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NSR database version of April 11, 2024.

Search: Author = P.Pella

Found 11 matches.

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1997PL01      Phys.Rev. C56, 263 (1997)

M.R.Plumley, J.W.Watson, B.D.Anderson, A.R.Baldwin, C.C.Foster, R.Madey, P.J.Pella, E.Ramstrom, W.Unkelbach, Y.Wang

Spin Observables for the 208Pb(p, n)208Bi Reaction at 135 MeV

NUCLEAR REACTIONS 208Pb(polarized p, n), E=135.7 MeV; measured reaction σ(E, θ), analyzing power vs E(neutron), spin observables; deduced spin-flip probability. 48Ca(polarized p, n), E not given; analyzed reaction σ, spin-flip probability. Neutron polarimeter, DWIA-RPA calculations.

doi: 10.1103/PhysRevC.56.263
Citations: PlumX Metrics


1996WA09      Nucl.Phys. A599, 211c (1996)

J.W.Watson, B.D.Anderson, A.R.Baldwin, R.Madey, M.Plumley, D.Prout, C.C.Foster, P.J.Pella, S.N.Ershov, F.A.Gareev, E.L.Trykov

Spin Observables for the Isovector Spin-Dipole Resonance Seen in 40Ca(p(pol), n(pol))

NUCLEAR REACTIONS 40Ca(polarized p, n), E=135 MeV; measured polarization transfer coefficient, σ(θ) vs energy transfer. 40Sc deduced isovector spin-dipole resonances, J, π. DWIA, finite Fermi systems theory.

doi: 10.1016/0375-9474(96)00063-2
Citations: PlumX Metrics


1995PA37      Phys.Rev. C52, 2552 (1995)

W.Pairsuwan, J.W.Watson, M.Ahmad, N.S.Chant, B.S.Flanders, R.Madey, P.J.Pella, P.G.Roos

Analyzing Powers for the 2H(p(pol), pn)1H Reaction at 200 MeV

NUCLEAR REACTIONS 2H(polarized p, np), E=200 MeV; measured σ(θp, θn, Ep), analyzing power vs θ.

doi: 10.1103/PhysRevC.52.2552
Citations: PlumX Metrics


1994ED01      Phys.Rev. C50, R1749 (1994)

T.Eden, R.Madey, W.-M.Zhang, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, M.Farkhondeh, J.M.Finn, B.S.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, D.M.Manley, P.Markowitz, J.Mougey, B.Ni, T.Payerle, P.J.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney

Electric Form Factor of the Neutron from the 2H(e(pol), e'n(pol))1H Reaction at Q2 = 0.255 (GeV/c)2

NUCLEAR REACTIONS 2H(polarized e, e'n), E=868 MeV; measured neutron polarization. 1n deduced electric form factor.

doi: 10.1103/PhysRevC.50.R1749
Citations: PlumX Metrics


1994ED02      Nucl.Instrum.Methods Phys.Res. A338, 432 (1994)

T.Eden, R.Madey, W.-M.Zhang, B.D.Anderson, A.R.Baldwin, J.M.Cameron, J.M.Finn, C.C.Foster, J.J.Kelly, S.Kowalski, R.Lourie, P.Markowitz, B.Ni, P.J.Pella, J.Schambach, M.Spraker, E.Steinfelds, E.J.Stephenson, J.W.Watson

Performance of a Neutron Polarimeter to Measure the Electric Form Factor of the Neutron

NUCLEAR REACTIONS 14C(polarized p, n), E=138.4 MeV; measured neutron spectra, analyzing power; deduced method suitability for 1n electric form factor extriction studies.

doi: 10.1016/0168-9002(94)91327-7
Citations: PlumX Metrics


1994WA24      Nucl.Phys. A577, 79c (1994)

J.W.Watson, B.D.Anderson, A.R.Baldwin, C.C.Foster, D.Lamm, R.Madey, M.R.Plumley, P.J.Pella

The Spin-Dipole Resonance in (p(pol), n(pol)) on 16O and 40Ca

NUCLEAR REACTIONS 16O, 40,48Ca, 208Pb(polarized p, n), E=135 MeV; measured spin observable D(NN')(θ); analyzed σ(θ) vs excitation, 0° neutron spectra data. 16F, 40,48Sc, 208Bi deduced spin dipole resonance features.

doi: 10.1016/0375-9474(94)90837-0
Citations: PlumX Metrics


1993MA21      Phys.Rev. C48, R5 (1993)

P.Markowitz, J.M.Finn, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, T.Eden, M.Farkhondeh, B.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, R.Madey, D.M.Manley, J.Mougey, B.Ni, T.Payerle, P.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney, W.M.Zhang

Measurement of the Magnetic Form Factor of the Neutron

NUCLEAR REACTIONS 2H(e, e'n), E not given; measured en-coin. 1n deduced magnetic form factor. Associated particle technique.

doi: 10.1103/PhysRevC.48.R5
Citations: PlumX Metrics


1992ZH09      Phys.Rev. C45, 2819 (1992)

W.-M.Zhang, B.D.Anderson, A.R.Baldwin, T.Eden, D.M.Manley, R.Madey, E.Steinfelds, J.W.Watson, P.J.Pella, C.C.Foster

P - A in the 48Ca(p, n)48Sc Reaction at 135 MeV

NUCLEAR REACTIONS 48Ca(polarized p, n), E=135 MeV; measured P(θ), analyzing power vs θ; deduced non-local effects. 48Sc levels deduced (P-A) differences, configurations role. DWIA analysis.

doi: 10.1103/PhysRevC.45.2819
Citations: PlumX Metrics


1988WA25      Nucl.Instrum.Methods Phys.Res. A272, 750 (1988)

J.W.Watson, M.R.Plumley, P.J.Pella, B.D.Anderson, A.R.Baldwin, R.Madey

A High-Performance Polarimeter for Medium-Energy Neutrons

NUCLEAR REACTIONS 14C(polarized p, n), E=100 MeV; measured polarized neutron spectra. High performance polarimeter.

doi: 10.1016/0168-9002(88)90756-5
Citations: PlumX Metrics


1986WA28      Phys.Lett. 181B, 47 (1986)

J.W.Watson, P.J.Pella, B.D.Anderson, A.R.Baldwin, T.Chittrakarn, B.S.Flanders, R.Madey, C.C.Foster, I.J.van Heerden

Gamow-Teller and Spin-Dipole Strength in the 40,48Ca(p(pol), n(pol)) Reactions at 135 MeV

NUCLEAR REACTIONS, MECPD 40,48Ca(polarized p, n), E=135 MeV; measured σ(En, θ), spin flip probabilities, neutron polarization vs θ, polarization transfer coefficient. 48Ca deduced 1+ strength in continuum near giant Gamow-Teller resonance. 40Ca deduced dipole resonance spin-flip, nonspin-flip component relative width.

doi: 10.1016/0370-2693(86)91252-9
Citations: PlumX Metrics


1984WA21      J.Phys.(Paris), Colloq.C-4, 91 (1984)

J.W.Watson, P.J.Pella, M.Ahmad, B.S.Flanders, N.S.Chant, P.G.Roos, D.W.Devins, D.L.Friesel

Neutron Deep-Hole States from the (p, pn) Reaction

NUCLEAR REACTIONS 2H, 9Be, 16O, 28Si, 58Ni, 90Zr(polarized p, np), E=148.8 MeV; measured separation energy spectra, σ(Ep, θp, θn), analyzing powers. 8Be, 15O, 27Si, 57Ni, 89Zr deduced tentative deep-hole neutron states. Si, Ge detectors, tof. DWIA calculations.


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Note: The following list of authors and aliases matches the search parameter P.Pella: , P.J.PELLA