NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = H.Funsten Found 27 matches. 2000MA25 Nucl.Phys. A663-664, 671c (2000) J.J.Manak, V.Burkert, F.Klein, B.Mecking, A.Coleman, H.Funsten, for the CLAS Collaboration Electro- and Photoproduction of ω(783) Mesons using CLAS at Jefferson Lab NUCLEAR REACTIONS 1H(γ, X), E=0.5-2.3 GeV; 1H(e, X), E=4 GeV; measured ω meson production σ(θ).
doi: 10.1016/S0375-9474(99)00713-7
1997MA25 Phys.Rev.Lett. 78, 4343 (1997) M.May, D.Alburger, S.Bart, R.Chrien, R.Sawafta, M.Deutsch, V.Lia, S.W.Wissink, J.Lisantti, S.P.Wells, S.M.Bowyer, W.A.Franklin, K.Hicks, H.Clark, R.Michael, L.Lee, H.Funsten, C.Kormanyos, J.Wise, M.B.Barakat, R.Stearns First Observation of the p(Λ) → s(Λ) γ-Ray Transition in 13C(Λ) NUCLEAR REACTIONS 13C(K-, π-), E at 750 MeV/c; measured γ(hypernucleus)-coin, excitation spectra; deduced p(λ) → s(λ) transition in hypernucleus 13C(λ).
doi: 10.1103/PhysRevLett.78.4343
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
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
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
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
1984FA11 Phys.Rev. C30, 1622 (1984) J.A.Faucett, B.E.Wood, D.K.McDaniels, P.A.M.Gram, M.E.Hamm, M.A.Oothoudt, C.A.Goulding, L.W.Swenson, K.S.Krane, A.W.Stetz, H.S.Plendl, J.Norton, H.Funsten, D.Joyce Kinematically Complete Measurement of the (π±, π±p) Reaction on 12C at 220 MeV NUCLEAR REACTIONS 12C(π+, π+p), (π-, π-p), (π-, π-'), (π+, π+'), E=220 MeV; measured σ(θ(π), E(π)), σ(θ(π), θ(p), E(p)), σ(θ(π), θ(p), E(π)), σ(θ(π), θ(p)), σ(θ(π), θ(p)) vs missing mass; deduced reaction mechanism. Kinematically complete experiment.
doi: 10.1103/PhysRevC.30.1622
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
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
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
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
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
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
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
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
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
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
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
1974LI15 Phys.Rev. C10, 1753 (1974) 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
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
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
1964RO02 Bull.Am.Phys.Soc. 9, No.1, 93, JC9 (1964) 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) 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) 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) 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
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