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NSR database version of April 24, 2024.

Search: Author = R.W.Kavanagh

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2002RA11      Eur.Phys.J. A 13, 377 (2002)

F.Raiola, P.Migliardi, G.Gyurky, M.Aliotta, A.Formicola, R.Bonetti, C.Broggini, L.Campajola, P.Corvisiero, H.Costantini, J.Cruz, A.D'Onofrio, Z.Fulop, G.Gervino, L.Gialanella, A.Guglielmetti, G.Imbriani, C.Gustavino, A.P.Jesus, M.Junker, R.W.Kavanagh, P.G.P.Moroni, A.Ordine, J.V.Pinto, E.Somorjai, F.Strieder, F.Terrasi, H.P.Trautvetter, S.Zavatarelli

Enhanced Electron Screening in d(d, p) for Deuterated Ta

NUCLEAR REACTIONS ²H(d, p), E=2.10, 21.5 keV; measured σ, astrophysical S-factor; deduced electron screening potential for atomic and molecular beams and a deuterated Ta target. Possible causes for a large electron screening discussed.

doi: 10.1007/s10050-002-8766-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1073.

2001BR22      Nucl.Phys. A688, 263c (2001)

C.R.Brune, J.Daly, R.Detwiler, B.Fisher, W.H.Geist, J.Gorres, H.J.Karwowski, R.W.Kavanagh, D.S.Leonard, P.Tischhauser, K.D.Veal, M.Wiescher

Using Sub-Coulomb α Transfer Reactions to Study the Low-Energy ¹²C(α, γ)¹⁶O S-Factor

NUCLEAR REACTIONS ¹²C(⁶Li, d), (⁷Li, t), E=2.7-7.0 MeV; measured Eγ, σ(θ), reduced α widths. ¹²C(α, γ), E=0-5 MeV; calculated E1 and E2 S-factors following R-matrix fits.

doi: 10.1016/S0375-9474(01)00711-4
Citations: PlumX Metrics

2001RA21      Eur.Phys.J. A 10, 487 (2001)

F.Raiola, G.Gyurky, M.Aliotta, A.Formicola, R.Bonetti, C.Broggini, L.Campajola, P.Corvisiero, H.Costantini, A.D'Onofrio, Z.Fulop, G.Gervino, L.Gialanella, A.Guglielmetti, C.Gustavino, G.Imbriani, M.Junker, R.W.Kavanagh, P.G.P.Moroni, A.Ordine, P.Prati, V.Roca, D.Rogalla, C.Rolfs, M.Romano, F.Schumann, E.Somorjai, O.Straniero, F.Strieder, F.Terrasi, H.P.Trautvetter, S.Zavatarelli

Stopping Power of Low-Energy Deuterons in ³He Gas

NUCLEAR REACTIONS ³He(d, p), E=10-100 keV; measured proton spectra; deduced deuteron stpping power in He gas.

doi: 10.1007/s100500170107
Citations: PlumX Metrics

2000WR01      Phys.Rev. C62, 055805 (2000)

P.R.Wrean, R.W.Kavanagh

Total Cross Sections and Reaction Rates for ¹⁹F(α, n)²²Na, ²²Ne(p, n)²²Na, and Their Inverses

NUCLEAR REACTIONS ¹⁹F(α, n), E=2.28-3.10 MeV; ²²Ne(p, n), E=3.7-5.4 MeV; measured neutron yields, σ; deduced reaction rates.

doi: 10.1103/PhysRevC.62.055805
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1049.

1999BR23      Phys.Rev. C60, 015801 (1999)

C.R.Brune, K.I.Hahn, R.W.Kavanagh, P.R.Wrean

Total Cross Section of the ³H(p, n)³He Reaction from Threshold to 4.5 MeV

NUCLEAR REACTIONS ³H(p, n), E=1-4.5 MeV; measured total σ; deduced thermonuclear reaction rate. Comparison with previous data.

doi: 10.1103/PhysRevC.60.015801
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0551.

1999BR46      Phys.Rev.Lett. 83, 4025 (1999)

C.R.Brune, W.H.Geist, R.W.Kavanagh, K.D.Veal

Sub-Coulomb α Transfers on ¹²C and the ¹²C(α, γ)¹⁶O S Factor

NUCLEAR REACTIONS ¹²C(⁶Li, d), E=2.7-7.0 MeV; ¹²C(⁷Li, t), E=4.75-7.0 MeV; measured Eγ, σ. ¹⁶O levels deduced α-widths. ¹²C(α, γ), E=low; deduced reaction S-factors. Nuclear Astrophysics.

doi: 10.1103/PhysRevLett.83.4025
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0593.

1998AD12      Rev.Mod.Phys. 70, 1265 (1998)

E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson

Solar Fusion Cross Sections

NUCLEAR REACTIONS ⁷Be, ^12,13C, ¹⁵N, ^16,17,18O(p, γ), ^14,15N, ^17,18O(p, α), ⁷Li(d, p), ³He(p, e⁺), (α, γ), (³He, 2p), ¹H(p, e⁺), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.

doi: 10.1103/RevModPhys.70.1265
Citations: PlumX Metrics

1998ST20      Eur.Phys.J. A 3, 1 (1998)

F.Strieder, F.Schumann, L.Gialanella, U.Greife, D.Rogalla, C.Rolfs, H.P.Trautvetter, Zs.Fulop, G.Gyurky, E.Somorjai, R.W.Kavanagh, L.Campajola, A.D'Onofrio, A.Ordine, V.Roca, M.Romano, F.Terrasi, C.Arpesella, A.D'Alessandro, C.Gustavino, M.Junker, O.Straniero, P.Corvisiero, M.Dessalvi, P.Prati, S.Zavatarelli, C.Broggini, G.Gervino, A.Fubini, E.Bellotti, R.Bonetti, A.Guglielmetti

Loss of ⁸Li Recoil Nuclei in ⁷Li(d, p)⁸Li and Implications on the ⁷Be(p, γ)⁸B Cross Section

NUCLEAR REACTIONS ⁷Li(d, p), E=0.4-1.8 MeV; measured yields; deduced recoil loss for several backing materials. ⁷Be(p, γ), E not given; deduced possible corrections to σ. Astrophysical implications.

doi: 10.1007/s100500050141
Citations: PlumX Metrics

1997GR11      Nucl.Phys. A621, 603c (1997)

U.Greife, C.Arpesella, E.Bellotti, K.Brand, C.Broggini, L.Campajola, P.Corvisiero, A.D'Onofrio, G.Fiorentini, A.Fubini, G.Gervino, L.Gialanella, C.Gustavino, E.Huttel, M.Junker, R.W.Kavanagh, R.Kubat, J.Lambert, G.Oliviero, P.Prati, H.Rebel, V.Roca, W.S.Rodney, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, F.Strieder, F.Terrasi, H.P.Trautvetter, D.Zahnow, S.Zavatarelli

Further Direct Approaches to the Nuclear Reactions in the Sun

doi: 10.1016/S0375-9474(97)00312-6
Citations: PlumX Metrics

1997KO31      Phys.Rev. C56, 1138 (1997)

P.E.Koehler, R.W.Kavanagh, R.B.Vogelaar, Yu.M.Gledenov, Yu.P.Popov

²⁶Al(n, p₁) and (n, α₀) Cross Sections from Thermal Energy to 70 keV and the Nucleosynthesis of ²⁶Al

NUCLEAR REACTIONS ²⁶Al(n, α), E thermal-10 keV; ²⁶Al(n, p), E thermal-70 keV; measured σ(E); deduced astrophysical reaction rates. ²⁷Al deduced resonances, Γ, resonance strength.

doi: 10.1103/PhysRevC.56.1138
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13897.

1996HA06      Phys.Rev. C53, 1273 (1996)

K.I.Hahn, C.R.Brune, R.W.Kavanagh

Angular Distributions of γ Rays from the ⁷Li(p, γ) Reaction at Low Energies

NUCLEAR REACTIONS, ICPND ⁷Li(p, γ), E=80-450 keV; measured Iγ(θ), relative yields; deduced Legendre coefficients.

doi: 10.1103/PhysRevC.53.1273
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0427.

1996ST08      Nucl.Phys. A601, 168 (1996)

F.Stegmuller, C.Rolfs, S.Schmidt, W.H.Schulte, H.P.Trautvetter, R.W.Kavanagh

²²Na(p, γ)²³Mg Resonant Reaction at Low Energies

NUCLEAR REACTIONS ²²Na(p, γ), E=0.2-0.63 MeV; measured γ-spectra; deduced reaction rates. ²³Mg deduced resonance energies, resonance strengths, reaction rates.

doi: 10.1016/0375-9474(96)00084-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0894.

1996VO07      Phys.Rev. C53, 1945 (1996)

R.B.Vogelaar, L.W.Mitchell, R.W.Kavanagh, A.E.Champagne, P.V.Magnus, M.S.Smith, A.J.Howard, P.D.Parker, H.A.O'Brien

Constraining ²⁶Al + p Resonances using ²⁶Al(³He, d)²⁷Si

NUCLEAR REACTIONS ²⁶Al(³He, d), E=20 MeV; measured σ(Ed), σ(θ); deduced implications for ²⁶Al(p, γ) stellar reaction rate, model parameters. ²⁷Si deduced levels, resonance, spectroscopic factors.

doi: 10.1103/PhysRevC.53.1945
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0102.

1995FI02      Z.Phys. A350, 289 (1995)

G.Fiorentini, R.W.Kavanagh, C.Rolfs

Prospects for Underground Accelerator Research

NUCLEAR REACTIONS, ICPND ³He(d, p), E ≤ 40 keV; compiled, reviewed astrophysical S-factor data, analyses. ¹²C(α, γ), E(cm) ≤ 3 MeV; compiled, reviewed capture σ(E) data, analyses. ²¹Ne(p, γ), E ≈ resonance; compiled, reviewed γ yield data, analyses; ³He(³He, 2p), E ≤ 350 keV; compiled, reviewed σ(E), astrophysical S-factor data, analyses. Underground accelerator research prospects discussed.

doi: 10.1007/BF01291186
Citations: PlumX Metrics

1995HA02      Phys.Rev. C51, 1624 (1995)

K.I.Hahn, C.R.Brune, R.W.Kavanagh

³H(p, γ)⁴He Cross Section

NUCLEAR REACTIONS, ICPND ³H(p, γ), E=0.1-6 MeV; measured Eγ, Iγ, σ(θ) vs E; deduced astrophysical S-factor vs E ≤ 0.8 MeV.

doi: 10.1103/PhysRevC.51.1624
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0089.

1995SC36      Nucl.Phys. A591, 227 (1995)

S.Schmidt, C.Rolfs, W.H.Schulte, H.P.Trautvetter, R.W.Kavanagh, C.Hategan, S.Faber, B.D.Valnion, G.Graw

²²Na(³He, d)²³Mg Reaction Studies of States Near the Proton Threshold and Hydrogen Burning of ²²Na

NUCLEAR REACTIONS ²²Na(³He, d), E=30 MeV; measured deuteron spectra, σ(θ); deduced stellar reaction rates. ²³Mg deduced resonances, J, π, Γ(p), resonance strengths. DWBA analysis.

doi: 10.1016/0375-9474(95)00164-V
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0893.

1994BR25      Phys.Rev. C50, 2205 (1994)

C.R.Brune, R.W.Kavanagh, C.Rolfs

³H(α, γ)⁷Li Reaction at Low Energies

NUCLEAR REACTIONS, ICPND ³H(α, γ), E(cm)=50-1200 keV; measured Eγ, Iγ; deduced σ(E), astrophysical S-factor vs E.

doi: 10.1103/PhysRevC.50.2205
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0191.

1994BR41      Nucl.Instrum.Methods Phys.Res. A343, 415 (1994)

C.R.Brune, R.W.Kavanagh

Production and Characterization of Thin Ti-³H and Ti-²H Targets

NUCLEAR REACTIONS ²H(³He, α), E=650 keV; ³H(d, α), E=400 keV; measured α spectra. ³H(d, α), E ≤ 800 keV; measured σ(E); deduced target fabrication features. Ti-²H, Ti-³H on Cu substrate.

doi: 10.1016/0168-9002(94)90218-6
Citations: PlumX Metrics

1994GR33      Nucl.Instrum.Methods Phys.Res. A350, 327 (1994)

U.Greife, C.Arpesella, C.A.Barnes, F.Bartolucci, E.Bellotti, C.Broggini, P.Corvisiero, G.Fiorentini, A.Fubini, G.Gervino, F.Gorris, C.Gustavino, M.Junker, R.W.Kavanagh, A.Lanza, G.Mezzorani, P.Prati, P.Quarati, W.S.Rodney, C.Rolfs, W.H.Schulte, H.P.Trautvetter, D.Zahnow

Laboratory for Underground Nuclear Astrophysics (LUNA)

NUCLEAR REACTIONS, ICPND ²H(d, n), (d, p), E=10 keV; ²H(³He, p), E=70 keV; measured spectra. ²H(³He, p), E ≤ 40 keV; ³He(³He, 2p), E ≤ 160 keV; measured astrophysical S-factor vs E. Windowless gas target system, close geometry detector telescopes.

doi: 10.1016/0168-9002(94)91182-7
Citations: PlumX Metrics

1994RO16      Z.Phys. A350, 93 (1994)

C.Rolfs, R.W.Kavanagh

Extrapolation of the S(E) Factor in ⁷Be(p, γ₀)⁸B: The ⁷Li(p, γ₀)⁸Be case

NUCLEAR REACTIONS, ICPND ⁷Li(p, γ), E ≤ 1.5 MeV; analyzed astrophysical S-factor; deduced resonance tail role, ⁷Be(p, γ) reaction astrophysical S-factor implications.

doi: 10.1007/BF01290674
Citations: PlumX Metrics

1994WR01      Phys.Rev. C49, 1205 (1994)

P.R.Wrean, C.R.Brune, R.W.Kavanagh

Total Cross Sections and Thermonuclear Reaction Rates for ⁹Be(α, n)¹²C

NUCLEAR REACTIONS, ICPND ⁹Be(α, n), E(cm)=0.16-1.87 MeV; measured σ(E), thick target yield. ⁹Be(p, p), E ≤ 2-66 MeV; measured σ(θ); deduced (α, n) reaction rate vs temperature, astrophysical S-factor.

doi: 10.1103/PhysRevC.49.1205
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0115.

1993BR17      Phys.Rev. C48, 3119 (1993)

C.R.Brune, I.Licot, R.W.Kavanagh

Low-Energy Resonances in ¹³C(α, n)

NUCLEAR REACTIONS, ICPND ¹³C(α, n), E=650-1600 KeV; measured yield vs E. ¹⁷O deduced resonances, Γn, Γα, resonance strengths.

doi: 10.1103/PhysRevC.48.3119
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0080.

1992BR05      Phys.Rev. C45, 1382 (1992)

C.R.Brune, R.W.Kavanagh

Total Cross Sections and Thermonuclear Reaction Rates for ¹³C(d, n) and ¹⁴C(d, n)

NUCLEAR REACTIONS, ICPND ^14,13C(d, n), E(cm) ≈ 0.2-2.3 MeV; measured σ(E); deduced thermonuclear reaction rates. 4π neutron detector.

doi: 10.1103/PhysRevC.45.1382
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0120.

1991BR03      Phys.Rev. C43, 875 (1991)

C.R.Brune, R.W.Kavanagh, S.E.Kellogg, T.R.Wang

Cross Sections for ³H(⁷Li, n₀)⁹Be and ³H(⁷Li, n(tot))

NUCLEAR REACTIONS ³H(⁷Li, n), E(cm)=0.15-1.24 MeV; measured σ(θ), total neutron yield; deduced thermonuclear reaction rates.

doi: 10.1103/PhysRevC.43.875
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0119.

1991BR19      Phys.Rev. C44, 1665 (1991)

C.R.Brune, R.W.Kavanagh

Width of the 0.55-MeV Resonance in ¹³C(p, γ)

NUCLEAR REACTIONS, ICPND ¹³C(p, γ), E=0.44-0.6 MeV; measured yields, relative σ(E). ¹⁴N deduced resonances, Γ.

doi: 10.1103/PhysRevC.44.1665
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0308.

1991WA02      Phys.Rev. C43, 883 (1991); Erratum Phys.Rev. C44, 1226 (1991)

T.R.Wang, R.B.Vogelaar, R.W.Kavanagh

¹¹B + α Reaction Rates and Primordial Nucleosynthesis

NUCLEAR REACTIONS, ICPND ¹¹B(α, n), E=350-2400 keV; ¹¹B(α, p), E=600-1800 keV; ¹⁴C(p, n), E=1000-1550 keV; measured σ(E), σ(θ), thick target yields. ¹¹B(α, γ), E=606 keV; measured γ(θ), thick target yields; deduced reaction rates. ¹⁵N deduced resonances, J, T.

doi: 10.1103/PhysRevC.43.883
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0519.

1990SE09      Nucl.Phys. A514, 471 (1990)

S.Seuthe, C.Rolfs, U.Schroder, W.H.Schulte, E.Somorjai, H.P.Trautvetter, F.B.Waanders, R.W.Kavanagh, H.Ravn, M.Arnould, G.Paulus

Resonances in the ²²Na(p, γ)²³Mg Reaction

NUCLEAR REACTIONS, ICPND ²²Na(p, γ), E=0.17-1.29 MeV; measured γ-spectra; deduced stellar reaction rates. ²³Mg deduced resonances, resonance strengths.

doi: 10.1016/0375-9474(90)90153-D
Citations: PlumX Metrics

1990VO06      Phys.Rev. C42, 753 (1990)

R.B.Vogelaar, T.R.Wang, S.E.Kellogg, R.W.Kavanagh

Low-Energy Reaction Yields for ¹⁸O(p, γ) and ¹⁸O(α, γ)

NUCLEAR REACTIONS, ICPND ¹⁸O(p, γ), E < 0.22 MeV; ¹⁸O(α, γ), E < 0.78 MeV; measured resonance γ yields, Eγ, Iγ; deduced thermonuclear reaction rate. ¹⁹F deduced resonance parameters, strengths, Γ. ²²Ne deduced resonance parameters, strengths, Γ, γ-branching.

doi: 10.1103/PhysRevC.42.753
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0368.

1989LE29      Nature(London) 340, 525 (1989)

N.S.Lewis, C.A.Barnes, M.J.Heben, A.Kumar, S.R.Lunt, G.E.McManis, G.M.Miskelly, R.M.Penner, M.J.Sailor, P.G.Santangelo, G.A.Shreve, B.J.Tufts, M.G.Youngquist, R.W.Kavanagh, S.E.Kellogg, R.B.Vogelaar, T.R.Wang, R.Kondrat, R.New

Searches for Low-Temperature Nuclear Fusion of Deuterium in Palladium

doi: 10.1038/340525a0
Citations: PlumX Metrics

1988SE09      Nucl.Instrum.Methods Phys.Res. A272, 814 (1988)

S.Seuthe, H.W.Becker, C.Rolfs, S.Schmidt, H.P.Trautvetter, R.W.Kavanagh, F.B.Waanders

Construction and Properties of a Gamma-Ray Detector Based on D(γ, n)H Neutron Counting

NUCLEAR REACTIONS ²⁷Al(p, γ), E ≈ 200-450 keV; ¹⁹F(p, αγ), E ≈ 750-1000 keV; measured γ yields. ²⁸Si levels deduced resonance strength. Neutron counting based γ-detector.

RADIOACTIVITY ⁶⁰Co(β^-); measured γ yields. ⁶⁰Ni deduced hexadecapole transition strength. Neutron counting based γ-detector.

doi: 10.1016/0168-9002(88)90763-2
Citations: PlumX Metrics

1987KA32      Phys.Rev. C36, 1194 (1987)

R.W.Kavanagh, R.G.Marcley

Thermal Cross Section for ¹⁰B(n, t)2α

NUCLEAR REACTIONS ¹⁰B(n, t), E=thermal; measured σ.

doi: 10.1103/PhysRevC.36.1194
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13124.

1987RO13      Nucl.Instrum.Methods Phys.Res. B26, 165 (1987)

C.Rolfs, R.W.Kavanagh

Gamma-Ray Detection via D(γ, n)H Neutron Counting

NUCLEAR REACTIONS ²⁷Al(p, γ), E=988-998 keV; measured thick target yields. D₂O graphite detector.

doi: 10.1016/0168-583X(87)90745-2
Citations: PlumX Metrics

1987SE13      Nucl.Instrum.Methods Phys.Res. A260, 33 (1987)

S.Seuthe, H.W.Becker, A.Krauss, A.Redder, C.Rolfs, U.Schroder, H.P.Trautvetter, K.Wolke, S.Wustenbecker, R.W.Kavanagh, F.B.Waanders

Production and Properties of Implanted Targets

NUCLEAR REACTIONS, ICPND ¹²C(p, γ), E=220-340 keV; ¹²C(α, γ), E=2.65-2.85 MeV; ¹⁴N(p, γ), E=260-360 keV; ²⁰Ne(p, γ), E=1165-1185 keV; ²³Na(p, γ), E=300-400 keV; measured γ-ray yields. Implanted targets.

doi: 10.1016/0168-9002(87)90385-8
Citations: PlumX Metrics

1987SK01      Phys.Rev. C35, 45 (1987)

R.T.Skelton, R.W.Kavanagh, D.G.Sargood

²⁶Mg(p, n)²⁶Al and ²³Na(α, n)²⁶Al Reactions

NUCLEAR REACTIONS, ICPND ²⁶Mg(p, n), ²³Na(α, n), E=3.5-5.8 MeV; measured σ(E); deduced inverse reaction ²⁶Al(n, p), (n, α) σ(E), thermal reaction rates vs temperature. Graphite cube neutron detector system.

doi: 10.1103/PhysRevC.35.45
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0304.

1986KA34      Phys.Rev. C34, 1477 (1986)

R.W.Kavanagh, L.W.Mitchell, D.G.Sargood

Branching Ratio of the Second Excited State of ³⁰P

NUCLEAR REACTIONS ²⁷Al(α, n), E=4.2 MeV; measured Eγ, Iγ. ³⁰P levels deduced decay charateristics, M1 transition width, M1 matrix element spin, orbital ratio, γ-branching.

doi: 10.1103/PhysRevC.34.1477
Citations: PlumX Metrics

1986RO13      Nucl.Phys. A455, 179 (1986)

C.Rolfs, R.W.Kavanagh

The ⁷Li(p, α)⁴He Cross Section at Low Energies

NUCLEAR REACTIONS, ICPND ⁷Li(p, α), E(cm)=25-873 keV; measured σ(θ); deduced σ, astrophysical S(E) factor.

doi: 10.1016/0375-9474(86)90351-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1438.

1986RO18      Nucl.Instrum.Methods Phys.Res. A247, 507 (1986)

C.Rolfs, R.W.Kavanagh

Gamma-Ray Detection via D(γ, n)H Neutron Counting

NUCLEAR REACTIONS, ICPND ²⁷Al(p, γ), E=988-998 keV; measured thick target yield curves. D₂O-graphite detector.

doi: 10.1016/0168-9002(86)90411-0
Citations: PlumX Metrics

1985MI17      Nucl.Phys. A443, 487 (1985)

L.W.Mitchell, R.W.Kavanagh, M.E.Sevior, C.I.W.Tingwell, D.G.Sargood

The ⁴²Ca(α, γ)⁴⁶Ti and ⁴²Ca(α, p)⁴⁵Sc Cross Sections and the Mass-45 Bottleneck

NUCLEAR REACTIONS, ICPND ⁴²Ca(α, γ), E=3.42-5.62 MeV; ⁴²Ca(α, pγ), E=4.06-5.92 MeV; ⁴²Ca(α, p), E=4.78-5.92 MeV; measured γ-ray, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.

doi: 10.1016/0375-9474(85)90414-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0310.

1984OL05      Phys.Rev. C30, 1375 (1984)

M.D.Olson, R.W.Kavanagh

⁷Li(α, n) Cross Section from Threshold to 5.67 MeV

NUCLEAR REACTIONS, ICPND ⁷Li(α, n), E=4.38-4.67 MeV; measured σ(E); deduced inverse reaction σ(E). ¹¹B resonances deduced parameters.

doi: 10.1103/PhysRevC.30.1375
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1984OS03      Nucl.Phys. A419, 115 (1984)

J.L.Osborne, C.A.Barnes, R.W.Kavanagh, R.M.Kremer, G.J.Mathews, J.L.Zyskind, P.D.Parker, A.J.Howard

Low-energy behavior of the ³He(α, γ)⁷Be cross section

NUCLEAR REACTIONS, ICPND ³He(α, γ), E=165-1169 keV; measured σ(E), Eγ, γ-branching ratio. ³He(α, γ), E(cm)=947, 1255 keV; measured σ(E). Enriched target.

doi: 10.1016/0375-9474(84)90288-4
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1984SK01      Nucl.Phys. A414, 141 (1984)

R.T.Skelton, R.W.Kavanagh

Measurement of the ⁷Be Branching Ratio

RADIOACTIVITY ⁷Be(EC) [from ⁷Li(p, n)]; measured Iγ. ⁷Li levels deduced branching. ⁸⁹Zr(EC), (β⁺) [from ⁸⁹Y(p, n)]; measured Iγ, T_1/2. Neutron-detection system.

doi: 10.1016/0375-9474(84)90501-3
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1984TH04      Phys.Rev. C30, 385 (1984)

J.H.Thomas, R.L.Rau, R.T.Skelton, R.W.Kavanagh

Half-Life of ²⁶Al

NUCLEAR REACTIONS Mg(p, n), E=5.8 MeV; measured Eγ, Iγ; deduced ²⁶Al atom yield.

RADIOACTIVITY ²⁶Al(β⁺), (EC) [from Mg(p, n), E=5.8 MeV]; measured Eγ, Iγ, T_1/2.

doi: 10.1103/PhysRevC.30.385
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1983SK03      Astrophys.J. 271, 404 (1983); Erratum Astrophys.J. 308, 485 (1986)

R.T.Skelton, R.W.Kavanagh, D.G.Sargood

²⁶Mg(p, n)²⁶Al Cross Section Measurements

NUCLEAR REACTIONS, ICPND ²⁶Mg(p, n), E(cm)=4.8-5.6 MeV; measured σ(E), total neutron yield vs E; deduced inverse reaction rate. Activation technique.

doi: 10.1086/161206
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1982OS02      Phys.Rev.Lett. 48, 1664 (1982)

J.L.Osborne, C.A.Barnes, R.W.Kavanagh, R.M.Kremer, G.J.Mathews, J.L.Zyskind, P.D.Parker, A.J.Howard

Low-Energy ³He(α, γ)⁷Be Cross-Section Measurements

NUCLEAR REACTIONS, ICPND ³He(α, γ), E(cm)=165-1170 keV; measured absolute σ vs E, γ-branching ratio; deduced zero-energy intercept. Activation technique, ³He gas target.

doi: 10.1103/PhysRevLett.48.1664
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1980WI13      Phys.Rev. C22, 1696 (1980)

H.S.Wilson, R.W.Kavanagh, F.M.Mann

Gamow-Teller Transitions in Some Intermediate-Mass Nuclei

RADIOACTIVITY ¹⁴O, ²¹Na, ²⁵Al, ²⁶Si, ^29,30P, ^30,31S, ^33,34mCl, ³⁵Ar, ³⁸Ca, ⁴¹Sc measured Iγ; deduced log ft. ²⁶Si, ²⁹P, ^30,31S, ^34mCl, ³⁸Ca; measured T_1/2. Shell model calculations, allowed Gamow-Teller transitions.

doi: 10.1103/PhysRevC.22.1696
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1977DE02      Phys.Rev. C15, 303 (1977)

N.M.Denkin, R.W.Kavanagh, G.Bedrosian

Lifetime and Branching Ratio of the Second Excited State of ³⁸K

NUCLEAR REACTIONS ²⁴Mg(¹⁶O, pn), E=27.5 MeV; measured recoil-distance. ³⁵Cl(α, n), E=7.31, 7.00 MeV; measured γ-spectrum. ³⁸K deduced levels, δ, T_1/2.

doi: 10.1103/PhysRevC.15.303
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1976MA14      Nucl.Phys. A258, 341 (1976)

F.M.Mann, H.S.Wilson, R.W.Kavanagh

Positron Decays of ²⁵Al, ³⁷K, ³⁸K and ³⁹Ca

RADIOACTIVITY ²⁵Al, ³⁷K, ³⁸K, ³⁹Ca; measured Iγ; deduced log ft.

doi: 10.1016/0375-9474(76)90010-5
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1975MA44      Nucl.Phys. A255, 287 (1975)

F.M.Mann, R.W.Kavanagh

(α, n) Measurements and the Determination of the Alpha Optical Potential

NUCLEAR REACTIONS ³⁵Cl(α, n), E=threshold-12 MeV; ⁵⁹Co, ^63,65Cu(α, n), E=threshold-18 MeV; measured σ. Hauser-Feshbach calculations.

doi: 10.1016/0375-9474(75)90680-6
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1974MA31      Phys.Lett. 51B, 49 (1974)

F.M.Mann, R.W.Kavanagh

Experimental Study of ¹⁹Ne Decay and its Significance to the Study of Neutral Weak Currents

RADIOACTIVITY ¹⁹Ne; measured Eγ, Iγ; deduced upper limit for Iβ.

doi: 10.1016/0370-2693(74)90148-8
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1974MA41      Nucl.Phys. A235, 299 (1974)

F.M.Mann, R.W.Kavanagh

Beta Decay of ²³Mg and ²⁷Si

RADIOACTIVITY ²³Mg, ²⁷Si; measured Iγ; deduced log ft. ²³Na, ²⁷Al levels deduced γ-branching.

doi: 10.1016/0375-9474(74)90194-8
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1973GO09      Phys.Rev. C7, 1717 (1973)

D.R.Goosman, R.W.Kavanagh

Cross Sections for ¹⁰Be(d, p)¹¹Be, ¹⁰Be(d, α)⁸Li, and ¹⁰Be(p, γ₀)¹¹B

NUCLEAR REACTIONS ¹⁰Be(d, p), (d, α), (p, γ₀); measured nothing; deduced σ based on new T_1/2(¹⁰Be).

doi: 10.1103/PhysRevC.7.1717
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1973MC01      Phys.Rev. C7, 489 (1973)

S.J.McCaslin, F.M.Mann, R.W.Kavanagh

Mass of the Second Excited State of ¹²C

NUCLEAR REACTIONS ¹⁵N(p, α), E approx threshold; measured Q, σ(Eα). ¹²C deduced level.

doi: 10.1103/PhysRevC.7.489
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1972KA41      Nucl.Phys. A195, 302 (1972)

R.W.Kavanagh, N.Schulz, J.C.Merdinger

Gamma-Ray Doppler-Shift Measurements in ⁴³Ca

NUCLEAR REACTIONS ⁴⁰Ar(α, nγ), E=6.3-8.0 MeV; measured Doppler-shift attenuation. ⁴³Ca levels deduced T_1/2.

doi: 10.1016/0375-9474(72)90738-5
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1972LI15      Nucl.Phys. A187, 1 (1972)

J.Lindskog, D.M.Gordon, R.W.Kavanagh

The Lifetime of the Lowest 5^- State in ³⁸Ar Measured by Recoil-Distance and Doppler-Shift Techniques

NUCLEAR REACTIONS ³⁵Cl(α, p), E=10.5 MeV; measured Doppler shift, recoil distance. ³⁸Ar deduced levels, T_1/2. Enriched, natural targets.

doi: 10.1016/0375-9474(72)90070-X
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1971GO10      Phys.Rev. C4, 145 (1971)

D.M.Gordon, R.W.Kavanagh

Lifetime of the 78-keV Level of ³²P

NUCLEAR REACTIONS ²⁹Si(α, pγ), ¹⁹F(α, nγ), E=4.5 MeV; measured σ(Ep, Eγ, θ(p)), recoil distance. ²²Na, ³²P levels deduced T_1/2.

doi: 10.1103/PhysRevC.4.145
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1971MO01      Phys.Rev. C3, 438 (1971)

J.M.Mosher, R.W.Kavanagh, T.A.Tombrello

Mass and Half-Life of ⁹C

RADIOACTIVITY ⁹C; measured T_1/2. ⁷Be(³He, n), E approx threshold; measured σ(E), delayed-p yield; deduced threshold. ⁹C deduced mass excess.

doi: 10.1103/PhysRevC.3.438
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1970CH07      Nucl.Phys. A146, 136 (1970)

Y.S.Chen, T.A.Tombrello, R.W.Kavanagh

Decay Modes of ⁹Li and States of ⁹Be

RADIOACTIVITY ⁹Li[from ³H(⁷Li, p), E=14 MeV; ¹⁸O(⁷Li, ¹⁶O), E=20 MeV]; measured T_1/2, Eβ, βn-coin, E(delayed n), E(delayed α); deduced log ft, Iβ. ⁹Be deduced levls, J, π, Γ, Γn.

doi: 10.1016/0375-9474(70)91093-6
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1970GO11      Phys.Rev. C1, 1939 (1970)

D.R.Goosman, R.W.Kavanagh

¹⁰Be(d, p)¹¹Be and the ¹⁰Be(d, α)⁸Li Reactions

NUCLEAR REACTIONS ¹⁰Be(d, α), E=0.67-3 MeV; ¹⁰Be(d, p), E=2.3-12 MeV; measured σ(Eα, θ), σ(Ep, θ); deduced Q. ¹¹Be deduced level, J, π, S.

doi: 10.1103/PhysRevC.1.1939
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1970KA08      Nucl.Phys. A146, 410 (1970)

R.W.Kavanagh, J.C.Merdinger, N.Schulz

Lifetime Measurements for the First Five Excited States in ³³S

NUCLEAR REACTIONS ³⁰Si(α, nγ), E=6.5-7.5 MeV; measured Doppler-shift attenuation. ³³S levels deduced T_1/2. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(70)90734-7
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1970LI06      Phys.Rev. C1, 816 (1970)

W.-K.Lin, F.Scheibling, R.W.Kavanagh

Investigations of the First Excited State of ⁴He via the Reaction ⁷Li(p, α)

NUCLEAR REACTIONS ⁷Li(p, α), E=9.1 MeV; measured σ(Eα, Ep, Et, θ(αp), θ(αt), θ((α)(³He))). ⁴He deduced resonance, J, π.

doi: 10.1103/PhysRevC.1.816
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1969KA18      Rev.Phys.Appl. 4, 215 (1969)

R.W.Kavanagh, N.Schulz, J.C.Merdinger

Lifetimes by Doppler Shift Using Solid and Gaseous Stopping Media

NUCLEAR REACTIONS ³⁰Si, ³⁷Cl, ⁴⁰Ar(α, n), ³⁵Cl(α, p), E approx threshold; measured Doppler shift attenuation. ³³S, ³⁸Ar, ⁴⁰K, ⁴³Ca levels deduced T_1/2. Ge(Li) detector.

doi: 10.1051/rphysap:0196900402021500
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1969KA41      Nucl.Phys. A129, 172 (1969)

R.W.Kavanagh

Gamow-Teller β-decays and M1 γ-rays in A = 4N+2 nuclei

RADIOACTIVITY ⁶He, ¹⁴C, ¹⁸Ne, ³⁰P(β^-), ¹⁰C, ¹⁴O, ¹⁸F, ²²Mg, ²⁶Al, ²⁶Si, ³⁰S(EC); analyzed available data; deduced an approximate sum rule for the Gamow-Teller strengths.

doi: 10.1016/0375-9474(69)90918-X
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1968KA15      Phys.Rev. 175, 1426 (1968)

R.W.Kavanagh, A.Gallmann, E.Aslanides, F.Jundt, E.Jacobs

Positron Decay of ³⁸Ca and ³⁸K

NUCLEAR STRUCTURE ¹⁴O, ³⁸K, ³⁸Ca, ³⁷K, ³⁵Ar, ³⁴Cl; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1426
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1968ME14      Nucl.Phys. A115, 204(1968)

J.C.Merdinger, N.Schulz, R.W.Kavanagh

Duree de Vie du Niveau Excite a 472 keV dans le ⁴³Sc

NUCLEAR REACTIONS ⁴⁰Ca(α, p), E = 10 MeV; measured pγ-delay. ⁴³Sc level deduced T_1/2. Natural target.

doi: 10.1016/0375-9474(68)90653-2
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1967GO09      Phys.Letters 24B, 507 (1967)

D.R.Goosman, R.W.Kavanagh

The Energy, Lifetime, and Spin of the 1611 keV Level in ³⁷Ar

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

doi: 10.1016/0370-2693(67)90409-1
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1967GO18      Phys.Rev. 161, 1156 (1967)

D.R.Goosman, R.W.Kavanagh

Nuclear Energy Levels of ³⁷K

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

doi: 10.1103/PhysRev.161.1156
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1967MI02      Nucl.Phys. A94, 261 (1967)

R.G.Miller, R.W.Kavanagh

Masses and Excitation Energies of Some Proton-Rich Nuclei

NUCLEAR REACTIONS ²⁴Mg, ²⁸Si, ³²S, ⁴⁰Ca(³He, n), ⁴⁶Ti, ⁵⁴Fe, ⁵⁸Ni(³He, n), (³He, p), E = 10-12 MeV; measured σ(En), σ(Ep); deduced Q. ²⁸Si(³He, n), E = 11.6 MeV; measured σ(θ). ⁵⁴Fe(³He, nγ), E = 11.5 MeV; measured Eγ. ²⁶Si, ³⁰S, ³⁴Ar, ⁴⁸V, ⁴⁸Cr, ⁵⁶Co, ⁵⁶Ni, ⁶⁰Cu, ⁶⁰Zn deduced levels, masses. Enriched ⁴⁶Ti, ⁵⁴Fe, ⁵⁸Ni targets.

doi: 10.1016/0375-9474(67)90003-6
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1967MI08      Nucl.Instr.Methods 48, 13 (1967)

R.G.Miller, R.W.Kavanagh

Semiconductor Detector as a Fast Neutron Spectrometer

NUCLEAR STRUCTURE ²⁶Mg, ²⁵Mg, ²⁸Al; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-554X(67)90456-9
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1966KA03      Phys.Rev. 143, 779 (1966)

R.W.Kavanagh, P.D.Parker

He³+p Elastic Scattering below 1 MeV

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

doi: 10.1103/PhysRev.143.779
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1966MI11      Phys.Letters 22, 461 (1966)

R.G.Miller, R.W.Kavanagh

Decay of ³⁴Ar

NUCLEAR STRUCTURE ³⁴Cl, ³⁴Ar; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)91227-3
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1966MI12      Nucl.Phys. 88, 492(1966)

R.G.Miller, R.W.Kavanagh

The Reaction ⁹Be(α, n)¹²C

NUCLEAR REACTIONS ⁹Be(α, n₀), E = 5.0-12.0 MeV; ⁹Be(α, n₁), E = 4.3-12.0; ⁹Be(α, n₂), E = 6.0-10.1; measured σ(E, θ = 0°). ¹³C deduced levels.

doi: 10.1016/0029-5582(66)90408-1
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1966PU02      Nucl.Phys. 83, 513(1966)

P.Purdom, Jr., P.A.Seeger, R.W.Kavanagh

Electromagnetic Decay of the 1.7 and 2.43 MeV Levels in ⁹Be

NUCLEAR REACTIONS ¹¹B(d, αγ), E = 1.70 MeV; measured γ-width/level-width for ⁹Be levels. ⁹Be levels deduced level-width. Natural target.

doi: 10.1016/0029-5582(66)90109-X
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1965MI01      Bull.Am.Phys.Soc. 10, No.1, 10, AC14 (1965)

R.G.Miller, R.W.Kavanagh

Mass Measurements Using (He³, n) Reactions

1964GO16      Bull.Am.Phys.Soc. 9, No.7, 705, B14 (1964)

D.R.Goosman, R.W.Kavanagh

Energy Levels in K³⁷

NUCLEAR STRUCTURE ³⁶Ar, ³⁷K; measured not abstracted; deduced nuclear properties.

1964KA08      Phys.Rev. 133, B1504 (1964)

R.W.Kavanagh

Q Values for B¹⁰(He³, n)N¹² and N¹²

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

doi: 10.1103/PhysRev.133.B1504
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1964KA13      Bull.Am.Phys.Soc. 9, No.5, 562, S7 (1964)

R.W.Kavanagh, D.R.Goosman

Branching in ³⁷K Positron Decay

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

1964KA24      Phys.Letters 12, 229 (1964); Erratum Phys.Letters 13, 358 (1964)

R.W.Kavanagh, D.R.Goosman

Energy Levels in K³⁷ and Ar³⁷, and Beta Decay of K³⁷

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

doi: 10.1016/0031-9163(64)91084-4
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1964PU04      Bull.Am.Phys.Soc. 9, No.7, 704, B8 (1964)

P.Purdom, P.A.Seeger, R.W.Kavanagh

Electromagnetic Decay of the 2.43-MeV State of Be⁹

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

1963KA28      Bull.Am.Phys.Soc. 8, No.8, 597, F1 (1963)

R.W.Kavanagh, P.D.Parker, G.D.Symons

He³(p, p) Elastic Scattering

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

1963MI18      Bull.Am.Phys.Soc. 8, No.8, 599, F12 (1963)

R.G.Miller, R.W.Kavanagh, G.Goldring

Mass of Ni⁵⁶

NUCLEAR STRUCTURE ⁵⁶Ni; measured not abstracted; deduced nuclear properties.

1963PA02      Bull.Am.Phys.Soc. 8, No.1, 37, J9 (1963)

P.D.Parker, R.W.Kavanagh

Absolute Cross Section of the Direct-Capture Reaction He³(α, γ)Be⁷

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

1963PA12      Phys.Rev. 131, 2578 (1963)

P.D.Parker, R.W.Kavanagh

He³(α, γ)Be⁷ Reaction

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

doi: 10.1103/PhysRev.131.2578
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1963SE17      Astrophys.J. 137, 704 (1963)

P.A.Seeger, R.W.Kavanagh

The 7.66-MeV State of C¹² and Helium-Burning

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

doi: 10.1086/147548
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1963SE23      Nucl.Phys. 46, 577 (1963)

P.A.Seeger, R.W.Kavanagh

Electromagnetic decay of the second excited state of C¹²

NUCLEAR REACTIONS ¹⁴N(d, α), E=1.8 MeV; measured Eα, (¹²C)α-coinc. ¹²C deduced radiative width of the second excited state.

doi: 10.1016/0029-5582(63)90630-8
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1962KA10      Bull.Am.Phys.Soc. 7, No.7, 462, IA5 (1962)

R.W.Kavanagh

Decay of Mg²²

NUCLEAR STRUCTURE ²²Mg; measured not abstracted; deduced nuclear properties.

1962SE07      Bull.Am.Phys.Soc. 7, No.7, 471, LA8 (1962)

P.A.Seeger, R.W.Kavanagh

N¹⁴(d, α)C^12*(7.656 MeV)

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

1960KA05      Nuclear Phys. 15, 411 (1960)

R.W.Kavanagh

Proton Capture in Be⁷

NUCLEAR STRUCTURE ⁸B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(60)90322-9
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1960KA17      Nuclear Phys. 18, 492 (1960)

R.W.Kavanagh

Protons from Deuteron Bombardment of Be⁷

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

doi: 10.1016/0029-5582(60)90419-3
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1959BA27      Phys.Rev.Letters 3, 518 (1959)

S.Bashkin, R.W.Kavanagh, P.D.Parker

Search for Li⁴

doi: 10.1103/PhysRevLett.3.518
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1959KA14      Bull.Am.Phys.Soc. 4, No.8, 444, C4 (1959)

R.W.Kavanagh

Be⁷(p, γ)B⁸ and Be⁷(d, p)Be⁸ Cross-Section Measurements

1959PA09      Bull.Am.Phys.Soc. 4, No.8, 443, C2 (1959)

P.D.Parker, S.Bashkin, R.W.Kavanagh

Investigation of the He³(p, γ), Li⁴ Reaction

1958KA14      Bull.Am.Phys.Soc. 3, No.5, 316, B7 (1958)

R.W.Kavanagh

Coincidence Studies of B¹² and F²⁰

1958KA31      Phys.Rev. 112, 503 (1958)

R.W.Kavanagh, C.A.Barnes

Boron Plus Deuteron Reactions

doi: 10.1103/PhysRev.112.503
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1956MA71      Phys.Rev. 104, 107 (1956)

J.B.Marion, R.W.Kavanagh

Q Value for the Cu⁶⁵(p, n)Zn⁶⁵ Reaction

doi: 10.1103/PhysRev.104.107
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1955BA14      Phys.Rev. 100, 1796A (1955)

C.A.Barnes, R.W.Kavanagh

15-MeV Gamma Radiation from B¹¹ + d

doi: 10.1103/PhysRev.100.1796A
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