References quoted in the ENSDF dataset: 120SN 120SN(P,P'),(3HE,3HE'),(A,A'),(17O,17O')

37 references found.

Clicking on a keynumber will list datasets that reference the given article.

Return to 120SN(P,P'),(3HE,3HE'),(A,A'),(17O,17O')

1965AL11

Nucl.Phys. 66, 481 (1965)

D.L.Allan, B.H.Armitage, B.A.Doran

Energy Levels in Even Tin Isotopes from 11 MeV Proton Inelastic Scattering

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(p, p'), E = 11 MeV; measured σ(Ep', θ). ^{116,118,120,122,124}Sn deduced levels.

doi: 10.1016/0029-5582(65)90779-0

1965JO11

Phys.Rev. 139, B318 (1965)

R.K.Jolly

Analysis of Single Excitations in Inelastic Deuteron Scattering from Ni⁶⁰, Zr⁹², and Sn¹²⁰ Nuclei

NUCLEAR STRUCTURE ¹²⁰Sn, ⁶⁰Ni, ⁴¹Ca, ⁴⁸Sc, ⁹²Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B318

1966BA11

Phys.Rev. 146, 861 (1966)

N.Baron, R.F.Leonard, J.L.Need, W.M.Stewart, V.A.Madsen

Inelastic Alpha-Particle Excitation in the Even Tin Isotopes

NUCLEAR STRUCTURE ¹¹⁸Sn, ¹¹⁶Sn, ¹²⁰Sn, ¹²²Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.146.861

1968FU12

Nucl.Phys. A111, 81 (1968)

S.A.Fulling, G.R.Satchler

Theoretical Analysis of 30 MeV Proton Inelastic Scattering

NUCLEAR REACTIONS ²⁸Si, ⁴⁰Ca, ⁵⁶Fe, ^58,60Ni, ¹²⁰Sn, ²⁰⁸Pb(p, p'), E=30.3 MeV; measured nothing; analyzed σ(θ). ²⁸Si, ⁴⁰Ca, ⁵⁶Fe, ^58,60Ni, ¹²⁰Sn, ²⁰⁸Pb deduced deformation parameters.

doi: 10.1016/S0375-9474(68)90388-6

1968KU20

J.Phys.Soc.Japan 25, 14 (1968)

I.Kumabe, H.Ogata, T.-H.Kim, M.Inoue, Y.Okuma, M.Matoba

Scattering of 34.4-MeV Alpha Particles by the Tin Isotopes

NUCLEAR REACTIONS ^{116,117,118,119,120}Sn(α, α'), E=34.4 MeV; measured σ(Eα', θ). ^{116,117,118,119,120}Sn deduced levels, L, deformation parameters.

1968MA34

Phys.Rev. 174, 1429 (1968)

W.Makofske, W.Savin, H.Ogata, T.H.Kruse

Elastic and Inelastic Proton Scattering from Even Isotopes of Cd, Sn, and Te

NUCLEAR REACTIONS ^{110,112,114,116}Cd, ^{112,116,118,120,122,124}Sn, ^126,128,130Te(p, p'), E=16 MeV; measured σ(θ).

doi: 10.1103/PhysRev.174.1429

1970BE20

Nucl.Phys. A147, 326 (1970)

O.Beer, A.El Behay, P.Lopato, Y.Terrien, G.Vallois, K.K.Seth

Spectroscopy of Even Tin Isotopes by Inelastic Scattering of 24.5 MeV Protons

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(p, p'), Ep=24.5 MeV; measured σ(Ep', θ). ^{116,118,120,122,124}Sn deduced J, π, β(L). Enriched targets.

doi: 10.1016/0375-9474(70)90271-X

1970BR07

Nucl.Phys. A146, 597 (1970)

G.Bruge, J.C.Faivre, H.Faraggi, A.Bussiere

44 MeV α-Particle Scattering on Doubly Even Spherical Nuclei Near Closed Shells and Nuclear Structure of Collective States

NUCLEAR REACTIONS ⁴⁰Ca, ^46,48,50Ti, ⁵²Cr, ^54,56,58Fe, ^58,60,62,64Ni, ⁶⁴Zn, ^{112,114,116,118,120,122,124}Sn, ²⁰⁸Pb(α, α'), Eα=44 MeV; measured σ(Eα', θ). ⁴⁰Ca, ^46,48,50Ti, ⁵²Cr, ^54,56,58Fe, ^58,60,62,64Ni, ⁶⁴Zn, ^{112,114,116,118,120,122,124}Sn, ²⁰⁸Pb deduced levels, deformation lengths, B(E2), B(E3). Enriched targets.

doi: 10.1016/0375-9474(70)90747-5

1970COZR

Thesis, Univ.Paris (1970); NP-18461 (1970)

V.Comparat

Etude de la Diffusion Elastique des Protons de 156 MeV par les Isotopes Pairs de l'Etain

NUCLEAR REACTIONS ^116,118,120Sn(p, p), (p, p'), E=156 MeV; measured σ(θ); deduced optical model parameters. 116, 118, 120sn deduced deformation parameters.

1970KA10

Nucl.Phys. A147, 461 (1970)

O.Karban, P.D.Greaves, V.Hnizdo, J.Lowe, G.W.Greenlees

Inelastic Scattering of Polarized Protons at 30.3 MeV by ^54,56Fe, ⁵⁸Ni, ¹²⁰Sn and ²⁰⁸Pb

NUCLEAR REACTIONS ^54,56Fe, ⁵⁸Ni, ¹²⁰Sn, ²⁰⁸Pb(polarized p, p'), E=30.3 MeV; measured σ(θ), asymmetry (θ). ^54,56Fe, ⁵⁸Ni, ¹²⁰Sn, ²⁰⁸Pb deduced nuclear deformations β(L). Enriched targets.

doi: 10.1016/0375-9474(70)90592-0

1971HN03

Phys.Lett. 35B, 35 (1971)

V.Hnizdo, J.Lowe

Collective-Model Analysis of Inelastic Proton Scattering Using Potentials Derived from Nuclear Matter Distributions

NUCLEAR REACTIONS ⁵⁶Fe, ⁵⁸Ni, ¹²⁰Sn, ²⁰⁸Pb(polarized p, p), E=30.3 MeV; measured nothing; analyzed σ(θ), asymmetry(θ). Collective model analysis.

doi: 10.1016/0370-2693(71)90433-3

1972BR28

Phys.Rev. C6, 595 (1972)

I.Brissaud, B.Tatischeff, L.Bimbot, V.Comparat, A.Willis, M.K.Brussel

Study of Some Properties of Tin Isotopes Through High-Energy Alpha-Particle Scattering

NUCLEAR REACTIONS ^{116,118,120,124}Sn(α, α), (α, α'), E=166 MeV; measured σ(θ); deduced optical model parameters. ^{116,118,120,124}Sn deduced B(E2), B(E3), nuclear radii.

doi: 10.1103/PhysRevC.6.595

1972HO34

Nucl.Phys. A192, 651 (1972)

R.H.Howell, G.R.Hammerstein

Effect of Complex Coupling in Inelastic Cross Sections, Asymmetries and Spin Flip in the DWA

NUCLEAR REACTIONS ⁵⁸Ni, ¹²⁰Sn, ²⁰⁸Pb(p, p'), calculated σ(θ), spin-flip probability, asymmetry(θ); analyzed complex coupling effects.

doi: 10.1016/0375-9474(72)90096-6

1972IW01

Nucl.Phys. A183, 105 (1972)

H.Iwe, R.Reif, C.Riedel

Reaction Spectroscopy with Even Tin Isotopes

NUCLEAR REACTIONS ^116,118Sn(t, p), E=12 MeV; ¹¹⁶Sn(p, p'), E=55 MeV; ^116,118,120Sn(p, p'), E=16 MeV; calculated σ(θ). DWBA.

doi: 10.1016/0375-9474(72)90933-5

1972LE39

Nucl.Phys. A196, 337 (1972)

M.B.Lewis, F.E.Bertrand

Evidence from Inelastic Proton Scattering for a Giant Quadrupole Vibration in Spherical Nuclei

NUCLEAR REACTIONS ²⁷Al, ⁵⁴Fe, ¹²⁰Sn, ²⁰⁹Bi(p, p'), Ep=61.7 MeV; measured σ(θ). ²⁷Al, ⁵⁴Fe, ¹²⁰Sn, ²⁰⁹Bi deduced giant quadrupole excitation from systematics of σ.

doi: 10.1016/0375-9474(72)90968-2

1972YU03

Yad.Fiz. 16, 677 (1972); Sov.J.Nucl.Phys. 16, 380 (1973)

A.V.Yushkov

Shapes of Heavy Nuclei

NUCLEAR REACTIONS ^92,100Mo, ^{116,118,120,122}Sn, ^{122,124,126,128,130}Te, ^148,152,154Sm, ¹⁶⁶Er, ¹⁷⁶Yb(α, α), (α, α'); calculated signs for equlibrium deformation.

1973BI12

Nucl.Phys. A210, 397 (1973)

L.Bimbot, B.Tatischeff, I.Brissaud, Y.Le Bornec, N.Frascaria, A.Willis

Study of Microscopic Wave Functions of Nuclear Levels Through Inelastic Scattering of 166 MeV α-Particles

NUCLEAR REACTIONS ¹²C, ²⁴Mg, ²⁸Si, ³²S, ^40,44,48Ca, ⁴⁸Ti, ⁵⁶Fe, ^58,60,62Ni, ⁶⁸Zn, ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ^{116,118,120,124}Sn, ¹⁴⁰Ce, ²⁰⁸Pb(α, α'), Eα=166 MeV; measured σ(Eα, θ); α-n interaction, phenomenological, calculated optical potentials used with DWBA; microscopic wave functions tested.

doi: 10.1016/0375-9474(73)90310-2

1973HA58

Nucl.Phys. A213, 45 (1973)

G.R.Hammerstein, R.H.Howell, F.Petrovich

Electron and Proton Inelastic Scattering from ⁴⁰Ca, ¹²⁰Sn, and ²⁰⁸Pb

NUCLEAR REACTIONS ⁴⁰Ca, ¹²⁰Sn, ²⁰⁸Pb(e, e'), (p, p'); calculated σ(θ).

doi: 10.1016/0375-9474(73)90181-4

1973PE06

Nucl.Phys. A206, 623 (1973)

G.Perrin, Nguyen Van Sen, J.Arvieux, C.Perrin, R.Darves-Blanc, J.L.Durand, A.Fiore, J.C.Gondrand, F.Merchez

Elastic and Inelastic Scattering of Polarized Deuterons by ¹²⁰Sn at 28.6 MeV

NUCLEAR REACTIONS ¹²⁰Sn(polarized d, d), E=28.6 MeV; measured σ(θ), iT₁₁(θ), T₂₀(θ), T₂₂(θ)-square root(3/2)T₂₀(θ); ¹²⁰Sn(polarized d, d'), E=28.6 MeV; measured σ(θ), iT₁₁(θ); deduced optical-model parameters. ¹²⁰Sn deduced deformations β₂, β₃. Enriched target.

doi: 10.1016/0375-9474(73)90091-2

1973TE01

Nucl.Phys. A199, 65 (1973)

Y.Terrien

Microscopic Calculation for Proton Inelastic Scattering from Collective Levels in the Tin Isotopes

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(p, p'), E=16, 24.5 MeV; analyzed σ(θ); deduced transition densities.

doi: 10.1016/0375-9474(73)90334-5

1973TE05

Phys.Lett. 45B, 235 (1973)

Y.Terrien, J.L.Escudie, M.Buenerd, J.M.Loiseaux, P.Martin, J.B.Viano

The Role of the Imaginary Part in the Microscopic Description of (p, p') Scattering

NUCLEAR REACTIONS ⁹²Mo, ^116,120,124Sn(p, p'), E=40 MeV; measured σ(θ).

doi: 10.1016/0370-2693(73)90191-3

1973TE07

Nucl.Phys. A215, 29 (1973)

Y.Terrien

The Role of the Imaginary Form Factor in the Microscopic Description of (p, p') Scattering from Nuclei with One Closed Shell

NUCLEAR REACTIONS ⁴⁰Ca, ^58,60,62,64Ni, ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ^{116,118,120,124}Sn(p, p'), E=20-62 MeV; calculated σ(Ep', θ).

doi: 10.1016/0375-9474(73)90098-5

1980BE50

Phys.Rev. C22, 1832 (1980)

F.E.Bertrand, G.R.Satchler, D.J.Horen, J.R.Wu, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, A. van der Woude

Giant Multipole Resonances from Inelastic Scattering of 152-MeV Alpha Particles

NUCLEAR REACTIONS ²⁰⁸Pb, ¹²⁰Sn, ⁹⁰Zr, ⁵⁸Ni, ⁴⁶Ti(α, α), (α, α'), E=152 MeV; measured σ(Eα, θ). ⁴⁶Ti, ⁵⁸Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb deduced GQR, giant monopole resonances, Γ, L, T, β(L), B(λ), EWSR. Folding model analysis.

doi: 10.1103/PhysRevC.22.1832

1981BE33

Phys.Lett. 103B, 326 (1981)

F.E.Bertrand, E.E.Gross, D.J.Horen, J.R.Wu, J.Tinsley, D.K.McDaniels, L.W.Swenson, R.Liljestrand

Excitation of Giant Resonance Modes in ⁹⁰Zr and ¹²⁰Sn by 200 MeV Protons

NUCLEAR REACTIONS ⁹⁰Zr, ¹²⁰Sn(p, p'), E=200 MeV; measured σ(Ep, θ). ⁹⁰Zr deduced M1 transition strength. ⁹⁰Zr, ¹²⁰Sn deduced GDR, isoscalar GQR, giant octupole resonance, hexadecapole strength upper limit. Broad-range magnetic spectrograph.

doi: 10.1016/0370-2693(81)90235-5

1981YA02

Phys.Rev. C23, 937 (1981); Erratum Phys.Rev. C23, 2798 (1981)

T.Yamagata, S.Kishimoto, K.Yuasa, K.Iwamoto, B.Saeki, M.Tanaka, T.Fukuda, I.Miura, M.Inoue, H.Ogata

High Energy Component of Giant Octupole Resonance in Medium and Heavy Mass Nuclei

NUCLEAR REACTIONS ^90,92Zr, ^116,118,120Sn, ¹⁴⁴Sm, ²⁰⁸Pb(³He, ³He'), E=110-140 MeV; measured σ(θ, E). ^90,92Zr, ^116,118,120Sn, ¹⁴⁴Sm, ²⁰⁸Pb deduced giant octupole resonance, deformation β₃, EWSR. Enriched target. DWBA analysis.

doi: 10.1103/PhysRevC.23.937

1982DJ04

Nucl.Phys. A388, 1 (1982)

C.Djalali, N.Marty, M.Morlet, A.Willis, J.C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky, P.Kitching

Systematics of the Excitation of M1 Resonances in Medium Heavy Nuclei by 200 MeV Proton Inelastic Scattering

NUCLEAR REACTIONS ⁵¹V, ^58,60,62Ni, ⁶⁸Zn, ^90,92,94,96Zr, ^{92,94,96,98,100}Mo, ^120,124Sn, ¹⁴⁰Ce(p, p'), E=200 MeV; measured σ(θ). ⁵¹V, ^58,60,62Ni, ⁶⁸Zn, ^90,92,94,96Zr, ^{92,94,96,98,100}Mo, ^120,124Sn, ¹⁴⁰Ce deduced resonances, Γ, T, M1 character.

doi: 10.1016/0375-9474(82)90505-X

1983BL09

Phys.Rev. C28, 1475 (1983)

M.Blann, H.K.Vonach

Global Test of Modified Precompound Decay Models

NUCLEAR REACTIONS, ICPND ²⁰²Hg(p, 2p), (p, n2p), E=30-90 MeV; calculated σ(E). ²⁷Al, ⁵⁸Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(p, X), E ≈ 10-100 MeV; ²⁰⁸Pb, ²⁷Al(n, X), E ≈ 0.3-100 MeV; Ni(n, X), E ≈ 1-15 MeV; Sn(n, X), E ≈ 0.5-30 MeV; calculated reaction σ(E). ⁵²Cr, ⁵⁶Fe, ⁹³Nb(n, xn), E=14.5 MeV; calculated σ vs En. ⁵²Cr, ⁵⁶Fe, ⁹³Nb(n, p), E=14.7 MeV; calculated σ(Ep). ⁵¹V(p, n), E=18-26 MeV; ^107,109Ag, ^108,110Pd(p, n), E=18, 22, 25 MeV; ²⁰⁸Pb(p, n), E=35, 45 MeV; ¹²⁰Sn, ⁴⁸Ca(p, n), E=25, 35, 45 MeV; ²⁷Al, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁹Bi(p, n), E=90 MeV; calculated σ(En). ⁹⁰Zr, ²⁰⁹Bi, ²⁷Al, ⁵⁸Ni(p, p'), E=90 MeV; ⁵⁴Fe, ²⁰⁹Bi(p, p'), E=39, 62 MeV; calculated σ(Ep'); deduced best-fit model, parameter set. Hybrid, geometry dependent hybrid precompound decay models.

doi: 10.1103/PhysRevC.28.1475

1983SA27

Phys.Rev. C28, 1527 (1983)

K.Sato, A.Iwamoto, K.Harada

Pre-Equilibrium Emission of Light Composite Particles in the Framework of the Exciton Model

NUCLEAR REACTIONS ⁸⁹Y, ¹²⁰Sn, ¹⁹⁷Au, ⁵⁴Fe(p, p), (p, d), (p, t), (p, ³He), (p, α), E=62 MeV; ⁵⁸Ni(p, t), (p, α), (p, ³He), E=90 MeV; calculated σ(Ep), σ(Ed), σ(Et), σ(E(³He)), σ(Eα); deduced composite particle emission mechanism. Exciton model.

doi: 10.1103/PhysRevC.28.1527

1984AM03

J.Phys.(London) G10, 331 (1984)

K.Amos, I.Morrison, R.Smith

Interacting Boson-Fermion Models and Transition Densities

NUCLEAR REACTIONS ²⁰Ne(p, p'), E=24.5 MeV; ^{112,114,116,118,120,122,124}Sn(n, n'), E=24 MeV; calculated σ(θ). ²⁰Ne(e, e'), E not given; calculated form factor. Interacting boson model spectroscopic amplitudes, B(E2) matching.

NUCLEAR STRUCTURE ²⁰Ne, ^{112,114,116,118,120,122,124}Sn; calculated BCS level occupancies, spectroscopic amplitudes. Interacting boson approximation.

doi: 10.1088/0305-4616/10/3/009

1984WO06

Phys.Rev. C29, 1710 (1984)

C.Wong, S.M.Grimes, R.W.Finlay

Analysis of (p, p), (p, n), and (n, n) Scattering on the Even Tin Isotopes using the Lane Coupled Equations

NUCLEAR REACTIONS ^{116,118,122,124}Sn(p, n), E=24.5 MeV; measured σ(θ), σ(En); deduced isocalar, isovector strengths of potential. ^116,120,124Sn(n, n), E=11 MeV; analyzed σ(θ); deduced potential parameters. Lane model, imaginary potential Coulomb correction.

doi: 10.1103/PhysRevC.29.1710

1985TIZZ

Diss.Abst.Int. 46B, 561 (1985)

J.R.Tinsley

A Survey of Giant Resonance Excitations with 200 MeV Protons

NUCLEAR REACTIONS ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(p, p'), E=200 MeV; measured σ(θ). ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb deduced giant multipole resonances.

1988BU21

Phys.Rev. C38, 2514 (1988)

M.Buenerd, K.Bouhelal, Ph.Martin, J.Chauvin, D.Lebrun, G.Perrin, P.de Saintignon, G.Duhamel

Quadrupole Transitions at Very Small Momentum Transfer in Nuclei

NUCLEAR REACTIONS ⁵⁸Ni, ⁹²Mo, ^120,124Sn, ¹⁴⁰Ce, ²⁰⁸Pb(³He, ³He'), E=108.5 MeV; measured σ(θ). ⁵⁸Ni, ⁹²Mo, ^120,124Sn, ¹⁴⁰Ce, ²⁰⁸Pb deduced giant resonances excitation, deformation parameters, B(λ).

doi: 10.1103/PhysRevC.38.2514

1988SH38

Phys.Rev. C38, 2562 (1988)

M.M.Sharma, W.T.A.Borghols, S.Brandenburg, S.Crona, A.van der Woude, M.N.Harakeh

Giant Monopole Resonance in Sn and Sm Nuclei and the Compressibility of Nuclear Matter

NUCLEAR REACTIONS ^{112,114,116,120,124}Sn, ^{144,148,150,152}Sm(α, α'), E=120 MeV; measured σ(E, θ); deduced compressibility of nuclear matter. ^{112,114,116,120,124}Sn, ^{144,148,150,152}Sm deduced GQR, GMR, Γ, sum rule strength. DWBA analysis.

doi: 10.1103/PhysRevC.38.2562

1993LI24

Nucl.Phys. A560, 733 (1993)

R.Liguori Neto, P.Roussel-Chomaz, L.Rochais, N.Alamanos, F.Auger, B.Fernandez, J.Gastebois, A.Gillibert, R.Lacey, A.Miczaika, D.Pierroutsakou, J.Barrette, S.K.Mark, R.Turcotte, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, T.Suomijarvi, A.Van der Woude, A.M.Van den Berg

Excitation of Giant Resonances in ²⁰⁸Pb, ¹²⁰Sn, ⁹⁰Zr and ⁶⁰Ni by 84 MeV/nucleon ¹⁷O Ions

NUCLEAR REACTIONS ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(¹⁷O, ¹⁷O), (¹⁷O, ¹⁷O'), E=1435 MeV; measured σ(θ); deduced model parameters. ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb levels deduced B(λ), giant monopole, quadrupole reasonances.

doi: 10.1016/0375-9474(93)90043-W

1998BA37

Nucl.Phys. A635, 428 (1998)

T.Baumann, E.Ramakrishnan, A.Azhari, J.R.Beene, R.J.Charity, J.F.Dempsey, M.L.Halbert, P.-F.Hua, R.A.Kryger, P.E.Mueller, R.Pfaff, D.G.Sarantites, L.G.Sobotka, D.W.Stracener, M.Thoennessen, G.Van Buren, R.L.Varner, S.Yokoyama

Evolution of the Giant Dipole Resonance in Excited ¹²⁰Sn and ²⁰⁸Pb Nuclei Populated by Inelastic Alpha Scattering

NUCLEAR REACTIONS ¹²⁰Sn(α, α'), E=40, 50 MeV/nucleon; ²⁰⁸Pb(α, α'), E=40 MeV/nucleon; measured Eγ, Iγ, Eα, Iα, αγ-coin. ¹²⁰Sn, ²⁰⁸Pb deduced GDR width vs temperature, shape effects. Adiabatic coupling model.

doi: 10.1016/S0375-9474(98)00197-3

2001BA08

Phys.Rev. C63, 024607 (2001)

E.Bauge, J.P.Delaroche, M.Girod

Lane-Consistent, Semimicroscopic Nucleon-Nucleus Optical Model

NUCLEAR REACTIONS ⁵⁸Ni(polarized p, p), E=10-200 MeV; ²⁰⁸Pb(polarized n, n), E=2-155 MeV; ^54,56Fe, ^58,61,62,64Ni, ⁷⁰Zn, ^90,96Zr, ⁹⁶Mo, ⁹⁶Ru, ¹¹⁵In, ^{112,116,117,118,120,124}Sn(polarized p, n), E=23 MeV; calculated σ(θ), Ay(θ). ⁴⁰Ca, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(n, X), E < 200 MeV; calculated total σ. ^54,56Fe, ⁶⁰Ni, ⁹²Mo, ⁹³Nb, ¹⁰⁴Pd, ^{112,116,120,124}Sn, ¹³⁸Ba, ¹⁴²Nd, ¹⁴⁴Sm, ²⁰⁸Pb(p, n), E=26, 30, 35 MeV; ⁴⁸Ca, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(p, n), E=25, 35, 45, 120, 135, 160 MeV; calculated σ(θ). Lane-consistent, semimicroscopic optical model, comparisons with data.

doi: 10.1103/PhysRevC.63.024607

2001SI02

Nucl.Phys. A679, 287 (2001)

C.P.Silva, M.A.G.Alvarez, L.C.Chamon, D.Pereira, M.N.Rao, E.S.Rossi, Jr., L.R.Gasques, M.A.E.Santo, R.M.Anjos, J.Lubian, P.R.S.Gomes, C.Muri, B.V.Carlson, S.Kailas, A.Chatterjee, P.Singh, A.Shrivastava, K.Mahata, S.Santra

The Heavy-Ion Nuclear Potential: Determination of a systematic behavior at the region of surface interaction distances

NUCLEAR REACTIONS ¹²⁰Sn(¹⁶O, ¹⁶O), E=53-55 MeV; ¹³⁸Ba(¹⁶O, ¹⁶O), E=54-57 MeV; ²⁰⁸Pb(¹⁶O, ¹⁶O), E=74-78 MeV; measured σ(θ); deduced optical potentials. Double-folding calculations with microscopic densities.

doi: 10.1016/S0375-9474(00)00347-X