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NSR database version of April 11, 2024.

Search: Author = C.K.Hargrove

Found 20 matches.

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2004BL02      Nucl.Instrum.Methods Phys.Res. A517, 139 (2004)

I.Blevis, J.Boger, E.Bonvin, B.T.Cleveland, X.Dai, F.Dalnoki-Veress, G.Doucas, J.Farine, H.Fergani, D.Grant, R.L.Hahn, A.S.Hamer, C.K.Hargrove, H.Heron, P.Jagam, N.A.Jelley, C.Jillings, A.B.Knox, H.W.Lee, I.Levine, M.Liu, S.Majerus, A.McDonald, K.McFarlane, C.Mifflin, A.J.Noble, S.Noel, V.M.Novikov, J.K.Rowley, M.Shatkay, J.J.Simpson, D.Sinclair, B.Sur, J.-X.Wang, M.Yeh, X.Zhu

Measurement of 222Rn dissolved in water at the Sudbury Neutrino Observatory

RADIOACTIVITY 222Rn(α); measured Eα, Iα, contribution to detector background.

doi: 10.1016/j.nima.2003.10.103
Citations: PlumX Metrics


1999HA46      Phys.Rev. C60, 034608 (1999)

C.K.Hargrove, D.J.Paterson, I.S.Batkin

Measurement of the Screening Potential in 3H β Decay

RADIOACTIVITY 3H(β-); measured β spectra; deduced electron screening potential. Gas proportional chamber technique. Comparison with model predictions.

doi: 10.1103/PhysRevC.60.034608
Citations: PlumX Metrics


1995HA49      Nucl.Instrum.Methods Phys.Res. A357, 157 (1995)

C.K.Hargrove, I.Blevis, D.Paterson, E.D.Earle

Use of Gd in Gas Counters as Neutron Detectors in SNO

NUCLEAR REACTIONS Gd(n, γ), E=reactor; measured I(ce) following neutron capture; deduced proportional wire chamber characteristics, applicability to solar neutrino studies. Gd(n, X), E=reactor; calculated γ-spectra Monte Carlo simulation.

doi: 10.1016/0168-9002(94)01520-1
Citations: PlumX Metrics


1984NA01      Phys.Rev.Lett. 52, 105 (1984)

I.Navon, M.J.Leitch, D.A.Bryman, T.Numao, P.Schlatter, G.Azuelos, R.Poutissou, R.A.Burnham, M.Hasinoff, J.M.Poutissou, J.A.Macdonald, J.E.Spuller, C.K.Hargrove, H.Mes, M.Blecher, K.Gotow, M.Moinester, H.Baer

Pion Double Charge Exchange at 50 MeV on 14C

NUCLEAR REACTIONS 14C(π+, π-), E=50 MeV; measured σ(θ), σ(E(π)). 14O deduced double analog, strong nonanalog state excitation.

doi: 10.1103/PhysRevLett.52.105
Citations: PlumX Metrics


1983CA09      Phys.Lett. 124B, 465 (1983)

A.L.Carter, C.R.Cox, M.S.Dixit, G.W.Dodson, M.Eckhause, C.K.Hargrove, E.P.Hincks, J.R.Kane, H.Mes, A.M.Rushton, R.T.Siegel, R.E.Welsh

Search for Two-Photon Emission from 2S States of Low-Z Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms Li, Be, B, N, O; measured metastable 2S-state yield; deduced two γ-emission quenching, possible mechanisms. Metal, hydrid, gas targets.

doi: 10.1016/0370-2693(83)91552-6
Citations: PlumX Metrics


1979LE13      Nucl.Phys. A322, 397 (1979)

M.Leon, J.N.Bradbury, P.A.M.Gram, R.L.Hutson, M.E.Schillaci, C.K.Hargrove, J.J.Reidy

Observation of the E2 Nuclear Resonance Effect in Some Pionic Atoms

ATOMIC PHYSICS, Fission 48,50Ti, 104,101Ru, 110,108Pd, 112,111,110Cd, 150,152Sm(π-, X-ray), E=at rest; measured I(X-ray); deduced attenuation due to nuclear E2 resonance effect.

doi: 10.1016/0375-9474(79)90434-2
Citations: PlumX Metrics


1976CA26      Phys.Rev.Lett. 37, 1380 (1976)

A.L.Carter, M.S.Dixit, M.K.Sundaresan, J.S.Wadden, P.J.S.Watson, C.K.Hargrove, E.P.Hincks, R.J.McKee, H.Mes, H.L.Anderson, A.Zehnder

New Determination of the π- Mass from Pionic-Atom Transition Energies

doi: 10.1103/PhysRevLett.37.1380
Citations: PlumX Metrics


1975KE05      Phys.Rev. C11, 1719 (1975)

D.Kessler, H.Mes, A.C.Thompson, H.L.Anderson, M.S.Dixit, C.K.Hargrove, R.J.McKee

Muonic X Rays in Lead Isotopes

ATOMIC PHYSICS, Mesic-Atoms 204,206,207,208Pb(μ-, X-ray), E approx 0; measured muonic transition energies, L-linewidth. 204,206,207,208Pb deduced nuclear polarization, Fermi parameters, anomalous fs splitting, isotope shift.

doi: 10.1103/PhysRevC.11.1719
Citations: PlumX Metrics


1971DI16      Phys.Rev.Lett. 27, 878 (1971)

M.S.Dixit, H.L.Anderson, C.K.Hargrove, R.J.McKee, D.Kessler, H.Mes, A.C.Thompson

Experimental Test of the Theory of Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms Ca, Ti, Fe, Sr, Ag, Cd, Sn, Ba, Pb; measured μ-mesic E(X-ray).

doi: 10.1103/PhysRevLett.27.878
Citations: PlumX Metrics


1971MC08      Nucl.Instrum.Methods 92, 421 (1971)

R.J.McKee, C.K.Hargrove, A.G.Smith, H.Mes, A.Thompson, M.Dixit

Precise Calibration of a Ge(Li)-Spectrometer Using a Digital to Analog Converter

RADIOACTIVITY 57Co; measured Eγ. Ge(Li) detector.

doi: 10.1016/0029-554X(71)90419-8
Citations: PlumX Metrics


1970KE20      Can.J.Phys. 48, 3029 (1970)

D.Kessler, R.J.McKee, C.K.Hargrove, E.P.Hincks, H.L.Anderson

Muonic X Rays and Capture γ Rays in 89Y

ATOMIC PHYSICS, Mesic-Atoms 89Y; measured μ-mesic X-ray spectra; deduced nuclear charge distribution.

NUCLEAR REACTIONS 89Y(μ-, X), E approx o; measured Eγ. 86,87,88,89Sr deduced transitions.

doi: 10.1139/p70-376
Citations: PlumX Metrics


1969AN02      Phys.Rev.Lett. 22, 221 (1969)

H.L.Anderson, C.K.Hargrove, E.P.Hincks, J.D.McAndrew, R.J.McKee, D.Kessler

Muonic X Rays in Pb206 and Possible Observation of Nuclear Polarization

ATOMIC PHYSICS, Mesic-Atoms 206Pb; measured muonic X-rays; deduced nuclear polarization.

doi: 10.1103/PhysRevLett.22.221
Citations: PlumX Metrics


1969AN26      Phys.Rev. 187, 1565 (1969)

H.L.Anderson, C.K.Hargrove, E.P.Hincks, J.D.McAndrew, R.J.McKee, R.D.Barton, D.Kessler

Precise Measurement of the Muonic X Rays in the Lead Isotopes

NUCLEAR REACTIONS 206,207,208Pb(μ-, xnγ), E ≈ 0; measured Eγ, Iγ. 203,205,206Tl deduced transitions. 206,207,208Pb; measured muonic X-ray spectra; deduced isotope shift, nuclear charge distributions.

doi: 10.1103/PhysRev.187.1565
Citations: PlumX Metrics


1969HA24      Phys.Rev.Letters 23, 215 (1969)

C.K.Hargrove, E.P.Hincks, G.R.Mason, R.J.McKee, D.Kessler, S.Ricci

Neutron Emission from Nuclear Excitation by Radiationless Transitions in μ-Atomic Bi209

ATOMIC PHYSICS, Mesic-Atoms 209Bi; measured neutron emission in radiationless transitions.

doi: 10.1103/PhysRevLett.23.215
Citations: PlumX Metrics


1967EH01      Phys.Rev.Letters 18, 959 (1967)

R.D.Ehrlich, D.Fryberger, D.A.Jensen, C.Nissim-Sabat, R.J.Powers, V.L.Telegdi, C.K.Hargrove

Precise Measurements of Muonic Isotope Shifts for 29 Nuclides, in Particular, for the Ca Isotopes 40, 42, 44, and 48

NUCLEAR STRUCTURE Ni, Si, Zr, K, Sr, Fe, Cu, Ca, Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.18.959
Citations: PlumX Metrics


1966HA43      Phys.Can. 22, No.2, 15, 3.12 (1966)

C.K.Hargrove, E.P.Hincks, H.L.Anderson, R.J.McKee

Hyperfine Structure of Mu-Atomic Transitions in Au

NUCLEAR STRUCTURE, Mesic-Atoms 197Au; measured not abstracted; deduced nuclear properties.


1963HA08      Nucl.Phys. 40, 566 (1963)

C.K.Hargrove, K.W.Geiger, A.Chatterjee

The Decay of 131I

NUCLEAR STRUCTURE 131I; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90303-1
Citations: PlumX Metrics


1962HA04      Phys.Can. 18, No.3, 19, 4.6 (1962)

C.K.Hargrove, K.W.Geiger, A.Chatterjee

Weak Transitions Associated with the Decay of I131 (8.06 Days)

NUCLEAR STRUCTURE 131I; measured not abstracted; deduced nuclear properties.


1962HA26      Can.J.Phys. 40, 964 (1962)

C.K.Hargrove, W.M.Martin

Short-Lived Isomeric States of Polonium

NUCLEAR STRUCTURE 205Po, 207Po; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p62-102
Citations: PlumX Metrics


1960HA23      Bull.Am.Phys.Soc. 5, No.5, 338, A5 (1960)

C.K.Hargrove, W.M.Martin

New Isomers in Polonium

NUCLEAR STRUCTURE 207Po, 205Po; measured not abstracted; deduced nuclear properties.


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