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NSR database version of April 27, 2024.

Search: Author = R.A.Esterlund

Found 25 matches.

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1998KR08      Appl.Radiat.Isot. 49, 981 (1998)

A.Kronenberg, K.Siemon, R.Weber, R.A.Esterlund, P.Patzelt

Determination of the Half-Life of 105mRh

RADIOACTIVITY 105mRh(IT); measured T1/2.

doi: 10.1016/S0969-8043(97)10097-5
Citations: PlumX Metrics

1996GO47      Radiochim.Acta 73, 105 (1996)

D.Gogrewe, M.Putz, R.Weber, K.Siemon, R.A.Esterlund, P.Patzelt

Determination of 210Pb via 210Bi using a Hydride Generation Technique Combined with β-Spectrometry

RADIOACTIVITY 210Pb(β-); 210Bi(β-), (α) [from 210Pb(β-decay)]; measured 210Bi count rate vs 210Pb initial activity; deduced 210Pb content determination. Hydride generation technique, β-spectrometry.

1994VA13      Appl.Radiat.Isot. 45, 419 (1994)

J.Van Aarle, W.Westmeier, R.A.Esterlund, P.Patzelt

227Ac: A suggested long-lived multiple-line gamma-ray calibration standard

RADIOACTIVITY 227Ac(β-), (α); measured Eγ, Iγ, E X-ray, I X-ray; deduced relative emission probabilities.

doi: 10.1016/0969-8043(94)90105-8
Citations: PlumX Metrics

1994VA24      Nucl.Phys. A578, 77 (1994)

J.van Aarle, W.Westmeier, R.A.Esterlund, P.Patzelt

252Cf: Neutron multiplicities in correlation with fission-fragment mass and energy

RADIOACTIVITY 252Cf(SF); measured neutron multiplicities following SF-decay, total kinetic energies; deduced fission decay modes. Multi-modal random neck-rupture model.

doi: 10.1016/0375-9474(94)90970-9
Citations: PlumX Metrics

1992BE19      Phys.Lett. 286B, 225 (1992)

S.Beiersdorf, R.A.Esterlund, M.Knaack, W.Westmeier, P.Patzelt, F.P.Hessberger, V.Ninov, A.Luttgen

Evaporation Residues at E(*) ≈ 400 MeV

NUCLEAR REACTIONS 104Ru(86Kr, X), E=11.4 MeV/nucleon; measured evaporation residue total yield, mass yield distributions, σ(θ) for X=145,147Eu, 146,149Gd, 151,153,155Tb, 157Dy, 160Er. Bohr-Wheeler fission-evaporation model.

doi: 10.1016/0370-2693(92)91766-3
Citations: PlumX Metrics

1992SI17      Appl.Radiat.Isot. 43, 873 (1992)

K.Siemon, R.A.Esterlund, J.Van Aarle, M.Knaack, W.Westmeier, P.Patzelt

A New Measurement of the Gamma-Ray Intensities of 234mPa Accompanying the Decay of 238U

RADIOACTIVITY 234mPa(β-) [from 238U(α) decay chain]; measured Eγ, Iγ. 234U deduced transitions absolute Iγ.

doi: 10.1016/0883-2889(92)90149-9
Citations: PlumX Metrics

1991JA07      Z.Phys. A339, 475 (1991)

B.Jackel, A.Rox, R.A.Esterlund, W.Westmeier, M.Knaack, P.Patzelt

Mass and Charge Flow in the Reaction 7.1 MeV/u 197Au + 63Cu

NUCLEAR REACTIONS 63Cu(197Au, X), E=7.1 MeV/nucleon; measured σ(fragment θ), mass yield; deduced fusion σ, different mechanisms contributions.

1989SC32      Phys.Lett. 232B, 37 (1989)

H.Schulte, B.Jackel, R.A.Esterlund, M.Knaack, W.Westmeier, A.Rox, P.Patzelt

Dynamic Contributions to Symmetric Fragmentation Processes

NUCLEAR REACTIONS 197Au(40Ar, X), (40Ar, F), E=5.3, 7.5 MeV/nucleon; measured fission, fission like fragment σ(θ), anisotropy; deduced fragmentation mechanism.

doi: 10.1016/0370-2693(89)90554-6
Citations: PlumX Metrics

1985ES01      Nucl.Phys. A435, 597 (1985)

R.A.Esterlund, W.Westmeier, U.Reus, A.M.Habbestad Watzig, P.Patzelt

Fusion-Like Processes and the Concept of Dynamic Equivalence: The system 132Xe + (nat)Fe

NUCLEAR REACTIONS Fe(132Xe, X), E=4.56-7.12 MeV/nucleon; measured σ(fragment A) vs E, fragment chain yield vs charge, mass yield vs mass number; deduced symmetric fragmentation σ, quasielastic transfer σ, evaporation σ, deep inelastic transfer σ, model parameters. Dynamic capture model.

doi: 10.1016/0375-9474(85)90479-8
Citations: PlumX Metrics

1984WE07      Z.Phys. A316, 27 (1984)

W.Westmeier, R.A.Esterlund

Particle-to-Fission Competition at High Excitation Energies

NUCLEAR REACTIONS, ICPND 182W(12C, F), (12C, p)(12C, α), E=70-170 MeV; 154Sm(40Ar, F), (40Ar, p), (40Ar, α), E=200-350 MeV; calculated fission, reaction σ(E). 181Ta(19F, F), E=105-125 MeV; 165Ho(20Ne, F), E=292 MeV; calculated pre-scission neutron multiplicity following 200Pb, 185Ir fission; deduced particle evaporation, collective motion towards scission relative times. Phenomenological model.

doi: 10.1007/BF01415657
Citations: PlumX Metrics

1982WE13      Phys.Lett. 117B, 163 (1982)

W.Westmeier, R.A.Esterlund, A.Rox, P.Patzelt

Further Evidence for ' Extra Push '

NUCLEAR REACTIONS Fe(132Xe, X), E(cm)=160-280 MeV; 238U(56Fe, X), E(cm)=250-440 MeV; calculated σ(fusion) vs E; deduced reaction mechanism. Phenomenological capture model.

doi: 10.1016/0370-2693(82)90538-X
Citations: PlumX Metrics

1981RE08      Z.Phys. A301, 363 (1981)

U.Reus, W.Westmeier, R.A.Esterlund, A.Rox, M.Rajagopalan, P.Patzelt

Evolution from Quasielastic to Deep-Inelastic Transfer in the System 132Xe + Fe(nat)

NUCLEAR REACTIONS Fe(132Xe, X), E=5.9 MeV/nucleon; measured σ(fragment θ), σ(fragment mass, Z); deduced deep inelastic to quasielastic process transition in production of 127,129,132Cs, 121,124,130I. Radiochemical procedure, catcher-foil technique.

doi: 10.1007/BF01421703
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1981WE04      Z.Phys. A299, 277 (1981)

W.Westmeier, U.Reus, R.A.Esterlund, J.Gilat, P.Patzelt

Search for a New Reaction Mechanism in the System 132Xe + (nat)Fe

NUCLEAR REACTIONS Fe(132Xe, X), E=5, 5.9, 7.15 MeV/nucleon; measured independent, cumulative production σ for mass 93-97, deep inelastic product to symmetric mass yield ratios; deduced no new mechanism. Thin targets.

doi: 10.1007/BF01443946
Citations: PlumX Metrics

1977ES01      Phys.Rev. C15, 319 (1977)

R.A.Esterlund, D.Molzahn, R.Brandt, P.Patzelt, P.Vater, A.H.Boos, M.R.Chandratillake, I.S.Grant, J.D.Hemingway, G.W.A.Newton

Search for Long-Lived Superheavy Elements in the Reaction System 238U + 9.6-MeV/Nucleon 63,65Cu

NUCLEAR REACTIONS 238U(63Cu, X), (65Cu, X), E=9.6 MeV/nucleon; measured σ for production of superheavy elements, 254Cf.

doi: 10.1103/PhysRevC.15.319
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1977RE09      Phys.Rev.Lett. 39, 171 (1977)

U.Reus, A.M.H.Watzig, R.A.Esterlund, P.Patzelt, I.S.Grant

Mass-Yield Distributions in the Reaction of 56Fe Ions with 238U

NUCLEAR REACTIONS 238U(56Fe, X), E=538 MeV; measured σ(A), quasielastic transfer, quasifission, fusion-fission σ.

doi: 10.1103/PhysRevLett.39.171
Citations: PlumX Metrics

1972ES01      Nucl.Phys. A179, 645 (1972)

R.A.Esterlund, A.F.Stehney, E.P.Steinberg

Secondary Nuclear Reactions of 11.5 GeV Protons on Uranium: A Search for the Production of Transcurium Actinide Elements

NUCLEAR REACTIONS 238U(p, X)254Fm/256Fm, E=11.5 GeV; measured activities; deduced upper limits for σ of secondary products.

doi: 10.1016/0375-9474(72)90609-4
Citations: PlumX Metrics

1967ES02      Phys.Rev. 156, 1094 (1967)

R.A.Esterlund, R.McPherson, A.M.Poskanzer, P.L.Reeder

Beta-Delayed Protons from Ne17

NUCLEAR STRUCTURE 17Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.156.1094
Citations: PlumX Metrics

1966ES04      BNL-10520 (1966)

R.A.Esterlund, R.McPherson, A.M.Poskanzer, P.L.Reeder

Beta-Delayed Protons from Ne17

NUCLEAR STRUCTURE 17Ne; measured not abstracted; deduced nuclear properties.

1966PO12      Phys.Rev. 152, 995 (1966)

A.M.Poskanzer, R.McPherson, R.A.Esterlund, P.L.Reeder

Beta-Delayed Protons from Ar33, Ca37, and Ti41

NUCLEAR STRUCTURE 41Ti, 37Ca, 33Ar; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.152.995
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1966RE07      Phys.Rev. 147, 781 (1966)

P.L.Reeder, A.M.Poskanzer, R.A.Esterlund, R.McPherson

Beta-Delayed Protons from Si25

NUCLEAR STRUCTURE 25Si; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.147.781
Citations: PlumX Metrics

1966RE15      Phys.Rev. 147, 781 (1966)

P.L.Reeder, A.M.Poskanzer, R.A.Esterlund, R.McPherson

Beta-Delayed Protons from Si25

RADIOACTIVITY 25Si(β+) [from 24Mg(3He, 2n), E=32 MeV]; measured β-delayed Ep, Ip, logft. 25Al; deduced levels, J, π.

doi: 10.1103/PhysRev.147.781
Citations: PlumX Metrics

1965ES03      Nucl.Phys. 69, 401 (1965)

R.A.Esterlund, B.D.Pate

Analysis of excitation functions via the compound statistical model

NUCLEAR REACTIONS 92Mo(α, n), 92Mo(α, p), 100Mo(α, n), E=6.8-27.8 MeV; measured products, 95Ru, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry R0048.

doi: 10.1016/0029-5582(65)90059-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetR0048.

1965MC09      Phys.Rev. 140, B1513 (1965)

R.McPherson, R.A.Esterlund, A.M.Poskanzer, P.L.Reeder

Oxygen-13

NUCLEAR STRUCTURE 13O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B1513
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1965PO06      Phys.Rev.Letters 15, 1030 (1965)

A.M.Poskanzer, R.A.Esterlund, R.McPherson

Decay of He8

NUCLEAR STRUCTURE 8He; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.15.1030
Citations: PlumX Metrics

1964RE08      Phys.Rev.Letters 13, 767 (1964)

P.L.Reeder, A.M.Poskanzer, R.A.Esterlund

New Delayed-Proton Emitters: Ti41, Ca37, and Ar33

NUCLEAR STRUCTURE 33Ar, 37Ca, 41Ti; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.13.767
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