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NSR database version of April 11, 2024.

Search: Author = H.O.Funsten

Found 24 matches.

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1996NA04      Phys.Rev. C53, 811 (1996)

R.Nair, H.S.Plendl, E.P.Gavathas, L.-C.Liu, R.J.Estep, B.J.Dropesky, J.D.Bowman, J.N.Knudson, B.J.Lieb, C.E.Stronach, H.O.Funsten, J.Mackenzie

Pion-Nucleus Single Charge Exchange Induced by Stopped Negative Pions

NUCLEAR REACTIONS 12C, 1H, 27Al, 31P, 32S, 45Sc, 115In(π-, π0), E at rest; measured branching ratio; deduced πN-isovector interaction implications.

doi: 10.1103/PhysRevC.53.811
Citations: PlumX Metrics

1993PL08      Acta Phys.Pol. B24, 1649 (1993)

H.S.Plendl, R.Nair, E.P.Gavathas, L.C.Liu, R.J.Estep, B.J.Dropesky, J.D.Bowman, J.N.Knudson, B.J.Lieb, C.E.Stronach, H.O.Funsten, J.MacKenzie

Single Charge Exchange following π- Capture

NUCLEAR REACTIONS C, 1H, 27Al, 31P, 32S, 45Sc, 115In(π-, π0), E ≈ threshold; measured branching ratio relative to (π-, X); deduced target shell structure role.

1992LY01      Phys.Rev. C45, 308 (1992)

C.R.Lyndon, H.O.Funsten, C.F.Perdrisat, V.Punjabi, J.M.Finn, B.J.Lieb, C.E.Stronach, N.L.Fuqua, H.S.Plendl, J.R.Mackenzie, R.Nair, J.R.Comfort, R.A.Giannelli, J.J.Reidy, L.Redmond, P.E.Koehler, S.A.Wender

Coincidence Analyzing-Power Measurements of the Reaction 12C(p(pol), p'γ)12C(*) Through the 15.11-MeV State

NUCLEAR REACTIONS 12C(polarized p, p'γ), E=318 MeV; measured coincidence analyzing powers vs φp. Relativistic, non-relativistic DWBA.

doi: 10.1103/PhysRevC.45.308
Citations: PlumX Metrics

1988CH49      Phys.Rev.Lett. 60, 2595 (1988)

R.E.Chrien, S.Bart, P.Pile, R.Sutter, N.Tsoupas, H.O.Funsten, J.M.Finn, C.Lyndon, V.Punjabi, C.F.Perdrisat, B.J.Lieb, T.Kishimoto, L.C.Liu, R.Estep, B.Dropesky, C.E.Stronach, R.L.Stearns

Search for Bound States in the η Meson in Light Nuclei

doi: 10.1103/PhysRevLett.60.2595
Citations: PlumX Metrics

1986JO12      Phys.Rev. C34, 1813 (1986)

D.Joyce, H.O.Funsten, B.J.Lieb, H.S.Plendl, J.Norton, C.E.Stronach, V.G.Lind, R.E.McAdams, O.H.Otteson, L.W.Swenson, C.Pillai, D.J.Vieira, A.J.Buffa

200-MeV-π+-Induced Single-Nucleon Removal from 24Mg

NUCLEAR REACTIONS 24Mg(π+, π+pγ), (π+, π+nγ), E=200 MeV; measured γp-, γπ+-coin, σ(θ), σ. Ge(Li) detector, particle telescopes. PWIA, intranuclear cascade calculations.

doi: 10.1103/PhysRevC.34.1813
Citations: PlumX Metrics

1984ST17      J.Phys.(London) G10, 1249 (1984)

C.E.Stronach, H.O.Funsten, W.J.Kossler, D.Joyce, B.J.Lieb, W.F.Lankford, H.S.Plendl, V.G.Lind

Nuclear γ Rays from π± - Induced Nucleon Removal Reactions on 23Na, 31P and 32S

NUCLEAR REACTIONS 23Na, S, 31P(π+, xn), (π+, xp), (π+, xα), E=180 MeV; 23Na, S, 31P(π-, xn), (π-, xp), (π-, xα), E=220 MeV; measured πγ-coin, Eγ, production σ, yields for 21Na, 21,20,19Ne, 20,19,18F, 18,17,16O, 15N; deduced reaction mechanism. Intranuclear cascade, statistical evaporation model.

doi: 10.1088/0305-4616/10/9/013
Citations: PlumX Metrics

1982LI15      Phys.Rev. C26, 2084 (1982)

B.J.Lieb, H.S.Plendl, C.E.Stronach, H.O.Funsten, V.G.Lind

(π±, πN) Reactions on 14N, 19F, 23Na, 27Al, and 31P near the Δ(1232) Resonance

NUCLEAR REACTIONS 14N, 19F, 23Na, 27Al, 31P(π+, π+p), (π-, π-n), E ≈ 200 MeV; measured residuals σ(θ=90°); deduced reaction mechanism. 13C, 18F, 18O, 22Na, 22Ne, 26Al, 26Mg, 30P levels deduced total σ(-)/σ(+). Final state nucleon exchange model.

doi: 10.1103/PhysRevC.26.2084
Citations: PlumX Metrics

1981ST05      Phys.Rev. C23, 2150 (1981)

C.E.Stronach, B.J.Lieb, H.O.Funsten, W.J.Kossler, H.S.Plendl, V.G.Lind

Absence of Jπ, T = 0+, 1 Level Excitations in Residual Nuclei from (π±, 2N) Reactions

NUCLEAR REACTIONS 12C, 32S(π+, X), E=180 MeV; 12C, 32S(π-, X), E=0, 220 MeV; measured Eγ, πγ-coin; deduced reaction mechanism, two-nucleon removal σ. 10B, 30P levels deduced selective population by two-nucleon removal.

doi: 10.1103/PhysRevC.23.2150
Citations: PlumX Metrics

1980LI14      Phys.Rev. C22, 1612 (1980)

B.J.Lieb, H.S.Plendl, H.O.Funsten, C.E.Stronach, V.G.Lind

Nuclear γ Rays from 720-MeV α-Induced Reactions on 27Al and 28Si

NUCLEAR REACTIONS 27Al, 28Si(α, Xγ), E=720 MeV; measured Eγ, Iγ, Doppler broadening. 27Si, 27,26,25Al, 26,25,24,22Mg, 23,22,21Na, 22,21,20,19,18Ne, 20,19,18F, 20,18,17,16,15O, 15N, 15,13,12C, 10B levels deduced production σ. 27Si, 27Al, 26,24Mg, 12C levels deduced widths. Spallation yield calculations.

doi: 10.1103/PhysRevC.22.1612
Citations: PlumX Metrics

1979LI11      Phys.Rev. C19, 2405 (1979)

B.J.Lieb, H.S.Plendl, C.E.Stronach, H.O.Funsten, V.G.Lind

Evidence for the Quasifree Character of the (π±, πN) Reactions on 12C, 24Mg, and 40Ca

NUCLEAR REACTIONS C, Mg, Ca(π+, πp), (π+, πn), (π-, πp), (π-, πn), E=200 MeV; measured Eγ, Iγ, σ. 11C, 11B, 23Mg, 23Na, 39Ca, 39K deduced ratio of σ for mirror levels.

doi: 10.1103/PhysRevC.19.2405
Citations: PlumX Metrics

1978FU07      Phys.Lett. 78B, 357 (1978)

H.O.Funsten, W.J.Kossler, B.J.Lieb, V.G.Lind, H.S.Plendl, C.E.Stronach

Nuclear γ-Rays Produced by 200 MeV (π+, π0) Charge Exchange on Cr And Ni

NUCLEAR REACTIONS Cr, Ni(π+, π0γ), E=200 MeV; measured Eγ. Ge(Li) detector.

1978LI18      Phys.Rev. C18, 1368 (1978)

B.J.Lieb, H.O.Funsten, C.E.Stronach, H.S.Plendl, V.G.Lind

π±-Induced Multinucleon Removal from 27Al and 28Si

NUCLEAR REACTIONS 28Si, 27Al(π+, X), E=190 MeV; 28Si, 27Al(π-, X), E=220 MeV; measured σ for multinucleon removal, σ(Eγ). Ge(Li) detector.

doi: 10.1103/PhysRevC.18.1368
Citations: PlumX Metrics

1978ST17      Nucl.Phys. A308, 290 (1978)

C.E.Stronach, H.S.Plendl, H.O.Funsten, W.J.Kossler, B.J.Lieb, V.G.Lind

Interactions of Stopped π- and of Fast π- and π+ Near the Δ(1232) Resonance with Calcium

NUCLEAR REACTIONS Ca(π-, X), E(av)=0, 220 MeV; Ca(π+, X), E(av)=180 MeV; measured relative γ-ray yields at θ=90°; calculated σ, nuclear recoil momenta.

doi: 10.1016/0375-9474(78)90552-3
Citations: PlumX Metrics

1977FU08      Phys.Rev. C16, 1521 (1977)

H.O.Funsten, W.J.Kossler. B.J.Lieb, H.S.Plendl, C.E.Stronach, V.G.Lind

Nuclear Gamma Rays from 51V Levels Populated by 200 MeV π± Inelastic Scattering

NUCLEAR REACTIONS 51V(π+, π+'γ), (π-, π-'γ), E=200 MeV; measured σ(Eγ) to levels in 51V.

doi: 10.1103/PhysRevC.16.1521
Citations: PlumX Metrics

1977ST09      Phys.Rev. C15, 984 (1977)

C.E.Stronach, W.J.Kossler, H.O.Funsten, W.F.Lankford, B.J.Lieb

Recoil-Momentum Spectrum of 12C* from π- Capture on 14N

NUCLEAR REACTIONS 14N(π-,12C), E=0 MeV; measured Eγ, Doppler broadening; deduced recoil momentum spectrum.

doi: 10.1103/PhysRevC.15.984
Citations: PlumX Metrics

1976LI18      Phys.Rev. C14, 1515 (1976)

B.J.Lieb, W.F.Lankford, S.H.Dam, H.S.Plendl, H.O.Funsten, W.J.Kossler, V.G.Lind, A.J.Buffa

Negative Pion Interactions with 19F, 27Al, and 51V Near the Δ(1232) Resonance

NUCLEAR REACTIONS 19F, 27Al, 51V(π-, X), E ≈ 230 MeV; measured γ yields; deduced σ, nuclear recoil momenta.

doi: 10.1103/PhysRevC.14.1515
Citations: PlumX Metrics

1975LI06      Phys.Rev.Lett. 34, 965 (1975)

B.J.Lieb, H.S.Plendl, H.O.Funsten, W.J.Kossler, C.E.Stronach

Cross Section Ratios for (π±, πN) Reactions on 16O Near the Δ(1236)

NUCLEAR REACTIONS 16O(π+, πX), (π-, πX), E=200 MeV; measured relative σ.

doi: 10.1103/PhysRevLett.34.965
Citations: PlumX Metrics

1974LI15      Phys.Rev. C10, 1753 (1974)

B.J.Lieb, H.O.Funsten

Gamma Rays Emitted Following the Interaction of 230-MeV Negative Pions With 16O

NUCLEAR REACTIONS 16O(π-, X), E=230 MeV; measured relative γ yields; deduced σ for levels in 10B, 12,13,14C, 14,15,16N, 15,16O.

doi: 10.1103/PhysRevC.10.1753
Citations: PlumX Metrics

1971KO23      Phys.Rev. C4, 1551 (1971)

W.J.Kossler, H.O.Funsten, B.A.MacDonald, W.F.Lankford

Nuclear Deexcitation γ Rays in 14N, 14C, and 15N Following π- Capture in 16O

NUCLEAR REACTIONS O(π-, Xγ), E approx o; measured Eγ, Iγ. 14,15N, 14C deduced transitions.

doi: 10.1103/PhysRevC.4.1551
Citations: PlumX Metrics

1964FU07      Phys.Rev. 134, B117 (1964)

H.O.Funsten, N.R.Roberson, E.Rost

Inelastic Proton Scattering from Nuclei with 28 Neutrons

NUCLEAR STRUCTURE 54Fe, 52Cr, 50Ti, 51V; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.134.117
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1326.

1964RO02      Bull.Am.Phys.Soc. 9, No.1, 93, JC9 (1964)

N.R.Roberson, H.O.Funsten

Inelastic Scattering of Protons by Ni58,60,62

NUCLEAR STRUCTURE 60Ni, 58Ni, 62Ni; measured not abstracted; deduced nuclear properties.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1318.

1963FU03      Bull.Am.Phys.Soc. 8, No.4, 367, R8 (1963)

H.O.Funsten, N.R.Roberson

Inelastic Proton Scattering in the f7/2 Shell

NUCLEAR STRUCTURE 51V, 59Co; measured not abstracted; deduced nuclear properties.

1963RO08      Bull.Am.Phys.Soc. 8, No.4, 367, R9 (1963)

N.R.Roberson, H.O.Funsten

Inelastic Proton Scattering in the f7/2 Shell. II

NUCLEAR STRUCTURE 52Cr, 54Fe, 56Fe, 58Fe, 50Ti; measured not abstracted; deduced nuclear properties.

1962WA31      Phys.Rev. 128, 1810 (1962)

E.K.Warburton, H.O.Funsten

High-Energy Gamma Rays and Low-Energy Protons and Deuterons from C12 + p for Ep = 14-20 MeV

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

doi: 10.1103/PhysRev.128.1810
Citations: PlumX Metrics

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