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NSR database version of April 26, 2024.

Search: Author = J.Davis

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2024CO05      Phys.Rev.Lett. 132, 152503 (2024)

I.Cox, Z.Y.Xu, R.Grzywacz, W.-J.Ong, B.C.Rasco, N.Kitamura, D.Hoskins, S.Neupane, T.J.Ruland, J.M.Allmond, T.T.King, R.S.Lubna, K.P.Rykaczewski, H.Schatz, B.M.Sherrill, O.B.Tarasov, A.D.Ayangeakaa, H.C.Berg, D.L.Bleuel, G.Cerizza, J.Christie, A.Chester, J.Davis, C.Dembski, A.A.Doetsch, J.G.Duarte, A.Estrade, A.Fijalkowska, T.J.Gray, E.C.Good, K.Haak, S.Hanai, J.T.Harke, C.Harris, K.Hermansen, D.E.M.Hoff, R.Jain, M.Karny, K.Kolos, A.Laminack, S.N.Liddick, B.Longfellow, S.Lyons, M.Madurga, M.J.Mogannam, A.Nowicki, T.H.Ogunbeku, G.Owens-Fryar, M.M.Rajabali, A.L.Richard, E.K.Ronning, G.E.Rose, K.Siegl, M.Singh, A.Spyrou, A.Sweet, A.Tsantiri, W.B.Walters, R.Yokoyama

Proton Shell Gaps in N=28 Nuclei from the First Complete Spectroscopy Study with FRIB Decay Station Initiator

RADIOACTIVITY ⁴⁵Cl(β^-) [from ⁹Be(⁸²Se, X), E=165 MeV/nucleon]; measured decay products, Eγ, Iγ, Eβ, Iβ; deduced β-decay strength distribution, the transitioning of neutrons into protons excited across the Z=20 shell gap. Comparison with shell model calculations using SDPF-MU interaction. The Facility for Rare Isotope Beams (FRIB) with the FRIB Decay Station Initiator.

doi: 10.1103/PhysRevLett.132.152503
Citations: PlumX Metrics

2023AL24      Chin.Phys.C 47, 103001 (2023)

S.Al Kharusi, G.Anton, I.Badhrees, P.S.Barbeau, D.Beck, V.Belov, T.Bhatta, M.Breidenbach, T.Brunner, G.F.Cao, W.R.Cen, C.Chambers, B.Cleveland, M.Coon, A.Craycraft, T.Daniels, L.Darroch, S.J.Daugherty, J.Davis, S.Delaquis, A.Der Mesrobian-Kabakian, R.DeVoe, J.Dilling, A.Dolgolenko, M.J.Dolinski, J.Echevers, W.Fairbank Jr., D.Fairbank, J.Farine, S.Feyzbakhsh, P.Fierlinger, Y.S.Fu, D.Fudenberg, P.Gautam, R.Gornea, G.Gratta, C.Hall, E.V.Hansen, J.Hoessl, P.Hufschmidt, M.Hughes, A.Iverson, A.Jamil, C.Jessiman, M.J.Jewell, A.Johnson, A.Karelin, L.J.Kaufman, T.Koffas, R.Krucken, A.Kuchenkov, K.S.Kumar, Y.Lan, A.Larson, B.G.Lenardo, D.S.Leonard, G.S.Li, S.Li, Z.Li, C.Licciardi, Y.H.Lin, R.MacLellan, T.McElroy, T.Michel, B.Mong, D.C.Moore, K.Murray, O.Njoya, O.Nusair, A.Odian, I.Ostrovskiy, A.Perna, A.Piepke, A.Pocar, F.Retiere, A.L.Robinson, P.C.Rowson, J.Runge, S.Schmidt, D.Sinclair, K.Skarpaas, A.K.Soma, V.Stekhanov, M.Tarka, S.Thibado, J.Todd, T.Tolba, T.I.Totev, R.Tsang, B.Veenstra, V.Veeraraghavan, P.Vogel, J.-L.Vuilleumier, M.Wagenpfeil, J.Watkins, M.Weber, L.J.Wen, U.Wichoski, G.Wrede, S.X.Wu, Q.Xia, D.R.Yahne, L.Yang, Y.-R.Yen, O.Ya.Zeldovich, T.Ziegler, EXO-200 Collaboration

Search for two-neutrino double-beta decay of ¹³⁶Xe to the 0⁺₁ excited state of ¹³⁶Ba with the complete EXO-200 dataset

RADIOACTIVITY ¹³⁶Xe(2β^-); analyzed available data using a deep learning-based convolutional neural network is used to discriminate signal from background events; deduced T_1/2 lower limit at 90% confidence level.

doi: 10.1088/1674-1137/aceee3
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021AL33      Phys.Rev. D 104, 112002 (2021)

S.Al Kharusi, G.Anton, I.Badhrees, P.S.Barbeau, D.Beck, V.Belov, T.Bhatta, M.Breidenbach, T.Brunner, G.F.Cao, W.R.Cen, C.Chambers, B.Cleveland, M.Coon, A.Craycraft, T.Daniels, L.Darroch, S.J.Daugherty, J.Davis, S.Delaquis, A.Der Mesrobian-Kabakian, R.DeVoe, J.Dilling, A.Dolgolenko, M.J.Dolinski, J.Echevers, W.Fairbank, D.Fairbank, J.Farine, S.Feyzbakhsh, P.Fierlinger, D.Fudenberg, P.Gautam, R.Gornea, G.Gratta, C.Hall, E.V.Hansen, J.Hoessl, P.Hufschmidt, M.Hughes, A.Iverson, A.Jamil, C.Jessiman, M.J.Jewell, A.Johnson, A.Karelin, L.J.Kaufman, T.Koffas, R.Krucken, A.Kuchenkov, K.S.Kumar, Y.Lan, A.Larson, B.G.Lenardo, D.S.Leonard, G.S.Li, S.Li, Z.Li, C.Licciardi, Y.H.Lin, R.MacLellan, T.McElroy, T.Michel, B.Mong, D.C.Moore, K.Murray, O.Njoya, O.Nusair, A.Odian, I.Ostrovskiy, A.Perna, A.Piepke, A.Pocar, F.Retiere, A.L.Robinson, P.C.Rowson, D.Ruddell, J.Runge, S.Schmidt, D.Sinclair, K.Skarpaas, A.K.Soma, V.Stekhanov, M.Tarka, S.Thibado, J.Todd, T.Tolba, T.I.Totev, R.Tsang, B.Veenstra, V.Veeraraghavan, P.Vogel, J.-L.Vuilleumier, M.Wagenpfeil, J.Watkins, M.Weber, L.-J.Wen, U.Wichoski, G.Wrede, S.X.Wu, Q.Xia, D.R.Yahne, L.Yang, Y.-R.Yen, O.Ya.Zeldovich, T.Ziegler

Search for Majoron-emitting modes of ¹³⁶Xe double beta decay with the complete EXO-200 dataset

RADIOACTIVITY ¹³⁶Xe(2β^-); analyzed available data; deduced T_1/2 limit on Majoron-emitting modes. The full EXO-200 dataset.

doi: 10.1103/PhysRevD.104.112002
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Data from this article have been entered in the XUNDL database. For more information, click here.

1996DA44      Hyperfine Interactions 101/102, 439 (1996)

J.D.Davis, R.E.Welsh

Muon Lifetimes and Weak Interaction Coupling Constants

NUCLEAR REACTIONS ¹H(μ⁺, X), (μ^-, X), E at rest; analyzed capture rates; deduced induced pseudo-scalar coupling constant to high accuracy, nucleon chiral structure related features.

1993HE25      At.Data Nucl.Data Tables 54, 181 (1993)

B.L.Henke, E.M.Gullikson, J.C.Davis

X-Ray Interactions: Photoabsorption, Scattering, Transmission, and Reflection at E = 50-30, 000 eV, Z = 1-92

COMPILATION Z=1-92; compiled theoretical σ of the primary interactions of low-energy x-rays within condensed matter, viz. photoabsorption and coherent scattering within 50 eV to 30 KeV range.

doi: 10.1006/adnd.1993.1013
Citations: PlumX Metrics

1993SU21      Phys.Rev. D47, 1762 (1993)

I.Supek, D.B.Barlow, W.J.Briscoe, J.F.Davis, G.J.Kim, D.W.Lane, A.Mokhtari, B.M.K.Nefkens, C.Pillai, M.E.Sadler, C.J.Seftor, M.F.Taragin, J.A.Wightman

Spin-Rotation Parameters A and R for π⁺p and π^-p Elastic Scattering from 427 to 657 MeV/c

NUCLEAR REACTIONS ¹H(π⁺, π⁺), (π^-, π^-), E at 427-657 MeV/c; measured spin rotation parameter, πp-coin. Polarized target.

doi: 10.1103/PhysRevD.47.1762
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1992OD02      Nucl.Instrum.Methods Phys.Res. A317, 445 (1992)

J.M.O'Donnell, J.Davis, R.A.DeHaven, E.Gray, R.Johnson, R.E.Lomax, B.J.McCloud, J.A.McGill, C.L.Morris, J.Novak, B.Rusnak, G.Tubb, J.M.Applegate, T.D.Averett, J.Beck, B.G.Ritchie, E.Haebel, D.Kiehlmann, U.Klein, M.Peiniger, P.Schafer, H.Vogel, H.Ward, C.F.Moore

A Superconducting Radio-Frequency Cavity for Manipulating the Phase Space of Pion Beams at LAMPF

NUCLEAR REACTIONS ⁹³Nb(π⁺, π⁺), E=50 MeV; ¹²C(π⁺, π⁺'), E=50 MeV; measured spectra. Superconducting radio-frequency cavity, pion beam phase space manipulation.

doi: 10.1016/0168-9002(92)90988-G
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1989BA08      Phys.Rev.Lett. 62, 1009 (1989)

D.B.Barlow, R.S.Kessler, G.J.Kim, B.M.K.Nefkens, C.Pillai, J.W.Price, J.A.Wightman, S.Hall, D.W.Lane, S.R.Loe, L.K.Morton, M.E.Sadler, S.D.Adrian, W.J.Briscoe, L.H.Kramer, A.Mokhtari, A.M.Petrov, C.J.Seftor, M.F.Taragin, J.F.Davis, I.Supek

Measurement of the Spin-Rotation Parameters A and R for π⁺p → π⁺p and π^-p → π^-p Scattering from 471 to 625 MeV/c

NUCLEAR REACTIONS ¹H(π⁺, π⁺), (π^-, π^-), E at 471-625 MeV/c; measured spin rotation parameters. Frozen spin polarized target.

doi: 10.1103/PhysRevLett.62.1009
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1986BR03      Phys.Rev. C33, 1235 (1986)

V.R.Brown, C.Wong, C.H.Poppe, J.D.Anderson, J.C.Davis, S.M.Grimes, V.A.Madsen

Cross Sections for the Ti(p, n) Reaction to Analogs of Ground and 2⁺ Excited States

NUCLEAR REACTIONS, ICPND ^{46,47,48,49,50}Ti(p, n), E=11.5-26 MeV; measured σ(En), σ(θ); deduced σ, β(n)/β(p). ^46,48,50Ti levels deduced β.

doi: 10.1103/PhysRevC.33.1235
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0098.

1986ST09      Nucl.Phys. A457, 669 (1986)

A.Stetz, L.W.Swenson, J.Davis, J.Kallne, R.C.Minehart, R.R.Whitney, V.Perez-Mendez, A.Sagle, J.Carroll, J.B.McClelland, J.A.Faucett

Pion Double Charge Exchange on ³He and ⁴He

NUCLEAR REACTIONS ³He(π^-, π⁺), ⁴He(π⁺, π^-), E=140, 200, 295 MeV; measured σ(E, E(π), θ); deduced σ(E, θ), σ(E). Phase space model.

doi: 10.1016/0375-9474(86)90474-4
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1985GR09      Phys.Rev. C31, 1679 (1985)

S.M.Grimes, J.D.Anderson, J.C.Davis, R.H.Howell, C.Wong, A.W.Carpenter, J.A.Carr, F.Petrovich

Gamow-Teller Matrix Elements from the ¹¹B(p, n)¹¹C Reaction at E(p) ≈ 26 MeV

NUCLEAR REACTIONS, ICPND ¹¹B(p, n), E=16-26 MeV; measured σ(En), σ(θ); deduced residual producation σ. ¹¹C levels deduced Gamow-Teller matrix elements. DWA analysis, Cohen-Kurath wave functions, G-matrix based interactions.

doi: 10.1103/PhysRevC.31.1679
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2665.

1984BO02      Phys.Rev. C29, 182 (1984)

K.G.Boyer, W.J.Braithwaite, W.B.Cottingame, S.J.Greene, L.E.Smith, C.F.Moore, C.L.Morris, H.A.Thiessen, G.S.Blanpied, G.R.Burleson, J.F.Davis, J.S.McCarthy, R.C.Minehart, C.A.Goulding

Pion Elastic and Inelastic Scattering from ^40,42,44,48Ca and ⁵⁴Fe

NUCLEAR REACTIONS ^40,42,44,48Ca, ⁵⁴Fe(π⁺, π⁺'), (π^-, π^-'), E=116, 118, 292.5 MeV; measured σ(E(π)), σ(θ). ^40,42,44,48Ca, ⁵⁴Fe level deduced neutron density rms radii. DWIA analysis.

doi: 10.1103/PhysRevC.29.182
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1981BO26      Phys.Rev. C24, 598 (1981)

K.G.Boyer, W.B.Cottingame, L.E.Smith, S.J.Greene, C.F.Moore, J.S.McCarthy, R.C.Minehart, J.F.Davis, G.R.Burleson, G.Blanpied, C.A.Goulding, H.A.Thiessen, C.L.Morris

Pion Inelastic Scattering to the Low-Lying States in ^42,44,48Ca: Determination of the neutron and proton multipole matrix elements

NUCLEAR REACTIONS ^42,44,48Ca(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=180 MeV; measured σ(θ). ^40,42,48Ca levels deduced neutron, proton multipole matrix elements, M(E2), M(E3). DWIA analysis, collective, microscopic model from factors.

doi: 10.1103/PhysRevC.24.598
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1981KA17      Phys.Lett. 103B, 13 (1981)

J.Kallne, J.F.Davis, J.S.McCarthy, R.C.Minehart, R.R.Whitney, R.L.Boudrie, J.B.McClelland, A.Stetz

Elastic π± + ³He Scattering

NUCLEAR REACTIONS ³He(π⁺, π⁺), (π^-, π^-), E=50, 100, 200 MeV; measured σ(θ); ³He(π⁺, π⁺), (π^-, π^-), (π^-, π⁰), E=295 MeV; analyzed data; deduced Coulomb interference effects, spin-flip contributions. Optical, multiple-scattering model analyses.

doi: 10.1016/0370-2693(81)90183-0
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1981KA41      J.Phys.(London) G7, L287 (1981)

J.Kallne, J.Davis, R.C.Minehart, R.R.Whitney, R.L.Boudrie, J.B.McClelland, A.W.Stetz

The (π±, p) Reactions and Nuclear pp and pn Correlations

NUCLEAR REACTIONS ^3,4He, ²⁷Al(π⁺, p), (π^-, p), E=50-300 MeV; measured σ(θ, Ep); deduced proton-proton, proton-neutron correlations.

doi: 10.1088/0305-4616/7/12/005
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1981MI05      Phys.Rev.Lett. 46, 1185 (1981)

R.C.Minehart, J.S.Boswell, J.F.Davis, D.Day, J.S.McCarthy, R.R.Whitney, H.J.Ziock, E.A.Wadlinger

Pion-Deuteron Elastic Scattering for Momenta from 408 to 600 MeV/c

NUCLEAR REACTIONS ²H(π⁺, π⁺), E at 408, 441, 539, 600 MeV/c; measured σ(θ). Liquid D₂ target.

doi: 10.1103/PhysRevLett.46.1185
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1981ST15      Phys.Rev.Lett. 47, 782 (1981)

A.Stetz, L.W.Swenson, J.Davis, J.Kallne, R.C.Minehart, R.R.Whitney, V.Perez-Mendez, A.Sagle, J.Carroll, J.B.McClelland, J.Faucett

Pion Double Charge Exchange on ⁴He and Meson Exchange Currents

NUCLEAR REACTIONS ⁴He(π⁺, π^-), E=140, 200, 295 MeV; measured σ(θ, E); deduced reaction mechanism, σ(total).

doi: 10.1103/PhysRevLett.47.782
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1980BU07      Phys.Rev. C21, 1452 (1980)

G.R.Burleson, G.S.Blanpied, J.Davis, J.S.McCarthy, R.C.Minehart, C.Goulding, C.L.Morris, H.A.Thiessen, W.B.Cottingame, S.Greene, C.F.Moore

Quasielastic Scattering of Pions from ¹²C and ^40,44,48Ca

NUCLEAR REACTIONS ¹²C, ^40,44,48Ca(π⁺, π⁺n), (π⁺, π⁺p), (π^-, π^-n), (π^-, π^-p), E=291 MeV; measured σ(θ(π+), E(π+)), σ(θ(π-), E(π-)). ¹²C, ^40,44,48Ca deduced participating nucleon number. Monte Carlo calculation, multiple scattering, Fermi gas model.

doi: 10.1103/PhysRevC.21.1452
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1980KA11      Phys.Rev. C21, 2681 (1980)

J.Kallne, J.Davis, P.C.Gugelot, J.S.McCarthy, G.R.Smith, R.L.Boudrie, B.Hoistad, C.L.Morris

(π, p) Absorption in ^6,7Li at 75 and 175 MeV

NUCLEAR REACTIONS ^6,7Li(π⁺, p), E=75, 175 MeV; measured σ(θp). ⁶Li(π⁺, p), (π^-, p), E=75, 175 MeV; measured σ(Ep); deduced reaction mechanism.

doi: 10.1103/PhysRevC.21.2681
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1980KA17      Phys.Rev.Lett. 45, 517 (1980)

J.Kallne, J.F.Davis, J.S.McCarthy, R.C.Minehart, R.R.Whitney, R.L.Boudrie, J.McClelland, A.Stetz

Pion-Helium Scattering above the (3, 3) Resonance

NUCLEAR REACTIONS ^3,4He(π⁺, π⁺), E=260, 295, 310 MeV; ^3,4He(π^-, π^-), E=295 MeV; measured σ(θ); deduced intermediate dibaryon state effects.

doi: 10.1103/PhysRevLett.45.517
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1980KA37      Phys.Lett. B97, 205 (1980)

J.Kallne, J.Davis, R.C.Minehart, R.R.Whitney, R.L.Boudrie, J.McClelland, A.W.Stetz

Two-Nucleon Pion Absorption in ^3,4He

NUCLEAR REACTIONS ^3,4He(π⁺, p), E=50-295 MeV; measured σ(θ, p(momentum)); deduced two-nucleon absorption effects.

doi: 10.1016/0370-2693(80)90583-3
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1979DA16      Phys.Rev. C20, 1946 (1979)

J.Davis, J.Kallne, J.S.McCarthy, R.C.Minehart, C.L.Morris, H.A.Thiessen, G.Blanpied, G.R.Burleson, K.Boyer, W.Cottingame, C.F.Moore, C.A.Goulding

Pion Double Charge Exchange Reactions in ¹²C and ^40,44,48Ca

NUCLEAR REACTIONS ¹²C, ^40,44,48Ca(π^-, π⁺), (π⁺, π^-), E=290 MeV; measured σ(E(π')).

doi: 10.1103/PhysRevC.20.1946
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1977DA18      Aust.J.Phys. 30, 167(1977)

J.R.Davis, G.U.Din

The ¹¹B(³He, n₀)¹³N Reaction

NUCLEAR REACTIONS ¹¹B(³He, n), E=5-12 MeV; measured σ(E;En, θ).

doi: 10.1071/PH770167
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0206.

1976MA07      Phys.Rev. C13, 548 (1976)

V.A.Madsen, V.R.Brown, S.M.Grimes, C.H.Poppe, J.D.Anderson, J.C.Davis, C.Wong

Effect of Inelastic Coupling on 0⁺ Analog Transitions

NUCLEAR REACTIONS ^92,98,100Mo(p, n), E=18, 22, 26 MeV; measured σ(θ). ^92,98,100Mo(p, n), E=16, 26 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.13.548
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0285.

1976PO06      Phys.Rev. C14, 438 (1976)

C.H.Poppe, J.D.Anderson, J.C.Davis, S.M.Grimes, C.Wong

Cross Sections for the ⁷Li(p, n)⁷Be Reaction between 4.2 and 26 MeV

NUCLEAR REACTIONS ⁷Li(p, n), E=4.2-26 MeV; measured σ(E, θ) to ⁷Be ground state, first excited state; θ=3.5°-159°.

doi: 10.1103/PhysRevC.14.438
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1470.

1975GR01      Phys.Rev. C11, 158 (1975)

S.M.Grimes, C.H.Poppe, J.D.Anderson, J.C.Davis, W.H.Dunlop, C.Wong

Energy Dependence of the (p, n) Analog Cross Sections of the Molybdenum Isotopes between 16 and 26 MeV

NUCLEAR REACTIONS ^{92,94,95,96,97,98,100}Mo(p, n), E=16, 18, 20, 22, 24, 26 MeV; measured σ(E, En, θ).

doi: 10.1103/PhysRevC.11.158
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0284.

1975WO01      Phys.Rev. C11, 137 (1975)

C.Wong, V.R.Brown, J.D.Anderson, J.C.Davis, S.M.Grimes, C.H.Poppe, V.A.Madsen

Population of Analogs of Excited States in ⁶³Cu(p, n) at 16, 19, and 22 MeV

NUCLEAR REACTIONS ⁶³Cu(p, n), E=16, 19, 22 MeV; ⁶⁴Zn(p, n), E=22 MeV; measured σ(En, θ). ⁶³Zn deduced analog states.

doi: 10.1103/PhysRevC.11.137
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1975WO11      Phys.Rev. C12, 2115 (1975)

C.Wong, J.D.Anderson, V.R.Brown, J.C.Davis, S.M.Grimes, V.A.Madsen, C.H.Poppe

Excited Analogs in ⁶²Ni and ⁶³Cu(p, n) and the Weak-Coupling Model

NUCLEAR REACTIONS ⁶²Ni(p, n), E=16, 19, 22 MeV; measured σ(θ) ground-state, excited-state analog; calculated σ(θ) using weak-coupling model.

doi: 10.1103/PhysRevC.12.2115
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0123.

1974AN10      Yad.Fiz. 19, 943 (1974); Sov.J.Nucl.Phys. 19, 483 (1975)

J.D.Anderson, H.H.Barschall, J.C.Davis

Total Cross Section of ²⁰⁷Pb for Neutrons Near 17 MeV

NUCLEAR REACTIONS ²⁰⁷Pb(n, X), E=16.8 MeV; measured σ. ²⁰⁸Pb deduced absence of previously reported resonance.

1974HA42      Phys.Rev. C10, 1111 (1974)

L.F.Hansen, J.C.Davis, F.S.Dietrich, M.C.Gregory, R.P.Koopman

Levels of ⁶⁴Ga via the ⁶⁴Zn(p, n) and ⁶⁴Zn(p, nγ) Reactions

NUCLEAR REACTIONS ⁶⁴Zn(p, n), E=10, 10.5 MeV; measured σ(En, θ). ⁶⁴Zn(p, nγ), E=8.0-10.5 MeV; measured σ(E, Eγ), γ(t); deduced Q. ⁶⁴Ga deduced levels, T_1/2, J, π.

doi: 10.1103/PhysRevC.10.1111
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0477.

1974PO11      Phys.Rev.Lett. 33, 856 (1974)

C.H.Poppe, S.M.Grimes, J.D.Anderson, J.C.Davis, W.H.Dunlop, C.Wong

Anomalous Behavior of the (p, n) Analog Reaction on the Molybdenum Isotopes

NUCLEAR REACTIONS ^{92,94,95,96,97,98,100}Mo(p, n), E=16-26 MeV; measured σ(E, θ). ^{92,94,95,96,97,98,100}Tc analog state deduced cross section ratios.

doi: 10.1103/PhysRevLett.33.856
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1973DA21      Phys.Rev. C8, 863 (1973)

J.C.Davis, J.D.Anderson, S.M.Grimes, C.Wong

Proton-Proton Final-State Interaction in the ²H(p, n)2p Reaction

NUCLEAR REACTIONS ²H(p, n), E=16-26 MeV; measured σ(E;En). Deduced p-p scattering length.

doi: 10.1103/PhysRevC.8.863
Citations: PlumX Metrics

1973GR13      Phys.Rev.Lett. 30, 992 (1973)

S.M.Grimes, J.D.Anderson, J.C.Davis, W.H.Dunlop, C.Wong

Cross-Section Measurements for the (p, n) Analog Transition in ¹⁸¹Ta, ¹⁹⁷Au, and ²⁰⁹Bi

NUCLEAR REACTIONS ¹⁸¹Ta, ¹⁹⁷Au, ²⁰⁹Bi(p, n), E=25, 27 MeV; ¹⁸¹W, ¹⁹⁷Hg, ²⁰⁹Po IAR measured σ(θ); ²⁰⁹Po IAR deduced level-width.

doi: 10.1103/PhysRevLett.30.992
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0312.

1973GR32      Phys.Rev. C8, 1770 (1973)

S.M.Grimes, J.D.Anderson, J.C.Davis, C.Wong

Nonequilibrium Contributions to the ⁵¹V(p, n)⁵¹Cr Reaction for 18 < E < 26 MeV

NUCLEAR REACTIONS ⁵¹V(p, n), Ep=18, 20, 22, 24, 26 MeV; measured σ(En, θ), θ=24-144°.

doi: 10.1103/PhysRevC.8.1770
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0920.

1973WE19      Nucl.Sci.Eng. 52, 35 (1973)

K.A.Weaver, J.D.Anderson, H.H.Barschall, J.C.Davis

Neutron Spectra from Deuteron Bombardment of D, Li, Be, and C

NUCLEAR REACTIONS ²H, Li, Be, C(d, xn), E < 20 MeV; measured σ(E;En).

doi: 10.13182/NSE73-A23287
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0218.

1973WO05      Phys.Rev. C7, 1895 (1973)

C.Wong, J.D.Anderson, J.C.Davis, S.M.Grimes

Energy Dependence of the ⁵¹V(p, n)⁵¹Cr Analog Transition between 16 and 26 MeV

NUCLEAR REACTIONS ⁵¹V(p, n), E=16-26 MeV; measured σ(E;En, θ) for ⁵¹Cr analog state.

doi: 10.1103/PhysRevC.7.1895
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1972DA02      Nucl.Phys. A179, 101 (1972)

J.R.Davis, G.U.Din

The ¹²C(d, n₀)¹³N Reaction from 3.6 MeV to 12.0 MeV

NUCLEAR REACTIONS ¹²C(d, n₀), E=3.6-12 MeV; measured σ(E:θ), σ(En, θ). Natural target.

doi: 10.1016/0375-9474(72)90108-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0803.

1972QU02      Nucl.Phys. A183, 173 (1972)

P.A.Quin, J.C.Davis, D.Hilscher

The ⁸⁹Y(d, n₀)⁹⁰Zr Reaction and Coulomb Effects in Stripping Reactions

NUCLEAR REACTIONS ⁸⁹Y(d, n₀), Ed=11.0 MeV; measured polarization parameter iT₁₁(θ). Natural target.

doi: 10.1016/0375-9474(72)90937-2
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1971DA07      Phys.Rev. C3, 1798 (1971)

J.C.Davis, H.H.Barschall

Fast-Neutron Total Cross Section of Deuterium

NUCLEAR REACTIONS ²H(n, X), E=1.5-27.5 MeV; measured σ(nT)(E).

doi: 10.1103/PhysRevC.3.1798
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10099.

1971DA24      Phys.Rev. C4, 1061 (1971)

J.C.Davis, K.A.Weaver, D.Hilscher, H.H.Barschall, A.B.Smith

Total Cross Section of Protons for 2.5-MeV Neutrons

NUCLEAR REACTIONS ¹H(n, X), E=2.5 MeV measured σ(nT).

doi: 10.1103/PhysRevC.4.1061
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10184.

1971DI21      Aust.J.Phys. 24, 497 (1971)

G.U.Din, J.R.Davis

A Study of Resonances in the ²⁹Si(p, γ)³⁰P Reaction

NUCLEAR REACTIONS ²⁹Si(p, γ), E=900-2120 keV; measured σ(E;Eγ). ³⁰P deduced resonances, levels, J, π, T, γ-branching. Ge(Li) detectors.

1971HI07      Nucl.Phys. A173, 216 (1971)

D.Hilscher, P.A.Quin, J.C.Davis

Comparison of the Vector Analysing Powers of the Mirror Reactions ³H(polarized d, n)⁴He and ³He(Polarized d, p)⁴He

NUCLEAR REACTIONS ³H(polarized d, n)⁴He, ³He(polarized d, p)⁴He, E=6, 10 MeV; measured vector analyzing power it11(Ed;θ). Enriched targets.

doi: 10.1016/0375-9474(71)90757-3
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1971HI09      Nucl.Phys. A174, 417 (1971)

D.Hilscher, J.C.Davis, P.A.Quin

Vector Analyzing Power of (d, n) Reactions on ¹¹B, ¹²C, ¹⁴N and ¹⁵N

NUCLEAR REACTIONS ¹¹B, ¹⁴N, ¹⁵N(d, n), Ed=10.0, 11.8 MeV; ¹²C(d, n), Ed=8.5 MeV; measured polarization parameter iT₁₁(Ed, θ); relative cross section σ(Ed, θ) for ¹²C, ¹⁴N(d, n). ¹²C level, ¹⁵O ground state deduced J, π.

doi: 10.1016/0375-9474(71)90674-9
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1969DA13      Nucl.Phys. A134, 361 (1969)

J.C.Davis, F.T.Noda

Neutron Energy Determinations

NUCLEAR REACTIONS ¹²C, ¹⁶O(n, X), E=3-8 MeV; measured σ(E). ²⁰Ne(n, α), E=3-6 MeV; measured σ(E). ¹³C, ¹⁷O, ²¹Ne deduced resonances.

doi: 10.1016/0375-9474(69)91059-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10021.

1968DA31      Phys.Lett. B 27, 636 (1968)

J.C.Davis, H.H.Barschall

Adjustments in the n-p singlet effective range

NUCLEAR REACTIONS ¹H(n, X), ¹⁴N(n, p), ²⁰Ne(n, α), ¹²C, ¹⁶O(n, n), E<5 MeV; analyzed available data; deduced σ, single effective ranges.

doi: 10.1016/0370-2693(68)90301-8
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Note: The following list of authors and aliases matches the search parameter J.Davis: , J.C.DAVIS, J.D.DAVIS, J.F.DAVIS, J.R.DAVIS