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Search: Author = C.M.Jones

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1987OL01      Nucl.Instrum.Methods Phys.Res. A254, 1 (1987)

D.K.Olsen, K.A.Erb, C.M.Jones, W.T.Milner, D.C.Weisser, N.F.Ziegler

Calibration of the HHIRF Tandem Accelerator Energy-Analyzing Magnet

NUCLEAR REACTIONS 12C(16O, α), E=27.3 MeV; measured σ(Eα). Energy analyzing magnet.

doi: 10.1016/0168-9002(87)90474-8
Citations: PlumX Metrics


1986HA02      Phys.Rev. A33, 914 (1986)

J.Hall, P.Richard, P.L.Pepmiller, D.C.Gregory, P.D.Miller, C.D.Moak, C.M.Jones, G.D.Alton, L.B.Bridwell, C.J.Sofield

Energy Systematics of Single and Double K-Shell-Vacancy Production in Titanium Bombarded by Chlorine Ions

NUCLEAR REACTIONS Ti(37Cl, X), E=6.88 MeV/nucleon; measured E K(X-ray), I K(X-ray); deduced single, double K-shell vacancy production σ.

doi: 10.1103/PhysRevA.33.914
Citations: PlumX Metrics


1977JO01      Phys.Rev. C15, 196 (1977)

C.H.Johnson, J.K.Bair, C.M.Jones, S.K.Penny, D.W.Smith

p-Wave Size Resonances Observed by the (p, n) Reaction for 2.6- to 7-MeV Protons Incident on Isotopes of Sn

NUCLEAR REACTIONS 117,118,119,120,122,124Sn(p, n), E=2.6-7 MeV; measured total σ, σ(E). 118,119,120,121,123,125Sb deduced resonances. Statistical, optical model analysis.

doi: 10.1103/PhysRevC.15.196
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0119.


1977JO03      Phys.Rev. C15, 915 (1977)

C.H.Johnson, J.K.Bair, C.M.Jones

Thresholds for 116Sn(p, n) and 118Sn(p, n)

NUCLEAR REACTIONS 116,118Sn(p, n), E ≈ threshold; measured thick target integrated σ; deduced Q.

doi: 10.1103/PhysRevC.15.915
Citations: PlumX Metrics


1976RO15      Phys.Rev. C14, 2126 (1976)

R.L.Robinson, J.K.Bair, C.H.Johnson, P.H.Stelson, W.B.Dress, C.M.Jones

Cross Sections for the Ni, Cu, Zn(16,18O, xn) Reactions Near the Coulomb Barrier

NUCLEAR REACTIONS 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn(16O, xn), (18O, xn), E=36-55 MeV; measured total σ(E).

doi: 10.1103/PhysRevC.14.2126
Citations: PlumX Metrics


1972HO28      Nucl.Phys. A190, 362 (1972)

J.L.Horton, C.L.Hollas, P.J.Riley, S.A.S.Zaidi, C.M.Jones, J.L.C.Ford, Jr.

The 90Zr(d, n)91Nb and 96Zr(d, n)97Nb Reactions

NUCLEAR REACTIONS 90Zr(d, n)91Nb, 96Zr(d, n)97Nb, E=12 MeV; measured σ(En, θ). 91Nb, 97Nb levels deduced angular momentum transfer values, S.

doi: 10.1016/0375-9474(72)90147-9
Citations: PlumX Metrics


1971RI12      Phys.Rev. C4, 1864 (1971)

P.J.Riley, J.L.Horton, C.L.Hollas, S.A.A.Zaidi, C.M.Jones, J.L.C.Ford, Jr.

Spectroscopy of 93,95,97Tc through the (d, n) Reaction

NUCLEAR REACTIONS 92,94,96Mo(d, n), E=12 MeV; measured σ(En, θ). 93,95,97Tc deduced levels, J, π, L(p), S.

doi: 10.1103/PhysRevC.4.1864
Citations: PlumX Metrics


1971TH03      Phys.Rev. C3, 1065 (1971)

S.T.Thornton, C.M.Jones, J.K.Bair, M.D.Mancusi, H.B.Willard

Test of Time-Reversal Invariance in the Reactions 16O(d, α)14N and 14N(α, d)16O

NUCLEAR REACTIONS 16O(d, α), E=3.6-5.3 MeV; 14N(α, d), 8.5-10 MeV; measured σ(E;θ); deduced consistency with detailed balance.

doi: 10.1103/PhysRevC.3.1065
Citations: PlumX Metrics


1970JO25      Phys.Rev. C2, 2113 (1970)

C.M.Jones, J.L.C.Ford, Jr., F.E.Obenshain, M.Reeves III

Search for Parity Nonconservation in the Force between Nucleons

RADIOACTIVITY 16N; measured β-delayed α-spectrum. 16O level deduced no parity-forbidden α-decay.

doi: 10.1103/PhysRevC.2.2113
Citations: PlumX Metrics


1970MO11      Phys.Rev. C1, 1100 (1970)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

Isobaric Analog Resonances in Proton Inelastic Scattering from 136Xe

NUCLEAR REACTIONS 136Xe(p, p'), E=9.77-12.89 MeV; measured σ(E;Ep', θ). 137Cs deduced isobaric analog resonances, level-width, S. 136Xe deduced levels, J, π, configurations.

doi: 10.1103/PhysRevC.1.1100
Citations: PlumX Metrics


1970ZA09      Phys.Rev.Lett. 25, 1503 (1970)

S.A.A.Zaidi, C.L.Hollas, J.L.Horton, P.J.Riley, J.L.C.Ford, Jr., C.M.Jones

Anomalies in the Cross Sections of (d, n) Reactions Leading to Isobaric Analog States

NUCLEAR REACTIONS 92,94,96Mo, 96Zr(d, n), E=12 MeV; measured σ(En, θ). 93,95,97Tc, 97Nb deduced isobaric analog states, S.

doi: 10.1103/PhysRevLett.25.1503
Citations: PlumX Metrics


1969KI14      Phys.Rev. 186, 1110 (1969)

H.J.Kim, J.K.Bair, C.M.Jones, H.B.Willard

Elastic and Inelastic Scattering of Protons from Krypton

NUCLEAR REACTIONS Kr(p, p), (p, p'), E = 3.6-5.4 MeV; measured σ(E;Ep', θ); deduced Q. 83,84,85Rb deduced resonances, J, π, isobaric analogs.

doi: 10.1103/PhysRev.186.1110
Citations: PlumX Metrics


1969MO02      Phys.Rev.Letters 22, 356(1969)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

Neutron Particle-Hole States Observed by Inelastic Proton Scattering from 136Xe

NUCLEAR REACTIONS 136Xe(p, p'), E=9.8-13.0 MeV; measured σ(E; Ep', θ). 137Cs deduced resonances, S, isobaric analog. 136Xe deduced levels J, π.

doi: 10.1103/PhysRevLett.22.356
Citations: PlumX Metrics


1969MO14      Phys.Rev. 180, 1213 (1969)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

Isobaric Analog Resonances in Proton Elastic Scattering from 136Xe

NUCLEAR REACTIONS 136Xe(p, p), E=9.77-12.98 MeV; measured σ(E;Ep). 137Cs deduced resonances, level-width, L(p), S. Deduced 137Cs-137Xe Coulomb energy difference. Enriched target.

doi: 10.1103/PhysRev.180.1213
Citations: PlumX Metrics


1969WE02      Phys.Rev. 179, 1047 (1969); Erratum Phys.Rev. C1, 367 (1970)

M.L.West, C.M.Jones, J.K.Bair, H.B.Willard

Level Structure in 15O from the Proton Bombardment of 14N

NUCLEAR REACTIONS 14N(p, p), (p, p'), (p, α), E=3.7-5.7 MeV; measured σ(E), σ(θ). 15O deduced resonances, J, π, level-width, L(p).

doi: 10.1103/PhysRev.179.1047
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1513.


1968MO21      Phys.Rev. 175, 1516 (1968)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

136Xe(d, p) and 136Xe(d, t) Reactions

NUCLEAR STRUCTURE 135Xe, 137Xe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1516
Citations: PlumX Metrics


1967MA37      Phys.Rev.Letters 19, 1449 (1967)

M.D.Mancusi, C.M.Jones, J.B.Ball

Search for Excited States in 3He

NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.19.1449
Citations: PlumX Metrics


1966BA03      Phys.Rev. 144, 799 (1966)

J.K.Bair, J.L.C.Ford, Jr., C.M.Jones

Total Neutron Yield from the Reaction 14C(α, n)17O

NUCLEAR STRUCTURE 14C, 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.144.799
Citations: PlumX Metrics


1966TH10      Phys.Rev.Lett. 17, 701 (1966)

S.T.Thornton, J.K.Bair, C.M.Jones, H.B.Willard

Search for the Trineutron

NUCLEAR REACTIONS 3H(n, p), E=20.8 MeV; measured reaction products, Ep, Ip; deduced lack of evidence for of bound 3n system.

doi: 10.1103/PhysRevLett.17.701
Citations: PlumX Metrics


1965FO05      Nucl.Phys. 63, 588 (1965)

J.L.C.Ford, Jr., J.K.Bair, C.M.Jones, H.B.Willard

The 18O(α, p) Reaction and the Beta Decay of 21F

NUCLEAR REACTIONS 18O(d, p), E=7.76-9.95 MeV; measured σ(E). 22Ne deduced levels. Enriched target. 21F; measured T1/2.

doi: 10.1016/0029-5582(65)90745-5
Citations: PlumX Metrics


1965JO19      Rev.Mod.Phys. 37, 437 (1965)

C.M.Jones, J.K.Bair, C.H.Johnson, H.B.Willard, M.Reeves III

Sequential Emission in the Reaction 7Li(d, n)2a

NUCLEAR REACTIONS 7Li(d, n), E=1.8-7.0 MeV; measured Eα, αα-coin; deduced sequential decay.

doi: 10.1103/RevModPhys.37.437
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0224.


1964BA08      Nucl. Phys. 50, 604 (1964)

A.C.L.Barnard, C.M.Jones, J.L.Weil

Elastic Scattering of 2-11 MeV Protons by He4

doi: 10.1016/0029-5582(64)90233-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1113.


1964BA09      Nucl. Phys. 50, 629 (1964)

A.C.L.Barnard, C.M.Jones, G.C.Phillips

The Scattering of He3 by He4

NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90235-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1269.


1964BA16      Nucl. Phys. 53, 209 (1964)

J.K.Bair, C.M.Jones, H.B.Willard

Neutrons from the Proton Bombardment of Li6, Li7, Be9, B11 and O18

NUCLEAR STRUCTURE 18O, 7Li, 9Be, 11B, 6Li; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90598-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1366.


1964SW02      Bull.Am.Phys.Soc. 9, No.4, 408, CA11 (1964)

J.B.Swint, T.B.Clegg, J.L.Weil, C.M.Jones, A.C.L.Barnard

Scattering of Protons by 12C

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1964WI06      Phys.Letters 9, 339 (1964)

H.B.Willard, J.K.Bair, C.M.Jones

N-D Scattering: A Search for Effects Due to the Dineutron

NUCLEAR STRUCTURE 2n; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90390-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11032.


1963BA04      Bull.Am.Phys.Soc. 8, No.2, 124, U4 (1963)

A.C.L.Barnard, C.M.Jones, J.L.Weil

He4(p, p)He4 Reaction and Phase Shifts

NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.


1963BA55      WASH-1044, p.64 (1963)

J.K.Bair, C.M.Jones, H.B.Willard

Neutrons from the Proton Bombardment of Li6, Li7, Be9, B11 and O18

NUCLEAR STRUCTURE 11B, 6Li; measured not abstracted; deduced nuclear properties.


1963FO03      Bull.Am.Phys.Soc. 8, No.4, 317, G5 (1963)

J.L.C.Ford, Jr., J.K.Bair, C.M.Jones, H.B.Willard

O18(α, p)F21 Reaction and the β Decay of F21

NUCLEAR STRUCTURE 18O, 21F; measured not abstracted; deduced nuclear properties.


1963PO05      Ornl Annual Information Meeting p.26 (1963)

D.Powers, J.Bair, H.B.Willard, J.L.C.Ford, C.M.Jones

O13(α, α)O18, O18(α, p)F21 and the Beta Decay of F21

NUCLEAR STRUCTURE 21F; measured not abstracted; deduced nuclear properties.


1963WI08      ORNL-3425, p.18 (1963)

H.B.Willard, J.K.Bair, J.L.C.Ford, Jr., C.M.Jones

The O16(α, p)F21 Reaction and the Beta Decay of F21

NUCLEAR STRUCTURE 21F; measured not abstracted; deduced nuclear properties.


1962HA37      Nuclear Phys. 38, 259 (1962)

R.W.Harris, G.C.Phillips, C.M.Jones

Phase Shift Analysis of the Elastic Scattering of Protons from Oxygen

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)91033-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1013.


1962JO01      Bull.Am.Phys.Soc. 7, No.2, 119, J2 (1962)

C.M.Jones, A.C.L.Barnard, G.C.Phillips

Elastic Scattering of He3 from He4

NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.


1962JO09      Nuclear Phys. 37, 1 (1962)

C.M.Jones, G.C.Phillips, R.W.Harris, E.H.Beckner

The Scattering of Alpha Particles from C12

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90242-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1029.


1961HA13      Bull.Am.Phys.Soc 6, No. 4, 341, F5 (1961)

R.W.Harris, G.C.Phillips, C.M.Jones

Phase Shift Analysis in the Elastic Scattering of Protons by O16

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


1961JO04      Bull.Am.Phys.Soc. 6, No.3, 227, AA10 (1961)

C.M.Jones, G.C.Phillips, R.W.Harris, E.H.Beckner

Elastic Scattering of Alpha Particles from C12

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1961TO09      Bull.Am.Phys.Soc. 6, No.6, 507, E14 (1961)

T.A.Tombrello, C.M.Jones, G.C.Phillips, J.L.Weil

Elastic Scattering of Protons from He3

NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.


1960JO03      Phys.Rev. 117, 525 (1960)

C.M.Jones, G.C.Phillips, P.D.Miller

Alpha-Alpha Scattering in the Energy Range 5 to 9 MeV

NUCLEAR STRUCTURE 8Be, 4He; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.117.525
Citations: PlumX Metrics


1959JO19      Bull.Am.Phys.Soc. 4, No.2, 104, P8 (1959)

C.M.Jones, P.D.Miller, G.C.Phillips

Alpha-Alpha Scattering in the Range 4.5 to 9 MeV


1958MO99      Phys.Rev. 110, 1369 (1958)

C.D.Moak, A.Galonsky, R.L.Traughber, C.M.Jones

Energy Levels of Be9, C12, and C13

doi: 10.1103/PhysRev.110.1369
Citations: PlumX Metrics


1957GA01      Bull.Am.Phys.Soc. 2, No.1, 51, RA1 (1957)

A.Galonsky, C.D.Moak, R.L.Traughber, C.M.Jones

Energy Levels of C13 from B11(He3, p)C13


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