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NSR database version of May 23, 2024.

Search: Author = C.H.Holbrow

Found 30 matches.

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1994BE60      Nucl.Instrum.Methods Phys.Res. A351, 256 (1994)

J.A.Behr, S.B.Cahn, S.B.Dutta, A.Ghosh, G.Gwinner, C.H.Holbrow, L.A.Orozco, G.D.Sprouse, J.Urayama, F.Xu

A Low-Energy Ion Beam from Alkali Heavy-Ion Reaction Products

NUCLEAR REACTIONS 197Au(18O, xn), E=110-115 MeV; measured Eα, Iα; deduced 209,210,211Fr yield vs target temperature. 51V(31P, n2p), E=90 MeV; 51V(32S, 2n2p), E=145 MeV; measured Eγ, Iγ following residuals decay. Ion beam apparatus for alkali atoms transport.

doi: 10.1016/0168-9002(94)91351-X
Citations: PlumX Metrics


1992BE07      Nucl.Instrum.Methods Phys.Res. A311, 224 (1992)

A.Berger, J.Billowes, J.Das, S.Dutta, G.Gwinner, C.H.Holbrow, T.Kuhl, T.Lauritsen, S.L.Rolston, J.Schecker, G.D.Sprouse, F.Xu

A Resonance Cell for On-Line Optical Spectroscopy of Accelerator Produced Radioactive Atoms

NUCLEAR MOMENTS 174,176,178,180Hf; measured isotope shifts. Resonance fluorescence detection.

RADIOACTIVITY 152,154,156,158Yb; measured isotope shifts. Radioactive beams, resonance cell, on-line optical spectroscopy.

doi: 10.1016/0168-9002(92)90868-5
Citations: PlumX Metrics


1992BE48      Hyperfine Interactions 74, 23 (1992)

J.Behr, S.Cahn, J.Das, G.Gwinner, C.H.Holbrow, T.Lauritsen, L.A.Orozco, S.Shang, J.Schecker, G.D.Sprouse, F.Xu

Laser Spectroscopy of Nuclear Reaction Products: Recent results and future prospects

ATOMIC PHYSICS 174,176,178,180Hf; measured fluorescence spectra. Laser spectroscopy, recoil into gas method. Information on 154,152,156,158Yb included.

doi: 10.1007/BF02398613
Citations: PlumX Metrics


1992HO16      Hyperfine Interactions 74, 119 (1992)

C.H.Holbrow, D.Murnick, R.R.Dasari, M.S.Feld

Studies of Weak Interaction Effects by Laser Spectroscopy of Short-Lived Atoms

RADIOACTIVITY 85mRb(IT); measured γ-anisotropy; deduced weak interaction implications. Sub-Doppler resolution, laser-induced nuclear orientation.


1991HO22      Nucl.Instrum.Methods Phys.Res. B56/57, 528 (1991); see 1991Ho27

C.H.Holbrow, G.D.Sprouse, J.Das, J.Schecker, T.Lauritsen, J.Billowes, A.Berger, F.Xu, W.Kim

Measurements of Isotope Shifts of Accelerator-Produced Radioactive Atoms in an On-Line Resonance Cell

doi: 10.1016/0168-583X(91)96087-2
Citations: PlumX Metrics


1991HO27      Nucl.Instrum.Methods Phys.Res. B56/57, 528 (1991)

C.H.Holbrow, G.D.Sprouse, J.Das, J.Schecker, T.Lauritsen, J.Billowes, A.Berger, F.Xu, W.Kim

Measurements of Isotope Shifts of Accelerator-Produced Radioactive Atoms in an On-Line Resonance Cell

RADIOACTIVITY 152,154,156,157,158Yb [from 154Sm(18O, X), E=107, 108 MeV; 144Sm(16O, X), E=101, 117 MeV; 96Ru(60Ni, X), E=250 MeV; 96Ru(58Ni, X), E=241 MeV]; measured isotope shifts relative to 174Y. Fluorescence spectra, gas filled, liquid nitrogen cooled resonance cell.

NUCLEAR MOMENTS 166,172,176Yb; measured isotope shifts relative to 174Y. Fluorescence spectra, gas filled, liquid nitrogen cooled resonance cell.

NUCLEAR REACTIONS 154Sm(18O, X)166Yb, E=101 MeV; 144Sm(18O, X)158Yb, E=108 MeV; 144Sm(16O, X)157Yb, E=101 MeV; 144Sm(16O, X)156Yb, E=117 MeV; 96Ru(60Ni, X)154Yb, E=250 MeV; 96Ru(58Ni, X)152Yb, E=241 MeV; measured residual production σ.

doi: 10.1016/0168-583X(91)96087-2
Citations: PlumX Metrics


1991MA21      Phys.Rev.Lett. 66, 1681 (1991)

J.Mackin, R.R.Dasari, C.H.Holbrow, J.T.Hutton, D.E.Murnick, M.Otteson, W.W.Quivers, Jr., G.Shimkaveg, M.S.Feld

Sub-Doppler Nuclear Detection of Laser-Induced Orientation of 85mRb

RADIOACTIVITY 85mRb [from 85Kr(β-decay)]; measured Iγ(θ), Doppler changes; deduced hyperfine transitions, isomer shift. 85mRb deduced electric quadrupole moment. Laser-induced nuclear orientation, optical saturation technique, sub-Doppler detection.

doi: 10.1103/PhysRevLett.66.1681
Citations: PlumX Metrics


1990MA61      Hyperfine Interactions 59, 157 (1990)

J.Mackin, J.T.Hutton, M.Otteson, M.S.Feld, R.R.Dasari, C.H.Holbrow, D.E.Murnick, W.W.Quivers, Jr.

Sub-Doppler Resolution Laser-Induced Nuclear Orientation of 85mRb(T1/2 = 1.0 μs)

RADIOACTIVITY 85Kr; measured γ-anisotropy; deduced 85mRb hfs. Sub-Doppler resolution laser induced nuclear orientation, source plus Rb for resonant charge exchange.

doi: 10.1007/BF02401213
Citations: PlumX Metrics


1990SP05      Hyperfine Interactions 59, 91 (1990)

G.D.Sprouse, J.Das, T.Lauritsen, J.Schecker, A.Berger, J.Billowes, C.H.Holbrow, W.Kim, F.Xu

Isotope Shift Measurements and Charge Radii of 152-158Yb

NUCLEAR MOMENTS 172,176Yb; measured isotope shift; deduced rms charge radii change. Other data considered.

RADIOACTIVITY 152,154,156,166Yb [from 144Sm(16O, 4n), (18O, 4n), 96Ru(58Ni, 2p2n), (60Ni, 2p2n)]; measured isotope shift; deduced rms charge radii change. Other data considered.

doi: 10.1007/BF02401197
Citations: PlumX Metrics


1989SP04      Phys.Rev.Lett. 63, 1463 (1989)

G.D.Sprouse, J.Das, T.Lauritsen, J.Schecker, A.Berger, J.Billowes, C.H.Holbrow, H.-E.Mahnke, S.L.Rolston

Laser Spectroscopy of Light Yb Isotopes On-Line in a Cooled Gas Cell

RADIOACTIVITY 166,158Yb [from 154,144Sm(18O, X), E=101, 108 MeV]; 157,156Yb [from 144Sm(16O, X), E=101, 117 MeV]; 154,152Yb [from 96Ru(60Ni, X), (58Ni, X), E=250, 241 MeV]; measured isotope shifts; deduced rms charge radius changes shell structure dependence.

doi: 10.1103/PhysRevLett.63.1463
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1986BI11      Phys.Lett. 178B, 145 (1986)

J.Billowes, C.H.Holbrow, T.Lauritsen, K.P.Lieb, R.G.Pillay, S.L.Rolston, G.D.Sprouse

g Factor above the First Backbend in 168W

NUCLEAR REACTIONS 110Pd(61Ni, 3n), E=255 MeV; measured γn-coin, γγ(θ, H). 168W deduced yrast band g factors, configuration. IMPAC technique.

doi: 10.1016/0370-2693(86)91485-1
Citations: PlumX Metrics


1984SH24      Phys.Rev.Lett. 53, 2230 (1984)

G.Shimkaveg, W.W.Quivers, Jr., R.R.Dasari, C.H.Holbrow, P.G.Pappas, M.Attili, J.E.Thomas, D.E.Murnick, M.S.Feld

Laser-Induced Nuclear Orientation of 1-μs 85mRb

RADIOACTIVITY 85mRb [from 85Kr(β-decay)]; measured γ anisotropy, oriented nuclei; deduced atomic D1 state hfs. 85mRb deduced μ, isomer shift. Laser induced nuclear orientation.

doi: 10.1103/PhysRevLett.53.2230
Citations: PlumX Metrics


1974HO06      Phys.Rev. C9, 902 (1974)

C.H.Holbrow, H.G.Bingham, R.Middleton, J.D.Garrett

Identification of Analog Pairs in 13C and 13N by Means of the 10B(6Li, 3He)13C and 10B(6Li, t)13N Reactions

NUCLEAR REACTIONS 10B(6Li, t), (6Li, 3He), E=18 MeV; measured σ(Et, θ), σ(E(3He), θ). 13N, 13C deduced levels, J, π.

doi: 10.1103/PhysRevC.9.902
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1971FO05      Phys.Rev. C3, 1441 (1971)

H.T.Fortune, R.Middleton, J.D.Garrett, C.H.Holbrow

Distorted-Wave Analysis of the 13C(3He, d) Reaction Leading to Unbound Levels of 14N

NUCLEAR REACTIONS 13C(3He, d), E not given; measured nothing; analyzed σ(θ). 14N levels deduced level-width, S.

doi: 10.1103/PhysRevC.3.1441
Citations: PlumX Metrics


1969HO23      Phys.Rev. 183, 880 (1969)

C.H.Holbrow, R.Middleton, W.Focht

Study of 14N by Several Transfer Reactions

NUCLEAR REACTIONS 13C(3He, d), E=15 MeV; 12C(3He, p), E=15 MeV; 15N(3He, α), E=15 MeV; 16O(d, α), E=11 MeV; measured σ(Ed, θ), σ(Ep, θ), σ(Eα, θ). 14N deduced levels, L, π.

doi: 10.1103/PhysRev.183.880
Citations: PlumX Metrics


1969PO11      Phys.Rev. 186, 966 (1969)

L.M.Polsky, C.H.Holbrow, R.Middleton

Nuclear Structure of F18

NUCLEAR REACTIONS 17O(3He, d), 16O(3He, p), E = 15 MeV; 20Ne(d, α), E = 11 MeV; measured σ(Ed, θ), σ(Ep, θ). 18F deduced levels, J, π, L, T, S.

doi: 10.1103/PhysRev.186.966
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1968MI09      Phys.Rev.Letters 21, 1398 (1968)

R.Middleton, L.M.Polsky, C.H.Holbrow, K.Bethge

Hole-Particle States in 18F

NUCLEAR REACTIONS 14N(7Li, t), E=15 MeV; measured σ(Et). 18F deduced levels, J, π.

doi: 10.1103/PhysRevLett.21.1398
Citations: PlumX Metrics


1967HO02      Nucl.Phys. A91, 551(1967)

C.H.Holbrow, B.Rosner

Investigation of States of 39Ar by the 38Ar(d, p)39Ar Reaction

NUCLEAR REACTIONS 38Ar(d, p), E = 11 MeV; measured σ(Ep, θ). 39Ar deduced levels, J, π, L. Enriched target.

doi: 10.1016/0375-9474(67)90574-X
Citations: PlumX Metrics


1967RO04      Phys.Rev. 154, 1080 (1967)

B.Rosner, C.H.Holbrow

Nuclear-Structure Studies of Co55 and Co57 by Means of the Fe54, 56(He3, d) Reaction

NUCLEAR STRUCTURE 57Co, 55Co; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.154.1080
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1966BO23      Nucl.Phys. 88, 689 (1966)

R.R.Borchers, R.M.Wood, C.H.Holbrow

Continuous Neutron Spectra from (p, n) Reactions

NUCLEAR REACTIONS 89Y, 93Nb, 115In, 139La, 141Pr, 181Ta, 197Au(p, n), E = 8-14 MeV; measured σ(E;En, θ(n)); deduced level densities. Natural targets.

doi: 10.1016/0029-5582(66)90424-X
Citations: PlumX Metrics


1966HE10      Nucl.Phys. 88, 561(1966)

P.V.Hewka, C.H.Holbrow, R.Middleton

Nuclear Structure of 16N

NUCLEAR REACTIONS 14N(t, p), E = 11.95 MeV; 15N(d, p), 18O(d, α), E = 11.98 MeV; measured σ(θ, Ep), σ(θ, Eα), Q. 16N deduced levels, J, π, L, level-width. Enriched targets.

doi: 10.1016/0029-5582(66)90415-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2079.


1966HO03      Nucl.Phys. 79, 505(1966)

C.H.Holbrow, P.V.Hewka, J.Wiza, R.Middleton

Level Structure of 37Ar and 41Ar

NUCLEAR REACTIONS 36Ar(d, p), 40Ar(d, p), E = 11 MeV; measured σ(Ep), Q. 37Ar, 41Ar deduced levels. Enriched targets.

doi: 10.1016/0029-5582(66)90259-8
Citations: PlumX Metrics


1966HO15      Phys.Rev. 152, 970 (1966)

C.H.Holbrow, R.Middleton, B.Rosner

Study of 14N by the Reaction 13C(3He, D)14N

NUCLEAR STRUCTURE 14N, 13C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.152.970
Citations: PlumX Metrics


1966RO13      Isobaric Spin in Nucl.Phys., J.D.Fox and D.Robson, Eds., Academic Press, p.595 (1966)

B.Rosner, C.H.Holbrow, D.J.Pullen

Analogue States in Co55, 57 and Cu59, 61 Excited by (He3, d) Reactions

NUCLEAR STRUCTURE 59Cu, 57Co, 61Cu, 55Co; measured not abstracted; deduced nuclear properties.


1965HE02      Bull.Am.Phys.Soc. 10, No.1, 39, CD3 (1965)

P.V.Hewka, J.Wiza, C.H.Holbrow

Energy Levels of Ar41

NUCLEAR STRUCTURE 41Ar; measured not abstracted; deduced nuclear properties.


1965WI02      Bull.Am.Phys.Soc. 10, No.1, 39, CD2 (1965)

J.L.Wiza, P.V.Hewka, C.H.Holbrow

Energy Levels of Ar37

NUCLEAR STRUCTURE 37Ar; measured not abstracted; deduced nuclear properties.


1963PO02      Phys.Rev. 129, 733 (1963)

C.H.Poppe, C.H.Holbrow, R.R.Borchers

Neutrons from D + T and D + H

NUCLEAR STRUCTURE 1H, 3H; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.129.733
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1090.


1962OV01      Bull.Am.Phys.Soc. 7, No.7, 471, LA5 (1962)

J.C.Overley, C.H.Holbrow

B10(d, n)C11 Reaction

NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.


1962PO13      Bull.Am.Phys.Soc. 7, 350, WA11 (1962)

C.H.Poppe, C.H.Holbrow, R.R.Borchers, B.Hoop

Neutrons from D+T and D+H

NUCLEAR REACTIONS 1,3H(d, X)1NN, E=5-12 MeV; measured reaction products, En, In, TOF; deduced σ(θ), neutron spectra.


1961BO17      Bull.Am.Phys.Soc. 6, No.5, 429, J3 (1961)

R.R.Borchers, C.H.Poppe, C.H.Holbrow

Neutrons from Proton Bombardment of Lithium

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.


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