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NSR database version of April 27, 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 ^{204,206,207,208}Pb(μ^-, X-ray), E approx 0; measured muonic transition energies, L-linewidth. ^{204,206,207,208}Pb 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.