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NSR database version of May 20, 2024.

Search: Author = Y.Eisen

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2022SH09      Phys.Rev. C 105, 025802 (2022)

A.Shor, L.Weissman, M.Tessler, O.Aviv, Y.Eisen, G.Feinberg, Y.Mishnayot, A.Plompen, S.Vaintraub

Measurements of the 210gBi to 210mBi activation ratio for the 209Bi (n, γ) reaction with thermal and epithermal neutrons at the Soreq IRR1 reactor

NUCLEAR REACTIONS 209Bi(n, γ), E=thermal, epithermal; measured Eγ, Iγ; deduced σ, isomeric ratio, Maxwellian averaged σ for isomeric and ground state. Activation technique. Comparison to other experimental results and evaluations from nuclear data libraries (JENDL/A-96, ROSFOND-2010, JENDL-4.0, JEFF-3.2, BROND-3.1).

RADIOACTIVITY 210Bi(β-); 210mBi(α)[from 209Bi(n, γ), E=thermal, epithermal]; 210Po(α)[from 210Bi(β-)]; measured Eγ, Iγ.

doi: 10.1103/PhysRevC.105.025802
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31849.


2019PA22      Eur.Phys.J. A 55, 44 (2019)

M.Paul, M.Tessler, M.Friedman, S.Halfon, T.Palchan, L.Weissman, A.Arenshtam, D.Berkovits, Y.Eisen, I.Eliahu, G.Feinberg, D.Kijel, A.Kreisel, I.Mardor, G.Shimel, A.Shor, I.Silverman

Reactions along the astrophysical s-process path and prospects for neutron radiotherapy with the Liquid-Lithium Target (LiLiT) at the Soreq Applied Research Accelerator Facility (SARAF)

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1880.4 - 1.92 keV[reaction threshold]; measured thick-target Eγ, Iγ(θ) using the Liquid-Lithium Target (LiLiT) system with the Soreq Applied Research Accelerator Facility (SARAF) Phase I; deduced astrophysical s-process sequence of nuclei.

doi: 10.1140/epja/i2019-12723-5
Citations: PlumX Metrics


2018SH12      Phys.Rev. C 97, 034303 (2018)

A.Shor, L.Weissman, O.Aviv, Y.Eisen, M.Brandis, M.Paul, A.Plompen, M.Tessler, S.Vaintraub

Branching ratio to the 803 keV level in 210Po α decay

RADIOACTIVITY 210Po(α)[from 210Bi(β-) decay, 210Bi from 209Bi(n, γ), E=thermal at Soreq nuclear reactor facility]; measured Eγ, Iγ, Eα, Iα, α-branching ratio to the 803-keV level in 206Pb. Comparison with previous experimental results from 1951 to 1999, and evaluated data in ENSDF and DDEP databases. Relevance to cross section for 209Bi(n, γ)210Bi involved in termination of the astrophysical s process.

NUCLEAR REACTIONS 209Bi(n, γ), E=thermal; measured Eα, Iα from decay of 210Po; deduced σ for thermal capture σ.

doi: 10.1103/PhysRevC.97.034303
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2017SH47      Phys.Rev. C 96, 055805 (2017)

A.Shor, M.Tessler, A.Plompen, A.Arenshtam, O.Aviv, D.Berkovits, M.Brandis, Y.Eisen, I.Eliyahu, G.Feinberg, M.Friedman, S.Halfon, M.Hult, B.Kaizer, D.Kijel, A.Krasa, A.Kreisel, T.Palchan, M.Paul, A.Perry, I.Silverman, S.Vaintraub, L.Weissman

Bismuth activation with quasi-Maxwellian neutrons at kT ∼ 30 keV

NUCLEAR REACTIONS 209Bi(n, γ), kT≈30 keV quasi-Maxwellian neutrons; measured Eβ from the decay of 210Bi and Eα and Eγ, Iγ from the decay of 206Po using PIPS silicon detector for particles and HPGe detector for γ rays at the linear accelerator of Soreq Applied Research Accelerator facility (SARAF); deduced Maxwellian averaged (MACS) σ, and compared with previous experimental results, and with evaluated cross sections in the ENDF, JEFF and JENDL data libraries. Relevance to termination point of the s-process cycle of nucleosynthesis in stellar environments.

doi: 10.1103/PhysRevC.96.055805
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31780.


2015HI08      Nucl.Instrum.Methods Phys.Res. B362, 29 (2015)

T.Y.Hirsh, A.Kreisel, J.Mrazek, L.Weissman, Y.Eisen, M.Stefanik, E.Simeckova, O.Aviv, S.Moscovici, Z.Yungrais, D.Berkovits

Accurate measurement of the 23Na(d, p)24Na cross section in the 1.7-20 MeV energy range

NUCLEAR REACTIONS 23Na(d, p), E=1.7-20 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data.

doi: 10.1016/j.nimb.2015.09.015
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0782.


2015TE06      Phys.Lett. B 751, 418 (2015)

M.Tessler, M.Paul, A.Arenshtam, G.Feinberg, M.Friedman, S.Halfon, D.Kijel, L.Weissman, O.Aviv, D.Berkovits, Y.Eisen, I.Eliyahu, G.Haquin, A.Kreisel, I.Mardor, G.Shimel, A.Shor, I.Silverman, Z.Yungrais

Stellar 30-keV neutron capture in 94, 96Zr and the 90Zr(γ, n)89Zr photonuclear reaction with a high-power liquid-lithium target

NUCLEAR REACTIONS 94,96Zr(n, γ), E=30 keV; 90Zr(γ, n), E not given; measured reaction products, Eγ, Iγ; deduced yields, Maxwellian averaged σ. Comparison with available data.

doi: 10.1016/j.physletb.2015.10.058
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31765.


2014WE10      Nucl.Instrum.Methods Phys.Res. B342, 7 (2014)

L.Weissman, A.Kreisel, T.Hirsh, O.Aviv, D.Berkovits, O.Girshevitz, Y.Eisen

Accurate measurements of the 63Cu(d, p)64Cu and natCu(d, x)65Zn cross-sections in the 2.77-5.62 MeV energy range

NUCLEAR REACTIONS 63Cu(d, p)64Cu, Cu(d, x)65Zn, E=2.77-5.62 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with experimental data.

doi: 10.1016/j.nimb.2014.09.002
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0753.


2013FR01      Nucl.Instrum.Methods Phys.Res. A698, 117 (2013)

M.Friedman, D.Cohen, M.Paul, D.Berkovits, Y.Eisen, G.Feinberg, G.Giorginis, S.Halfon, A.Krasa, A.J.M.Plompen, A.Shor

Simulation of the neutron spectrum from the 7Li(p, n) reaction with a liquid-lithium target at Soreq Applied Research Accelerator Facility

NUCLEAR REACTIONS 7Li(p, n), E<3.5 MeV; analyzed available data; deduced neutron source parameters for Maxwellian-averaged σ measurements. Comparison with available data.

doi: 10.1016/j.nima.2012.09.027
Citations: PlumX Metrics


2012FE06      Phys.Rev. C 85, 055810 (2012)

G.Feinberg, M.Friedman, A.Krasa, A.Shor, Y.Eisen, D.Berkovits, D.Cohen, G.Giorginis, T.Hirsh, M.Paul, A.J.M.Plompen, E.Tsuk

Quasi-stellar neutrons from the 7Li(p, n)7Be reaction with an energy-broadened proton beam

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1.85-1.95 MeV; measured time of flight, spectrum, E(n), I(n), σ(θ), narrow and broad-energy proton beam; deduced angle-integrated spectrum and Maxwellian-flux distribution. 27Al(p, γ), E=0.985-1.0 MeV; measured thick-target σ(E). 197Au(n, γ), E<160 keV; measured Eγ, Iγ, average activation σ for neutrons from 7Li(p, n) reaction. Relevance to s-process cross sections.

doi: 10.1103/PhysRevC.85.055810
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23284.


2012FE11      J.Phys.:Conf.Ser. 337, 012044 (2012)

G.Feinberg, A.Shor, D.Berkovits, Y.Eisen, M.Friedman, G.Giorginis, T.Hirsh, A.Krasa, M.Paul, A.Plompen, E.Tsuk

Energy-broadened proton beam for production of quasi-stellar neutrons from the 7Li(p, n)7Be reaction

NUCLEAR REACTIONS 7Li(p, n), E=1912 keV; measured thick target En, In(θ) using ToF with 6Li glass detectors and both narrow- and broad-energy beams; deduced σ(En, θ).

doi: 10.1088/1742-6596/337/1/012044
Citations: PlumX Metrics


1994EI10      Nucl.Instrum.Methods Phys.Res. A353, 60 (1994)

Y.Eisen, Y.Horovitz

Correction of Incomplete Charge Collection in CdTe Detectors

RADIOACTIVITY 133Ba(EC); analyzed spectra; deduced CdTe detectors associated incomplete charge collection correction function. Monte Carlo code.

doi: 10.1016/0168-9002(94)91603-9
Citations: PlumX Metrics


1994MC11      Nucl.Instrum.Methods Phys.Res. A343, 527 (1994)

D.S.McGregor, R.A.Rojeski, G.F.Knoll, F.L.Terry, Jr., J.East, Y.Eisen

Present Status of Undoped Semi-Insulating LEC Bulk GaAs as a Radiation Spectrometer

RADIOACTIVITY 228Th(α); measured α-spectra. Thick bulk GaAs detector.

doi: 10.1016/0168-9002(94)90233-X
Citations: PlumX Metrics


1992EI01      Nucl.Instrum.Methods Phys.Res. A322, 596 (1992)

Y.Eisen

Current State-of-the-Art Applications Utilizing CdTe Detectors

RADIOACTIVITY 133Ba(EC); 57Co(EC); measured spectra. Single or array of CdTe detectors, different applications discussed.

doi: 10.1016/0168-9002(92)91238-5
Citations: PlumX Metrics


1980EY01      Phys.Rev. C21, 1377 (1980)

Y.Eyal, A.Gavron, I.Tserruya, Z.Fraenkel, Y.Eisen, S.Wald, R.Bass, C.R.Gould, G.Kreyling, R.Renfordt, K.Stelzer, R.Zitzmann, A.Gobbi, U.Lynen, H.Stelzer, I.Rode, R.Bock

Neutron Emission in Deep-Inelastic Collisions Induced by 86Kr on 166Er at 5.7, 7.0, and 7.9 MeV/Nucleon

NUCLEAR REACTIONS 166Er(86Kr, X), E=496, 602, 675 MeV; measured n(fragment)(fragment)-, (fragment)(fragment)-coin; deduced σ(En), out-of-plane neutron anisotropy, multiplicities. Statistical model.

doi: 10.1103/PhysRevC.21.1377
Citations: PlumX Metrics


1980ST09      Phys.Rev. C21, 2427 (1980)

R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilansky, I.Tserruya

Fusion of 16O + 148,150,152,154Sm at Sub-Barrier Energies

NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured evaporation residue Eγ, E(K X-ray), I(K X-ray); deduced fusion σ(E).

doi: 10.1103/PhysRevC.21.2427
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1608.


1979KO20      Phys.Rev. C20, 1305 (1979)

D.G.Kovar, D.F.Geesaman, T.H.Braid, Y.Eisen, W.Henning, T.R.Ophel, M.Paul, K.E.Rehm, S.J.Sanders, P.Sperr, J.P.Schiffer, S.L.Tabor, S.Vigdor, B.Zeidman, F.W.Prosser, Jr.

Systematics of Carbon- and Oxygen-Induced Fusion on Nuclei with 12 ≤ A ≤ 19

NUCLEAR REACTIONS 12C(12C, X), E(cm)=7.4-31.2 MeV; 12C(13C, X), E(cm)=7.6-24.9 MeV; 12C(14N, X), E(cm)=15.1-24.0 MeV; 12C(15N, X), E(cm)=8.9-26.7 MeV; 12C(16O, X), E(cm)=12.9-27.0 MeV; 12C(18O, X), E(cm)=11.9-28.0 MeV; 12C(19F, X), E(cm)=11.6-27.1 MeV; 16O(16O, X), E(cm)=16.9-36.0 MeV; measured fusion σ(E); deduced fusion barrier parameters.

doi: 10.1103/PhysRevC.20.1305
Citations: PlumX Metrics


1978EY01      Phys.Rev.Lett. 41, 625 (1978)

Y.Eyal, A.Gavron, I.Tserruya, Z.Fraenkel, Y.Eisen, S.Wald, R.Bass, G.R.Gould, G.Kreyling, R.Renfordt, K.Stelzer, R.Zitzmann, A.Gobbi, U.Lynen, H.Stelzer, I.Rode, R.Bock

Neutron Emission in Strongly Damped Collisions of 86Kr on 166Er at 602 MeV

NUCLEAR REACTIONS 166Er(86Kr, xn), E=602 MeV; measured neutron multiplicity.

doi: 10.1103/PhysRevLett.41.625
Citations: PlumX Metrics


1978HE14      Phys.Rev. C17, 2245 (1978)

W.Henning, Y.Eisen, H.-J.Korner, D.G.Kovar, J.P.Schiffer, S.Vigdor, B.Zeidman

Optimum Q Value in Heavy-Ion-Induced Neutron Transfer at the Coulomb Barrier

NUCLEAR REACTIONS 118Sn(18O, 16O), E=53-62 MeV; measured σ(E, θ); deduced optimum Q.

doi: 10.1103/PhysRevC.17.2245
Citations: PlumX Metrics


1978KO01      Phys.Rev. C17, 83 (1978)

D.G.Kovar, W.Henning, B.Zeidman, Y.Eisen, J.R.Erskine, H.T.Fortune, T.R.Ophel, P.Sperr, S.E.Vigdor

16O + 48Ca Reaction at 56 Mev. I. Transitions to Resolved Levels

NUCLEAR REACTIONS 48Ca(16O, 16O), (16O, 16O'), (16O, 17O), (16O, 18O), (16O, 14N), 48Ca(16O, 15N), (16O, 16N), (16O, 13C), (16O, 14C), (16O, 15C), (16O, 19O), 48Ca(16O, 17N), (16O, 12C), (16O, 11B), (16O, 12B), (16O, 13B), E=56 MeV; measured σ(θ); deduced optical model parameters. 51,50Ti, 18O, 50Sc, 51V, 48Sc, 49Ti levels deduced reaction population.

doi: 10.1103/PhysRevC.17.83
Citations: PlumX Metrics


1978ST15      Phys.Rev.Lett. 41, 465 (1978)

R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilansky, I.Tserruya

Effect of Nuclear Deformation on Heavy-Ion Fusion

NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured fusion σ(E).

doi: 10.1103/PhysRevLett.41.465
Citations: PlumX Metrics


1978ST29      S.Afr.J.Phys. 1, 171 (1978)

R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilanski, I.Tserruya

The Effect of Nuclear Deformation on Heavy-Ion Fusion

NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured σ(fusion); deduced importance of nuclear deformation.


1978TS04      Phys.Rev. C18, 1688 (1978)

I.Tserruya, Y.Eisen, D.Pelte, A.Gavron, H.Oeschler, D.Berndt, H.L.Harney

Total Fusion Cross Section for the 16O + 16O System

NUCLEAR REACTIONS 16O(16O, X), E=27-66 MeV; measured fusion σ(E); deduced barrier, critical parameters. Statistical model analysis.

doi: 10.1103/PhysRevC.18.1688
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1541.


1977EI01      Nucl.Phys. A291, 459 (1977)

Y.Eisen, I.Tserruya, Y.Eyal, Z.Fraenkel, M.Hillman

Total Fusion Cross Sections for 18,17,16O + 27Al at Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 27Al(16O, X), (17O, X), (18O, X), E=27-42 MeV; measured complete fusion σ(E). 27Al(16O, 16O), (17O, 17O), (18O, 18O), E=21-40 MeV; measured σ(E, θ); deduced effective fusion radii.

doi: 10.1016/0375-9474(77)90332-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1541.


1977HE02      Phys.Rev. C15, 292 (1977)

W.Henning, Y.Eisen, J.R.Erskine, D.G.Kovar, B.Zeidman

Optical-Model Potential in Single-Nucleon-Transfer Reactions Induced by Heavy Ions

NUCLEAR REACTIONS 48Ca(16O, 16O), (16O, 15N), (19F, 18O), E=56 MeV; 45Sc(15N, 15N), E=47.53 MeV; 48Ca(15N, 14C), E=48 MeV; measured σ(θ). Optical model, DWBA analyses.

doi: 10.1103/PhysRevC.15.292
Citations: PlumX Metrics


1977SA04      Nucl.Phys. A279, 210 (1977)

M.Samuel, U.Smilansky, B.A.Watson, Y.Eisen, A.M.Kleinfeld, D.Werdecker

Measurement of Nuclear Deformation Parameters from Elastic and Inelastic Scattering of α and 3He Ions on Te Isotopes

NUCLEAR REACTIONS 122,124,126,128Te(α, α), 128Te(3He, 3He), E=8-18 MeV; measured σ(θ, E) for ground state, first 2+ state; deduced optical model parameters. 122,124,126,128Te deduced deformations, B(E2). Enriched targets.

doi: 10.1016/0375-9474(77)90224-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0866.


1977TA07      Phys.Rev. C16, 673 (1977)

S.L.Tabor, Y.Eisen, D.G.Kovar, Z.Vager

Comparison of Light- and Heavy-Ion Emission from the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, p), (16O, α), E=30-64 MeV; measured σ(E, θ). 12C(16O, X), E=35, 49, 62 MeV; measured σ(Z, θ).

doi: 10.1103/PhysRevC.16.673
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0117.


1976EI02      Phys.Rev. C13, 699 (1976)

Y.Eisen, H.T.Fortune, W.Henning, D.G.Kovar, S.Vigdor, B.Zeidman

Two-Nucleon Transfer Reactions Induced by 16O on 42Ca and 48Ca

NUCLEAR REACTIONS 42,48Ca(16O, 18O), (16O, 14C), E=56 MeV; measured σ(θ). 44,50Ti, 40,46Ca levels deduced L. 18O, 46Ca, 44,50Ti levels deduced S.

doi: 10.1103/PhysRevC.13.699
Citations: PlumX Metrics


1976EI03      Phys.Lett. 63B, 253 (1976)

Y.Eisen, B.Day

Importance of the Non-Open N-N Force and of the Exchange Potential for Elastic Scattering of Alpha Particles

NUCLEAR REACTIONS 90Zr(α, α), E=6-24 MeV; calculated potential.

doi: 10.1016/0370-2693(76)90256-2
Citations: PlumX Metrics


1976SP03      Phys.Rev.Lett. 36, 405 (1976)

P.Sperr, S.Vigdor, Y.Eisen, W.Henning, D.G.Kovar, T.R.Ophel, B.Zeidman

Oscillations in the Excitation Function for Complete Fusion of 16O + 12C

NUCLEAR REACTIONS 12C(16O, X), E(cm)=13-27 MeV; measured total fusion σ(E).

doi: 10.1103/PhysRevLett.36.405
Citations: PlumX Metrics


1976SP07      Phys.Rev.Lett. 37, 321 (1976)

P.Sperr, T.H.Braid, Y.Eisen, D.G.Kovar, F.W.Prosser, Jr., J.P.Schiffer, S.L.Tabor, S.Vigdor

Fusion Cross Sections of Light Heavy-Ion Systems: Resonances and shell effects

NUCLEAR REACTIONS 12C(12C, X), (18O, X), (19F, X), E(cm)=6-32 MeV; measured fusion σ.

doi: 10.1103/PhysRevLett.37.321
Citations: PlumX Metrics


1975EI03      Phys.Lett. 56B, 313 (1975)

Y.Eisen, B.Day, E.Friedman

Microscopic Description of the Real Alpha-Nucleus Potential at Large Distances

NUCLEAR REACTIONS 90Zr, 208Pb(α, α); calculated optical potentials.

doi: 10.1016/0370-2693(75)90307-X
Citations: PlumX Metrics


1975FO09      Phys.Lett. 57B, 445 (1975)

H.T.Fortune, W.Henning, D.C.Kovar, B.Zeidman, Y.Eisen

Transfer of Three Identical Nucleons in 16O + 48Ca

NUCLEAR REACTIONS 48Ca(16O, X), E=56 MeV; measured σ(E(fragment mass), θ). 48Ca(16O, 13B), (16O, 19O), E=56 MeV; measured σ(θ); deduced Q.

doi: 10.1016/0370-2693(75)90264-6
Citations: PlumX Metrics


1975HE16      Phys.Lett. 58B, 129 (1975)

W.Henning, J.P.Schiffer, D.G.Kovar, S.Vigdor, B.Zeidman, Y.Eisen, H.-J.Korner

Study of Direct-Reaction Cross Sections in Collisions between Heavy Ions

NUCLEAR REACTIONS 118Sn(18O, 17O), (18O, 16O), (18O, 15N), (18O, 14C), (18O, 13C), (18O, 12C), E=50-62 MeV; 48Ca(16O, X), E=56 MeV; measured σ.

doi: 10.1016/0370-2693(75)90618-8
Citations: PlumX Metrics


1974EI05      Nucl.Phys. A236, 327 (1974)

Y.Eisen, E.Abramson, G.Engler, M.Samuel, U.Smilansky, Z.Vager

Elastic Scattering of 3He and 4He at Incident Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 110,112,113Cd, 128Te(3He, 3He), 90,91Zr, 92,94Mo, 110,111,112,113,114Cd, 128Te(α, α), E=7-17.5 MeV; measured σ(E, θ); deduced optical model parameters, α-scattering systematics. Enriched targets.

doi: 10.1016/0375-9474(74)90258-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0865.


1974KO25      Phys.Rev.Lett. 33, 1611 (1974)

D.G.Kovar, W.Henning, B.Zeidman, Y.Eisen, H.T.Fortune

Measurement of the Reaction 48Ca(16O, 15C)49Ti

NUCLEAR REACTIONS 48Ca(16O, 15C), E=56 MeV; measured σ(E(15C), θ); deduced Q.

doi: 10.1103/PhysRevLett.33.1611
Citations: PlumX Metrics


1972EI04      Nucl.Phys. A187, 219 (1972)

Y.Eisen, Z.Vager

The Incoming Wave Boundary Condition for Elastic Scattering of Heavy Particles at Incident Energies Near the Coulomb Barrier

doi: 10.1016/0375-9474(72)90085-1
Citations: PlumX Metrics


1972EI07      Nucl.Phys. A195, 513 (1972)

Y.Eisen, R.A.Eisenstein, U.Smilansky, Z.Vager

Elastic Scattering of 16O and 18O by Even Ca Isotopes, 52Cr and 62Ni at Incident Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 62Ni, 52Cr, 48,44,40Ca(18O, 18O), 62Ni, 52Cr(16O, 16O), E=25-42 MeV; measured σ(θ, E) at backward angles; deduced differences between 16O, 18O. Enriched targets.

doi: 10.1016/0375-9474(72)91073-1
Citations: PlumX Metrics


1971BE26      Nucl.Phys. A167, 216 (1971)

M.C.Bertin, S.L.Tabor, B.A.Watson, Y.Eisen, G.Goldring

The Elastic Scattering of 16O from Even Ca Isotopes Near the Coulomb Barrier

NUCLEAR REACTIONS 40,44,48Ca(16O, 16O), E=20-40 MeV; measured σ(E;θ). 40,44,48Ca deduced relative nuclear sizes. Enriched targets.

doi: 10.1016/0375-9474(71)90595-1
Citations: PlumX Metrics


1971EI07      Phys.Lett. 37B, 33 (1971)

Y.Eisen

A Combined Microscopic and Phenomenological Approach to the Real Part of the Optical Potential for Heavy Ion Reactions

NUCLEAR REACTIONS 40,42,44,48Ca(16O, 16O), E approx Coulomb barrier; calculated nuclear matter differences in outer regions of nuclei, real part of optical potential.

doi: 10.1016/0370-2693(71)90562-4
Citations: PlumX Metrics


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