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NSR database version of April 26, 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, 96}Zr 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
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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
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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 + ^{148,150,152,154}Sm at Sub-Barrier Energies

NUCLEAR REACTIONS ^{148,150,152,154}Sm(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
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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 ^{148,150,152,154}Sm(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 ^{148,150,152,154}Sm(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 ^{122,124,126,128}Te(α, α), ¹²⁸Te(³He, ³He), E=8-18 MeV; measured σ(θ, E) for ground state, first 2+ state; deduced optical model parameters. ^{122,124,126,128}Te 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, ^{110,111,112,113,114}Cd, 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
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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
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