85 (1990)

A.Scalia

The Extended Elastic Model Applied to the Reaction ³He(³He, 2p)⁴He

NUCLEAR REACTIONS, ICPND ³He(³He, 2p), E(cm) ≤ 1 MeV; calculated fusion σ(E), cross section factor vs temperature. Extended elastic model.

doi: 10.1007/BF02902621
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1990SC16      Nuovo Cim. 103A, 213 (1990)

A.Scalia

The Extended Elastic Model Applied to the Reaction ³He(α, γ)⁷Be

NUCLEAR REACTIONS, ICPND ³He(α, γ), E ≈ 1.3 MeV; calculated σ(E), cross section factor vs temperature. Extended elastic model.

doi: 10.1007/BF02820594
Citations: PlumX Metrics

1990SC17      Nuovo Cim. 103A, 255 (1990)

A.Scalia

The Nuclear Fusion for the Reaction ³He(d, p)⁴He

NUCLEAR REACTIONS, ICPND ³He(d, p), E(cm) ≤ 180 keV; calculated σ(E), cross section factor vs temperature. Extended elastic model.

doi: 10.1007/BF02820597
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1990SC18      Nuovo Cim. 103A, 269 (1990)

A.Scalia, R.Giordano, S.Sambataro, F.Porto, P.Figuera, S.Pirrone

A New Approach to Heavy-Ion Fusion III. An Extension to Systems with Large Mass Asymmetry

NUCLEAR REACTIONS, ICPND ⁴⁰Ca, ¹⁸¹Ta(¹⁹F, X), (²⁴Mg, X), ⁴⁰Ca, ¹⁷⁴Yb(¹⁶O, X), ¹⁶⁰Gd(¹²C, X), ¹⁴¹Pr, ^116,124Sn(³⁵Cl, X), ²⁷Al(³²S, X), (²⁰Ne, X), ¹⁶⁵Ho(⁴⁰Ar, X), E not given; calculated fusion σ(E). Elastic model.

doi: 10.1007/BF02820599
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1990SC22      Nuovo Cim. 103A, 927 (1990)

A.Scalia

The Extended Elastic Model II Applied to the Reaction ²H(α, γ)⁶Li

NUCLEAR REACTIONS, ICPND ²H(α, γ), E(cm) ≈ 0.5-4 MeV; calculated fusion σ(E). Extended elastic model.

doi: 10.1007/BF02799236
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1990SC26      Nuovo Cim. 103A, 1177 (1990)

A.Scalia

The Nuclear Fusion for the Reaction ³He(α, γ)⁷Be

NUCLEAR REACTIONS, ICPND ³He(α, γ), E(cm) ≈ 100-1400 keV; calculated σ(E). Modified extended elastic model.

doi: 10.1007/BF02820546
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1989SC18      Nuovo Cim. 101A, 781 (1989)

A.Scalia

A New Approach to Heavy-Ion Fusion. - I.

NUCLEAR REACTIONS ¹²C(¹⁸O, X), ²⁶Mg(¹⁶O, X), ²⁷Al(¹²C, X), (³⁵Cl, X), ²⁴Mg, ⁷⁶Ge(³²S, X), ¹⁰⁹Ag, ¹⁶⁵Ho(⁴⁰Ar, X), E not given; calculated critical fusion radius vs (E/(A₁+A₂)).

doi: 10.1007/BF02844869
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1989SC19      Nuovo Cim. 101A, 795 (1989)

A.Scalia

The Nuclear Fusion for the Reactions ²H(d, n)³He, ²H(d, p)³H, ³H(d, n)⁴He

NUCLEAR REACTIONS, ICPND ²H(d, n), (d, p), E ≤ 225 keV; ³H(d, n), E ≈ 10-70 keV; calculated fusion σ(E), reaction rate. Subbarrier fusion, elastic model.

doi: 10.1007/BF02844871
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1989SC25      Nuovo Cim. 102A, 953 (1989)

A.Scalia

The Reaction Rate at T ≈ 300 K for the Reactions ²H(p, γ)³He, ²H(d, p)³H, ²H(d, n)³He, ³H(d, n)⁴He, ³He(d, p)⁴He, ²H(α, γ)⁶Li, ³He(³He, 2p), ³He(α, γ)⁷Be

NUCLEAR REACTIONS ²H(p, γ), (d, p), (d, n), ³H(d, n), (d, p), ²H(α, γ), ³He(³He, 2p), ³He(α, γ), E=low; calculated reaction rate.

doi: 10.1007/BF02730762
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1989SC36      Nuovo Cim. 102A, 1105 (1989)

A.Scalia

The Nuclear Fusion for the Reactions ²H(d, n)³He, ²H(d, p)³H at Low Energy

NUCLEAR REACTIONS, ICPND ²H(d, n), (d, p), E=low; calculated cross section factor. ²H(d, X), E ≈ 10-225 keV; calculated fusion σ(E). Subbarrier fusion elastic model.

1989SC41      Nuovo Cim. 102A, 1101 (1989)

A.Scalia

The Nuclear Fusion for the Reaction ³H(d, n)⁴He at Very Low Energy

1988SC18      Nuovo Cim. 100A, 559 (1988); Erratum Nuovo Cim. 101A, 355 (1989)

A.Scalia

The Reaction Rate in Nuclear Fusion

NUCLEAR REACTIONS ¹⁵²Sm, ²⁰Ne, ¹²C, ¹⁶O(¹²C, X), ^150,148Nd, ^{148,150,154,152}Sm, ¹⁶O(¹⁶O, X), ⁴⁴Ca(¹⁸O, X), (⁴⁰Ca, X), ^58,62Ni, ²⁷Al(³⁵Cl, X), ⁵⁸Ni(⁵⁸Ni, X), ^{92,94,96,98,100}Mo, ^104,100,102Ru, ¹⁰³Rh, ^{104,105,106,108,110}Pd(³²S, X), ^92,94,96,98Mo, ^{101,100,102,104}Ru, ^{104,105,106,108,110}Pd(³⁶S, X), ¹⁶²Dy(α, X), ¹⁵⁹Tb(⁷Li, X), ^144,148,154Sm(⁴⁰Ar, X), E not given; calculated fusion reaction rate.

doi: 10.1007/BF02789499
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1987SC33      Nuovo Cim. 98A, 571 (1987)

A.Scalia

Subbarrier Fusion with the Elastic Model

NUCLEAR REACTIONS, ICPND ^92,94,100Mo, ^100,103,104Ru, ^{104,105,106,108}Pd(³²S, X), ^94,96,98Mo, ^{100,101,102,104}Ru, ¹⁰³Rh, ^{104,105,106,108,110}Pd(³⁶S, X), E(cm) ≈ 76-92 MeV; ^92,98,96Mo(³²S, X), ¹⁰⁰Mo(³⁶S, X), E(cm) ≈ 74-90 MeV; ¹⁰⁰Mo(³²S, X), E(cm) ≈ 72-88 MeV; ¹⁰¹Ru(³²S, X), E(cm) ≈ 80-92 MeV; ¹⁰⁸Pd(³²S, X), E(cm) ≈ 78-94 MeV; ¹⁴⁸Sm(⁴⁰Ar, X), E(cm) ≈ 114-146 MeV; ¹⁵⁴Sm(⁴⁰Ar, X), E(cm) ≈ 112-144 MeV; ^{150,152,154,148}Sm(¹⁶O, X), E(cm) ≈ 52-68 MeV; ¹⁴⁴Sm(⁴⁰Ar, X), E(cm) ≈ 120-140 MeV; ²⁷Al(³⁵Cl, X), E(cm) ≈ 30-70 MeV; ⁶²Ni(³⁵Cl, X), E(cm) ≈ 58-110 MeV; ¹⁴⁸Nd(¹⁸O, X), E(cm) ≈ 54-70 MeV; ^148,150Nd(¹⁶O, X), E(cm) ≈ 56-72 MeV; ¹⁵⁰Nd(¹⁶O, X), E(cm) ≈ 14-26 MeV; ¹⁵⁹Tb(⁷Li, X), ⁴⁴Ca(¹⁸O, X), E(cm) ≈ 18-30 MeV; ¹⁵²Sm(¹²C, X), E(cm) ≈ 42-58 MeV; ⁵⁸Ni(³⁵Cl, X), E(cm) ≈ 60-92 MeV; ⁴⁴Ca(⁴⁰Ca, X), E(cm) ≈ 48-54 MeV; ⁵⁸Ni(⁵⁸Ni, X), E(cm) ≈ 92-108 MeV; ¹²C(¹²C, X), E(cm) ≈ 3-5 MeV; ¹⁶O(¹²C, X), E(cm) ≈ 5-13 MeV; ²⁰Ne(¹²C, X), E(cm) ≈ 8-15 MeV; ¹⁶O(¹⁶O, X), E(cm) ≈ 7-12 MeV; calculated fusion σ(E).

doi: 10.1007/BF02902014
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1987SC34      Nuovo Cim. 98A, 589 (1987)

A.Scalia

An Energy-Dependent Nucleus-Nucleus Potential from the Elastic Model

NUCLEAR REACTIONS ¹²C, ²⁰Ne(¹²C, ¹²C), ¹²C, ¹⁶O(¹⁶O, ¹⁶O), ⁴⁴Ca(¹⁸O, ¹⁸O), ²⁷Al, ^58,62Ni(³⁵Cl, ³⁵Cl), ⁵⁸Ni(⁵⁸Ni, ⁵⁸Ni), ^{92,96,98,94,100}Mo, ^100,101,102Ru, ¹⁰³Rh, ¹⁰⁴Pd(³²S, ³²S), ^94,96,98Mo, ¹⁰⁰Ru(³⁶S, ³⁶S), ^144,148,154Sm(⁴⁰Ar, ⁴⁰Ar), E not given; calculated nucleus-nucleus potential, parameter energy dependence.

doi: 10.1007/BF02902015
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1986SC32      Nuovo Cim. 94A, 88 (1986)

A.Scalia

The Heavy-Ion Fusion in Terms of the Rutherford Trajectories

NUCLEAR REACTIONS, ICPND ¹²C, ²⁴Mg(¹⁸O, X), ^24,26Mg(¹⁶O, X), ²⁴Mg, ²⁷Al(¹²C, X), ²⁷Al, ⁶²Ni(³⁵Cl, X), ⁷⁶Ge(³²S, X), ¹⁰⁹Ag, ¹⁶⁵Ho(⁴⁰Ar, X), E ≤ 350 MeV; calculated fusion σ(E). Elastic model, closest distance approach.

doi: 10.1007/BF02894808
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1984SC15      Lett.Nuovo Cim. 39, 383 (1984)

A.Scalia

Entrance Channel Effects in Heavy-Ion Reactions

NUCLEAR REACTIONS ¹⁹⁷Au(²⁰Ne, X), E(cm)=136.17-363.13 MeV; ¹⁰⁹Ag(⁴⁰Ar, X), E(cm)=123.63-246.53 MeV; ¹⁶⁵Ho(⁵⁶Fe, X), E(cm)=345 MeV; ²⁷Al(¹⁶O, X), E(cm)=54.62-101.09 MeV; ⁴⁰Ca(⁴⁰Ar, X), E(cm)=80.52-136.05 MeV; ¹³C(¹⁴N, X), E(cm)=41.4-86.7 MeV; ²⁶Mg(¹²C, X), E(cm)=13.3-40 MeV; ²⁶Mg(¹²C, X), E(cm)=13.3-40 MeV; ⁷⁶Ge(³²S, X), E(cm)=111.18-158.33 MeV; ¹⁰B(¹⁴N, X), E(cm)=35.83-73.51 MeV; calculated reaction σ; deduced entrance channel effects. One-dimensional model.

doi: 10.1007/BF02787253
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1984SC24      Lett.Nuovo Cim. 40, 33 (1984)

A.Scalia

Some Remarks on the Generalized Critical-Distance Model for Heavy-Ion Fusion

NUCLEAR REACTIONS, ICPND ¹⁶⁵Ho(⁴⁰Ar, X), E(cm)=144.87-314.7 MeV; ¹⁸¹Ta(²⁴Mg, X), E(cm)=238.39-300.19 MeV; ¹⁹⁷Au(³⁵Cl, X), E(cm)=174-270 MeV; ⁶²Ni(³⁵Cl, X), E(cm)=102.26-137.42 MeV; ¹¹⁶Sn(³⁵Cl, X), E(cm)=122.91-165.16 MeV; ¹⁴¹Pr(³⁵Cl, X), E(cm)=124.17-172.24 MeV; ¹⁰⁹Ag(⁴⁰Ar, X), E(cm)=123.63-246.53 MeV; ²⁴Mg(¹²C, X), E(cm)=13.33-40 MeV; Sb(⁴⁰Ar, X), E(cm)=125.76-222.91 MeV; ⁷⁶Ge(³²S, X), E(cm)=76-158.33 MeV; calculated fusion σ. Generalized critical distance model.

doi: 10.1007/BF02817807
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1984SC28      Lett.Nuovo Cim. 40, 205 (1984)

A.Scalia

Elastic Scattering and Fusion Process in Heavy-Ion Reactions

NUCLEAR REACTIONS ⁴⁰Ca(³²S, ³²S), E(cm)=55.55 MeV; ²⁷Al(³²S, ³²S), E(cm)=66.4, 73.22 MeV; ⁴⁸Ti(³²S, ³²S), E(cm)=96 MeV; ⁷⁶Ge(³²S, ³²S), E(cm)=158.3 MeV; ²⁴Mg(¹⁵O, ¹⁵O), E(cm)=24 MeV; calculated σ(elastic)/σ(Rutherford). Generalized critical distance, heavy ion fusion model.

doi: 10.1007/BF02719536
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1984SC36      Lett.Nuovo Cim. 40, 523 (1984)

A.Scalia

Determination of the Nucleus-Nucleus Potential from the Generalized Critical-Distance Model

NUCLEAR REACTIONS ^112,120Sn(³⁵Cl, X), ¹⁴¹Pr(³⁵Cl, X), ¹⁶⁵Ho, ¹²³Sb, ¹⁰⁹Ag(⁴⁰Ar, X), E not given; calculated nucleus-nucleus potential vs critical distance, entrance channel parameters.

doi: 10.1007/BF02749384
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1984SC40      Lett.Nuovo Cim. 41, 237 (1984)

A.Scalia

Calculation of the Real Part of the Interaction Potential between Two Heavy Ions from the Generalized Critical-Distance Model

NUCLEAR REACTIONS ¹⁶⁵Ho, ¹²³Sb, ¹⁰⁹Ag(⁴⁰Ar, X), ^112,120Sn, ¹⁴¹Pr, ⁹⁰Zr, ²⁷Al, ⁵⁶Fe(³⁵Cl, X), ¹²C, ⁷⁶Ge, ³²S(²⁴Mg, X), ²⁴Mg(³²S, X), E not given; calculated ion-ion potential parameters. Asymmetric dynamical system.

doi: 10.1007/BF02747010
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1983GI03      Lett.Nuovo Cim. 36, 125 (1983)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

Heavy-Ion Fusion and Its Connections with Elastic Scattering

NUCLEAR REACTIONS ⁴⁸Ti(³²S, ³²S), E=160 MeV; ²⁸Si(³²S, ³²S), E=97 MeV; analyzed σ(θ); deduced fusion, Coulomb scattering relation.

doi: 10.1007/BF02749655
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1983GI12      Nuovo Cim. 77A, 135 (1983)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

Elastic, Fusion and Total Reaction Cross-Sections for the ¹²C + ³²S System at E(³²S) = 160 MeV

NUCLEAR REACTIONS ¹²C(³²S, ³²S), (³²S, X), E=160 MeV; measured σ(E(³²S)), σ(θ), total reaction σ, σ(fragment θ) vs Z, σ(fragment) vs mass, fusion σ; deduced reaction mechanisms. Modified sum of differences method.

1983SC26      Lett.Nuovo Cim. 37, 129 (1983)

A.Scalia

Heavy-Ion Elastic Scattering and Its Connections with Fusion and Absorption Processes

NUCLEAR REACTIONS ²⁷Al(³²S, ³²S), E=145, 160 MeV; ⁴⁸Ti(³²S, ³²S), E=160 MeV; calculated s(θ) elastic to Rutherford scattering ratio; deduced σ(fusion), total σ(reaction).

doi: 10.1007/BF02817912
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1982CO23      Nuovo Cim. 71A, 381 (1982)

S.Costa, R.Giordano, F.Porto, S.Sambataro, A.Scalia, L.Zuffi

Analysis of α Scattering from ²⁵Mg at 12.5 MeV in Terms of the Coupled-Channel Calculation

NUCLEAR REACTIONS ²⁵Mg(α, α), (α, α'), E=12.1-12.9 MeV; measured σ(Eα'), σ(θ); deduced direct contribution, optical model parameters. ²⁵Mg deduced β₂, ground state quadrupole moment, rms radius. Statistical, deformed optical model analyses.

doi: 10.1007/BF02898933
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1982CO24      Nuovo Cim. 72A, 40 (1982)

S.Costa, R.Giordano, F.Porto, S.Sambataro, A.Scalia

The Modified SOD Method Related to a Simple Model of the Scattering Process

NUCLEAR REACTIONS ^63,65Cu(α, α), E=13, 14 MeV; measured σ(θ); deduced σ(reaction). Modified sum of differences method.

doi: 10.1007/BF02784791
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1982GI09      Lett.Nuovo Cim. 35, 33 (1982); Erratum Lett.Nuovo Cim. 36, 512 (1983)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

Fusion Cross-Section from Modified SOD Method

NUCLEAR REACTIONS, ICPND ²⁸Si, ^26,24Mg(¹⁶O, X), ²⁴Mg(¹⁸O, X), ^28,30Si, ¹²C, ²⁷Al(¹⁹F, X), ²⁷Al, ⁴⁰Ca(³²S, X), ⁶²Ni, ⁴⁸Ti(³⁵Cl, X), E(cm) ≈ 50-200 MeV; calculated fusion σ vs E. Phenomenological approach.

doi: 10.1007/BF02755012
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1982GI13      Lett.Nuovo Cim. 35, 161 (1982)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

Reaction and Fusion Cross-Sections for Identical Heavy Ions

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, X), E(cm)=7-31 MeV; ¹⁶O(¹⁶O, X), E=27-66 MeV; ²⁴Mg(²⁴Mg, X), E(cm)=24.7-66.2 MeV; ²⁸Si(²⁸Si, X), E=80-140 MeV; ⁴⁰Ca(⁴⁰Ca, X), E=112.5-165 MeV; calculated fusion σ vs E, total reaction σ. Phenomenological model.

doi: 10.1007/BF02754996
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1981GI03      Nuovo Cim. 61A, 182 (1981)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

Some Remarks on the Determination of Total Reaction Cross-Sections by Means of the << Sum of Differences >> Method

NUCLEAR REACTIONS Cr, Fe, Zr(α, α), E=13.5 MeV; Ge(α, α), E=13.2 MeV; measured σ(θ); deduced σ(reaction). Optical model analysis.

doi: 10.1007/BF02776609
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1981GI04      Nuovo Cim. 62A, 49 (1981)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

The Multistep Process in the ²⁴Mg(³He, α)²³Mg Reaction at 10 MeV

NUCLEAR REACTIONS ²⁴Mg(³He, α), E=10 MeV; analyzed σ(θ); ²³Mg levels deduced multistep process excitation. CCBA, entrance, exit channel inelastic effects.

doi: 10.1007/BF02776641
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1981GI07      Lett.Nuovo Cim. 31, 189 (1981)

R.Giordano, F.Porto, S.Sambataro, A.Scalia

A Modified SOD Method Applied to Heavy-Ion Reactions

NUCLEAR REACTIONS ²⁷Al(³²S, ³²S), E=145, 160 MeV; calculated σ(θ), σ(reaction); ⁴⁸Ti(³²S, ³²S), E(cm)=96 MeV; calculated σ(reaction).

doi: 10.1007/BF02776130
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1980GI09      Lett.Nuovo Cim. 29, 155 (1980)

R.Giordano, A.Guarrera, F.Porto, S.Sambataro, A.Scalia

Statistical Analysis of α-Scattering from ²⁵Mg between 11.8 and 13.2 MeV

NUCLEAR REACTIONS ²⁵Mg(α, α'), E=11.8-13.2 MeV; measured σ(E, θ); deduced compound nucleus contributions. Enriched target. Statistical model analysis.

doi: 10.1007/BF02743325
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