NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.J.Seestrom Found 107 matches. Showing 1 to 100. [Next]2018PA53 Science 360, 627 (2018) R.W.Pattie, N.B.Callahan, C.Cude-Woods, E.R.Adamek, L.J.Broussard, S.M.Clayton, S.A.Currie, E.B.Dees, X.Ding, E.M.Engel, D.E.Fellers, W.Fox, P.Geltenbort, K.P.Hickerson, M.A.Hoffbauer, A.T.Holley, A.Komives, C.-Y.Liu, S.W.T.MacDonald, M.Makela, C.L.Morris, J.D.Ortiz, J.Ramsey, D.J.Salvat, A.Saunders, S.J.Seestrom, E.I.Sharapov, S.K.Sjue, Z.Tang, J.Vanderwerp, B.Vogelaar, P.L.Walstrom, Z.Wang, W.Wei, H.L.Weaver, J.W.Wexler, T.L.Womack, A.R.Young, B.A.Zeck Measurement of the neutron lifetime using a magneto-gravitational trap and in situ detection RADIOACTIVITY 1NN(β-); measured T1/2 of free neutron using ultracold neutrons stored in a magneto-gravitational trap at the Los Alamos Neutron Science Center UCN facility. Comparison with previous measurements.
doi: 10.1126/science.aan8895
2017SE02 Phys.Rev. C 95, 015501 (2017) S.J.Seestrom, E.R.Adamek, D.Barlow, M.Blatnik, L.J.Broussard, N.B.Callahan, S.M.Clayton, C.Cude-Woods, S.Currie, E.B.Dees, W.Fox, M.Hoffbauer, K.P.Hickerson, A.T.Holley, C.-Y.Liu, M.Makela, J.Medina, D.J.Morley, C.L.Morris, R.W.Pattie, J.Ramsey, A.Roberts, D.J.Salvat, A.Saunders, E.I.Sharapov, S.K.L.Sjue, B.A.Slaughter, P.L.Walstrom, Z.Wang, J.Wexler, T.L.Womack, A.R.Young, J.Vanderwerp, B.A.Zeck Total cross sections for ultracold neutrons scattered from gases NUCLEAR REACTIONS 1H, 3He(n, n'), E=ultracold neutrons; measured scattered neutrons, transmission ratio as a function of pressure, total cross sections, total cross section as a function of the number of hydrogen atoms using the following gas targets: hydrogen, ethane, methane, isobutene, n-butane, ethylene, water vapor, propane, neopentane, isopropyl alcohol, and 3He; deduced cross section per hydrogen atom as a function of molecular mass. Relevance to ongoing experiments pn neutron half-life measurements using ultracold neutrons (UCN) at LANL facility.
doi: 10.1103/PhysRevC.95.015501
2015SE18 Phys.Rev. C 92, 065501 (2015) S.J.Seestrom, E.R.Adamek, D.Barlow, L.J.Broussard, N.B.Callahan, S.M.Clayton, C.Cude-Woods, S.Currie, E.B.Dees, W.Fox, P.Geltenbort, K.P.Hickerson, A.T.Holley, C.-Y.Liu, M.Makela, J.Medina, D.J.Morley, C.L.Morris, J.Ramsey, A.Roberts, D.J.Salvat, A.Saunders, E.I.Sharapov, S.K.L.Sjue, B.A.Slaughter, B.VornDick, P.L.Walstrom, Z.Wang, T.L.Womack, A.R.Young, B.A.Zeck, for the UCN|t Collaboration Upscattering of ultracold neutrons from gases NUCLEAR REACTIONS 1,2H, C, F, N, Ne, Ar, Xe(n, n'), E=UCNs from Los Alamos Neutron Science Center (LANSCE) ultracold neutron source; measured Eγ, Iγ, E(n), I(n), upscattered cross sections for room temperature gas targets of hydrogen, deuterium, nitrogen, neon, argon, xenon, C4H10, CF4, and air. Comparison with experimental values for higher neutron energies, and with theoretical calculations. Relevance to measurement of the half-life of free neutron decay at LANSCE using a magnetogravitational trap.
doi: 10.1103/PhysRevC.92.065501
2014SA31 Phys.Rev. C 89, 052501 (2014) D.J.Salvat, E.R.Adamek, D.Barlow, J.D.Bowman, L.J.Broussard, N.B.Callahan, S.M.Clayton, C.Cude-Woods, S.Currie, E.B.Dees, W.Fox, P.Geltenbort, K.P.Hickerson, A.T.Holley, C.-Y.Liu, M.Makela, J.Medina, D.J.Morley, C.L.Morris, S.I.Penttila, J.Ramsey, A.Saunders, S.J.Seestrom, E.I.Sharapov, S.K.L.Sjue, B.A.Slaughter, J.Vanderwerp, B.VornDick, P.L.Walstrom, Z.Wang, T.L.Womack, A.R.Young Storage of ultracold neutrons in the magneto-gravitational trap of the UCNT experiment RADIOACTIVITY 1n(β-); measured mean storage times of ultracold neutrons (UCN) in a magneto-gravitational trap at the LANSCE-LANL UCN source, with and without activation of the field; discussed half-life of neutron decay, and systematic effects.
doi: 10.1103/PhysRevC.89.052501
2013SH41 Phys.Rev. C 88, 037601 (2013) E.I.Sharapov, C.L.Morris, M.Makela, A.Saunders, E.R.Adamek, Y.Bagdasarova, L.J.Broussard, C.B.Cude-Woods, D.E.Fellers, P.Geltenbort, S.I.Hasan, K.P.Hickerson, G.Hogan, A.T.Holley, C.-Y.Liu, M.P.Mendenhall, J.Ortiz, R.W.Pattie, D.G.Phillips, J.Ramsey, D.J.Salvat, S.J.Seestrom, E.Shaw, S.K.L.Sjue, W.E.Sondheim, B.VornDick, Z.Wang, T.L.Womack, A.R.Young, B.A.Zeck Measurements of ultracold neutron upscattering and absorption in polyethylene and vanadium NUCLEAR REACTIONS 1H, V(n, n'), (n, γ), E=ultracold neutrons; measured E(n), I(n), Eγ, Iγ, ultra-cold neutron (UCN) upscattering and capture σ at UCN facility of LANL. Application to nuclear and particle physics, cosmology and gravity.
doi: 10.1103/PhysRevC.88.037601
2013SH46 Phys.Rev. C 88, 064605 (2013) E.I.Sharapov, C.L.Morris, M.Makela, A.Saunders, E.R.Adamek, L.J.Broussard, C.B.Cude-Woods, D.E.Fellers, P.Geltenbort, M.Hartl, S.I.Hasan, K.P.Hickerson, G.Hogan, A.T.Holley, C.M.Lavelle, C.-Y.Liu, M.P.Mendenhall, J.Ortiz, R.W.Pattie, D.G.Phillips, J.Ramsey, D.J.Salvat, S.J.Seestrom, E.Shaw, S.Sjue, W.E.Sondheim, B.VornDick, Z.Wang, T.L.Womack, A.R.Young, B.A.Zeck Upscattering of ultracold neutrons from the polymer [C6H12]n NUCLEAR REACTIONS 1H(n, n'), E=ultracold; measured spectra and rates of upscattered neutrons up to 100 meV range, shapes of spectra at LANSCE-LANL facility; deduced similar density of states in polyethylene (PE) and polymethylpentene (PMP) samples. Analysis using MCNP computer code.
doi: 10.1103/PhysRevC.88.064605
2004SA45 Phys.Lett. B 593, 55 (2004) A.Saunders, J.M.Anaya, T.J.Bowles, B.W.Filippone, P.Geltenbort, R.E.Hill, M.Hino, S.Hoedl, G.E.Hogan, T.M.Ito, K.W.Jones, T.Kawai, K.Kirch, S.K.Lamoreaux, C.-Y.Liu, M.Makela, L.J.Marek, J.W.Martin, C.L.Morris, R.N.Mortensen, A.Pichlmaier, S.J.Seestrom, A.Serebrov, D.Smith, W.Teasdale, B.Tipton, R.B.Vogelaar, A.R.Young, J.Yuan Demonstration of a solid deuterium source of ultra-cold neutrons
doi: 10.1016/j.physletb.2004.04.048
2002MO40 Phys.Rev.Lett. 89, 272501 (2002) C.L.Morris, J.M.Anaya, T.J.Bowles, B.W.Filippone, P.Geltenbort, R.E.Hill, M.Hino, S.Hoedl, G.E.Hogan, T.M.Ito, T.Kawai, K.Kirch, S.K.Lamoreaux, C.-Y.Liu, M.Makela, L.J.Marek, J.W.Martin, R.N.Mortensen, A.Pichlmaier, A.Saunders, S.J.Seestrom, D.Smith, W.Teasdale, B.Tipton, M.Utsuro, A.R.Young, J.Yuan Measurements of Ultracold-Neutron Lifetimes in Solid Deuterium
doi: 10.1103/PhysRevLett.89.272501
2002SM02 Phys.Rev. C65, 024607 (2002) D.A.Smith, J.D.Bowman, B.E.Crawford, C.A.Grossmann, T.Haseyama, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, A.M.Sukhovoj, V.W.Yuan Neutron Resonance Spectroscopy of 104Pd, 105Pd, and 110Pd NUCLEAR REACTIONS 104,105,110Pd(n, γ), (n, X), E=1-2100 MeV; measured transmission spectra, Eγ, Iγ. 106,108Pd(n, X), (n, γ), E not given; analyzed data. 104,105,106,108,110Pd deduced resonance parameters, level spacings, strength functions.
doi: 10.1103/PhysRevC.65.024607
2002SM04 Phys.Rev. C65, 035503 (2002) D.A.Smith, J.D.Bowman, B.E.Crawford, C.A.Grossmann, T.Haseyama, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, V.W.Yuan Parity Violation in Neutron Resonances of Palladium NUCLEAR REACTIONS Pd(polarized n, X), E=60-160 eV; measured transmission neutron spectra. 104,105,106,108Pd deduced resonance parameters, parity nonconservation asymmetries.
doi: 10.1103/PhysRevC.65.035503
2001MA55 Phys.Rev. C64, 015501 (2001) Y.Matsuda, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, T.Haseyama, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Masuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, Y.-F.Yen, V.W.Yuan Parity Violation in Neutron Resonances of Antimony and Iodine NUCLEAR REACTIONS 121,123Sb, 127I(polarized n, n'), E ≈ 5-350 eV; measured transmission neutron spectra. 121,123Sb, 127I deduced resonance parameters, parity-nonconserving asymmetries, weak spreading widths.
doi: 10.1103/PhysRevC.64.015501
2001SM07 Phys.Rev. C64, 015502 (2001) D.A.Smith, J.D.Bowman, B.E.Crawford, C.A.Grossmann, T.Haseyama, M.B.Johnson, A.Masaike, Y.Matsuda, G.E.Mitchell, V.A.Nazarenko, S.I.Penttila, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, L.M.Smotritsky, S.L.Stephenson, S.Tomsovic, V.W.Yuan Parity Violation in Neutron Resonances of 117Sn NUCLEAR REACTIONS 117Sn(polarized n, n'), E ≈ 0.8-1100 eV; measured neutron spectra. 117Sn deduced resonance parameters, parity-nonconserving asymmetries, weak spreading width.
doi: 10.1103/PhysRevC.64.015502
2000MI09 Phys.Rev. C61, 045503 (2000) G.E.Mitchell, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, M.Iinuma, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Matsuda, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, Y.-F.Yen, V.W.Yuan New Search for Parity Violation in Nonresonant Neutron Scattering on Thorium NUCLEAR REACTIONS 232Th(polarized n, n), E=30-300 eV; measured transmission neutron spectra; deduced off-resonance parity violating asymmetry.
doi: 10.1103/PhysRevC.61.045503
2000SH02 Phys.Rev. C61, 025501 (2000) E.I.Sharapov, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, M.Iinuma, J.N.Knudson, L.Y.Lowie, J.E.Lynch, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, S.L.Stephenson, Y.-F.Yen, V.W.Yuan Parity Violation in 232Th Neutron Resonances Above 250 eV NUCLEAR REACTIONS 232Th(polarized n, n), E=40-2100 eV; measured transimission yields, asymmetry. 232Th deduced resonances, parity-nonconservation effects.
doi: 10.1103/PhysRevC.61.025501
2000ST08 Phys.Rev. C61, 045501 (2000) S.L.Stephenson, J.D.Bowman, F.Corvi, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, M.Iinuma, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Masuda, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, H.M.Shimizu, Y.-F.Yen, V.W.Yuan, L.Zanini Parity Violation in Neutron Resonances in 115In NUCLEAR REACTIONS In(polarized n, n), E=6-316 eV; measured transmission neutron spectra. 115In(n, γ), E=3-480 eV; measured Eγ, Iγ, σ(En). 115In deduced p-wave resonances J, π, asymmetries, parity violation, weak spreading width.
doi: 10.1103/PhysRevC.61.045501
1999CR03 Phys.Rev. C60, 055503 (1999) B.E.Crawford, J.D.Bowman, P.P.J.Delheij, T.Haseyama, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, V.W.Yuan Parity Nonconservation in 106Pd and 108Pd Neutron Resonances NUCLEAR REACTIONS 106,108Pd(polarized n, γ), E=20-2000 eV; measured capture σ vs helicity; deduced weak spreading widths, possible parity nonconservation effects.
doi: 10.1103/PhysRevC.60.055503
1999LO01 Phys.Rev. C59, 1119 (1999) L.Y.Lowie, J.D.Bowman, F.Corvi, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, M.Iinuma, J.N.Knudson, A.Masaike, Y.Masuda, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, H.M.Shimizu, S.L.Stephenson, Y.-F.Yen, V.W.Yuan, L.Zanini Parity Violation in Neutron Resonances in 107, 109Ag NUCLEAR REACTIONS Ag(polarized n, X), E=32-422 eV; measured total σ helicity dependence, longitudinal asymmetries; deduced parity nonconservation features. 107,109Ag(n, γ), E=10-800 eV; measured Eγ, Iγ, tof spectra. 107,109Ag deduced resonances E, Γ, J.
doi: 10.1103/PhysRevC.59.1119
1999SH11 Phys.Rev. C59, 1131 (1999) E.I.Sharapov, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, K.Fukuda, M.Iinuma, J.N.Knudson, S.J.Lokitz, L.Y.Lowie, A.Masaike, Y.Masuda, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, H.M.Shimizu, S.L.Stephenson, Y.-F.Yen, V.W.Yuan Search for Parity Violation in 93Nb Neutron Resonances NUCLEAR REACTIONS 93Nb(polarized n, n), E=32-1000 eV; measured total σ, longitudinal asymmetries. 93Nb deduced resonances E, Γ, upper limit for weak spreading width.
doi: 10.1103/PhysRevC.59.1131
1999SH17 Phys.Rev. C59, 1772 (1999) E.I.Sharapov, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, T.Haseyama, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Masuda, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, S.L.Stephenson, Y.-F.Yen, V.W.Yuan Parity Nonconservation in Neutron Resonances in 133Cs NUCLEAR REACTIONS 133Cs(polarized n, γ), E=5-400 eV; measured transmission spectra, σ(E) asymmetry. 133Cs deduced resonances E, Γ, parity non-conserving matrix element, weak spreading width.
doi: 10.1103/PhysRevC.59.1772
1999SM03 Phys.Rev. C59, 2836 (1999) D.A.Smith, J.D.Bowman, B.E.Crawford, C.A.Grossmann, T.Haseyama, M.B.Johnson, A.Masaike, Y.Matsuda, G.E.Mitchell, V.A.Nazarenko, S.I.Penttila, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, L.M.Smotritsky, S.L.Stephenson, V.Yuan Neutron Resonance Spectroscopy of 117Sn from 1 eV to 1.5 keV NUCLEAR REACTIONS 117Sn(n, γ), E=1-1500 eV; measured σ(E). 117Sn deduced neutron resonance parameters.
doi: 10.1103/PhysRevC.59.2836
1999SM15 Phys.Rev. C60, 045502 (1999) D.A.Smith, J.D.Bowman, B.E.Crawford, C.A.Grossmann, T.Haseyama, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, V.Yuan Neutron Resonance Spectroscopy of 103Rh from 30 eV to 2 keV NUCLEAR REACTIONS 103Rh(n, γ), E=30-2000 eV; measured σ(En); deduced resonance parameters. Tof technique.
doi: 10.1103/PhysRevC.60.045502
1999SM16 Phys.Rev. C60, 045503 (1999) D.A.Smith, J.D.Bowman, B.E.Crawford, C.A.Grossmann, T.Haseyama, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, V.Yuan Parity Violation in Neutron Resonances of 103Rh NUCLEAR REACTIONS 103Rh(n, γ), E=30-490 eV; analyzed data; deduced resonance parameters, parity nonconservation.
doi: 10.1103/PhysRevC.60.045503
1998CR04 Phys.Rev. C58, 729 (1998) B.E.Crawford, J.D.Bowman, P.P.J.Delheij, T.Haseyama, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, V.W.Yuan Neutron Resonance Spectroscopy of 106Pd and 108Pd from 20 to 2000 eV NUCLEAR REACTIONS 106,108Pd(n, γ), (n, n'γ), E=20-2000 eV; measured transmission, capture Eγ, Iγ. 106,108Pd deduced resonances E, Γ, J, π. Multilevel, multichannel analysis.
doi: 10.1103/PhysRevC.58.729
1998CR05 Phys.Rev. C58, 1225 (1998) B.E.Crawford, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, M.Iinuma, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, Y.-F.Yen, V.W.Yuan, and the TRIPLE Collaboration Parity Nonconservation in Neutron Resonances in 238U NUCLEAR REACTIONS 238U(polarized n, n), E=10-300 eV; measured total σ, longitudinal asymmetries. 238U deduced resonance parameters, parity violating matrix element.
doi: 10.1103/PhysRevC.58.1225
1998MO09 Phys.Lett. 419B, 25 (1998) C.L.Morris, J.D.Zumbro, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Reidel, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, J.Ouyang, R.J.Peterson, J.E.Wise Evidence for Δ+ Components in Nuclei NUCLEAR REACTIONS 12,13C, 90Zr, 208Pb(π+, π+p), (π+, π-p), E=500 MeV; measured σ(DCX)/σ(NCX); deduced nuclear wave function Δ+ components.
doi: 10.1016/S0370-2693(97)01453-6
1998SE21 Phys.Rev. C58, 2977 (1998) S.J.Seestrom, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, M.Iinuma, J.N.Knudson, P.E.Koehler, L.Y.Lowie, A.Masaike, Y.Masuda, Y.Matsuda, G.E.Mitchell, S.I.Penttila, Yu.P.Popov, H.Postma, N.R.Roberson, E.I.Sharapov, H.M.Shimizu, D.A.Smith, S.L.Stephenson, Y.F.Yen, V.W.Yuan Parity Nonconservation in Neutron Capture on 113Cd NUCLEAR REACTIONS Cd, 113Cd(polarized n, γ), E=7-520 eV; measured Eγ, Iγ, transmission spectra, total capture σ helicity dependence. 113Cd deduced resonances J, π, widths, parity-violating asymmetries.
doi: 10.1103/PhysRevC.58.2977
1998ST14 Phys.Rev. C58, 1236 (1998) S.L.Stephenson, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, M.Iinuma, J.N.Knudson, L.Y.Lowie, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, Y.-F.Yen, V.W.Yuan Parity Nonconservation in Neutron Resonances in 232Th NUCLEAR REACTIONS 232Th(polarized n, n), E=8-300 eV; measured total σ, longitudinal asymmetries. 232Th deduced resonance parameters, parity violating matrix element.
doi: 10.1103/PhysRevC.58.1236
1997LO04 Phys.Rev. C56, 90 (1997) L.Y.Lowie, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, T.Haseyama, J.N.Knudson, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, Y.-F.Yen, V.W.Yuan Neutron Resonance Spectroscopy of 107Ag and 109Ag NUCLEAR REACTIONS 107,109Ag(n, X), E=10-800 eV; measured neutron transmission spectra. 108,110Ag deduced resonances, gΓ(n), l, J. 107Ag(n, γ), E=10-800 eV; measured Eγ, Iγ. 108Ag deduced resonance isotopic assignments.
doi: 10.1103/PhysRevC.56.90
1996LA04 Phys.Rev. C53, 1167 (1996) C.M.Laymon, W.Amos, M.G.Burlein, H.T.Fortune, T.Ekenberg, A.Kotwal, J.M.O'Donnell, J.D.Silk, J.D.Zumbro, C.L.Morris, S.J.Seestrom, K.S.Dhuga, R.Garnett, M.W.Rawool-Sullivan, C.F.Moore, S.L.Morris, D.L.Watson Pion Elastic and Inelastic 2+1 Scattering on 58,60,62,64Ni at T(π) = 180 MeV NUCLEAR REACTIONS 58,60,62,64Ni(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ); deduced nucleon radii, deformation parameters. 58,60,62,64Ni levels deduced neutron, proton matrix elements.
doi: 10.1103/PhysRevC.53.1167
1996SZ02 Phys.Rev. C53, R2576 (1996) J.J.Szymanski, W.M.Snow, J.D.Bowman, B.Cain, B.E.Crawford, P.P.J.Delheij, R.D.Hartman, T.Haseyama, C.D.Keith, J.N.Knudson, A.Komives, M.Leuschner, L.Y.Lowie, A.Masaike, Y.Matsuda, G.E.Mitchell, S.I.Penttila, H.Postma, D.Rich, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, S.L.Stephenson, Y.F.Yen, V.W.Yuan Observation of a Large Parity Nonconserving Analyzing Power in Xe NUCLEAR REACTIONS Xe(polarized n, X), E ≈ resonance; measured large parity nonconserving analyzing power. Transmission through liquid Xe target, natural isotopic abundance.
doi: 10.1103/PhysRevC.53.R2576
1994CA50 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.40 (1994) A.D.Carlson, W.E.Parker, P.W.Lisowski, G.L.Morgan, S.J.Seestrom, N.W.Hill, K.Meggers Measurements of the fission cross section of 237Np NUCLEAR REACTIONS 237Np(n, f), E=5.171 eV-5.1 keV; measured product s; deduced σ, σ(E). Data were imported from EXFOR entry 14035. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14035. 1993BO25 Phys.Rev. C48, 1116 (1993) J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, J.J.Yeh, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Experimental Limit on Parity Violation in Nonresonant Neutron-Nucleus Scattering NUCLEAR REACTIONS 232Th(polarized n, X), E=6-86 eV; measured transmission spectra, parity nonconserving longitudinal asymmetry; deduced nonresonant scattering parity violation limit.
doi: 10.1103/PhysRevC.48.1116
1993FR13 Phys.Rev. C48, 1601 (1993) C.M.Frankle, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.S.Patterson, S.I.Penttila, Yu.P.Popov, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, Y.-F.Yen, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Neutron Resonance Spectroscopy of 113In and 115In NUCLEAR REACTIONS In(n, X), E=25-500 eV; measured transmission; deduced σ(E). 115In(n, γ), E=25-500 eV; measured capture Eγ, Iγ. 114,116In deduced resonances, parameters.
doi: 10.1103/PhysRevC.48.1601
1993FR19 Nucl.Instrum.Methods Phys.Res. B79, 306 (1993) C.M.Frankle, J.D.Bowman, J.N.Knudson, S.I.Penttila, S.J.Seestrom, S.H.Yoo, V.W.Yuan, C.R.Gould, D.G.Haase, G.E.Mitchell, N.R.Roberson, Yu.P.Popov, E.I.Sharapov, P.P.J.Delheij, H.Postma, and the TRIPLE Collaboration Measurement of Parity Violation in Compound Nuclear Resonances using Epithermal Polarized Neutrons NUCLEAR REACTIONS 81Br, 139La, 232Th, 238U(polarized n, X), E=epithermal; compiled, reviewed parity nonconserving analyzing power data.
doi: 10.1016/0168-583X(93)95351-5
1993HA39 Nucl.Instrum.Methods Phys.Res. B79, 300 (1993) D.G.Haase, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, J.N.Knudson, J.E.Koster, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, S.H.Yoo, V.W.Yuan Bulk Magnetic Structure Studies using Polarized Epithermal Neutrons NUCLEAR REACTIONS Ho(polarized n, n), E=epithermal; measured neutron depolarization. Thick single ferromagnetic holmium crystal.
doi: 10.1016/0168-583X(93)95349-A
1993RO25 Nucl.Instrum.Methods Phys.Res. A326, 549 (1993) N.R.Roberson, C.D.Bowman, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, R.N.Mortensen, S.I.Penttila, H.Postma, S.J.Seestrom, J.J.Szymanski, S.A.Wender, S.H.Yoo, V.W.Yuan, X.Zhu An Apparatus and Techniques of Tests for Fundamental Symmetries in Compound-Nucleus Scattering with Epithermal Polarized Neutron Beams NUCLEAR REACTIONS 238U(polarized n, X), E=5-300 eV; measured neutron transmission. 239U resonance deduced average parity violating asymmetry.
doi: 10.1016/0168-9002(93)90858-F
1993WI15 Phys.Rev. C48, 1840 (1993) J.E.Wise, M.R.Braunstein, S.Hoibraten, M.D.Kohler, B.J.Kriss, J.Ouyang, R.J.Peterson, J.A.McGill, C.L.Morris, S.J.Seestrom, R.M.Whitton, J.D.Zumbro, C.M.Edwards, A.L.Williams Quasifree Pion Scattering at 500 MeV NUCLEAR REACTIONS C(π+, π+), (π-, π-), E=500 MeV; measured σ(θ) vs energy loss, σ(θ). Ca, Zr, Pb(π+, π+), (π-, π-), E=500 MeV; measured σ(θ); deduced surface single nucleon knockout evidence.
doi: 10.1103/PhysRevC.48.1840
1993ZU01 Phys.Rev.Lett. 71, 1796 (1993) J.D.Zumbro, C.L.Morris, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Edwards, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, R.J.Peterson, J.Ouyang, J.E.Wise, W.R.Gibbs Inclusive Scattering of 500-MeV Pions from Carbon NUCLEAR REACTIONS C(π+, π+X), (π-, π-X), E=500 MeV; measured inclusive σ(θ, E(π)); deduced comparison with (e, e'X).
doi: 10.1103/PhysRevLett.71.1796
1992FR07 Phys.Rev. C45, 2143 (1992) C.M.Frankle, C.D.Bowman, J.D.Bowman, S.J.Seestrom, E.I.Sharapov, Yu.P.Popov, N.R.Roberson Neutron Resonance Spectroscopy on 113Cd: The p-wave levels NUCLEAR REACTIONS 113Cd(n, n), 113Cd, Cd(n, γ), E=0-500 eV; measured En, capture γ yield, σ(E). 114Cd deduced levels, resonance parameters, p-wave strength function, level density. Enriched target.
doi: 10.1103/PhysRevC.45.2143
1992FR14 Phys.Rev. C46, 778 (1992) C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Nonconservation for Neutron Resonances in 232Th NUCLEAR REACTIONS 232Th(polarized n, X), E=6-400 eV; measured total σ, parity violating asymmetries. 233Th deduced resonances, p-wave parity nonconserving matrix element rms values, spreading width.
doi: 10.1103/PhysRevC.46.778
1992FR15 Phys.Rev. C46, 1542 (1992) C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Nonconservation for the 0.88-eV Neutron Resonance in 81Br NUCLEAR REACTIONS 81Br(polarized n, n), E=0.88 eV; measured parity nonconserving longitudinal analyzing power, σ for p-wave resonances.
doi: 10.1103/PhysRevC.46.1542
1992HI01 Phys.Rev. C45, 601 (1992) N.M.Hintz, X.H.Yang, M.Gazzaly, S.J.Seestrom-Morris, C.L.Morris, D.C.Cook, A.M.Mack, J.W.McDonald, S.Mordechai, D.S.Oakley, C.F.Moore, M.Lynker, J.D.Zumbro Determination of Neutron and Proton Multipole Matrix Elements in 208Pb from π- and π+ Scattering at 180 MeV NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-'), (π-, π-), E=180 MeV; measured σ(θ). 208Pb levels deduced neutron, proton multipole matrix elements.
doi: 10.1103/PhysRevC.45.601
1992HO08 Phys.Rev. C46, 499 (1992) D.J.Horen, C.L.Morris, S.J.Seestrom, F.W.Hersman, J.R.Calarco, M.Holtrop, M.Leuschner, M.Rawool-Sullivan, R.W.Garnett, S.J.Greene, M.A.Plum, J.D.Zumbro Isospin Character of the Transition to the 0.803-MeV State in 206Pb from π± Scattering at 180 MeV NUCLEAR REACTIONS 206Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ). 206Pb deduced neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.
doi: 10.1103/PhysRevC.46.499
1992PO13 Hyperfine Interactions 75, 153 (1992) H.Postma, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Violation at Neutron p-Wave Resonances of 238U and 232Th and Related Questions NUCLEAR REACTIONS 238U, 232Th(n, X), E ≈ epithermal; measured transmission. 239U, 233Th deduced p-wave resonances, parity violation matrix element rms value.
doi: 10.1007/BF02398972
1992ZH12 Phys.Rev. C46, 768 (1992) X.Zhu, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, and the TRIPLE Collaboration Parity Nonconservation for Neutron Resonances in 238U NUCLEAR REACTIONS 238U(polarized n, X), E=6-300 eV; measured total σ; deduced P-odd, P-even effective nucleon-nucleon interaction. 239U deduced resonances, l, gΓn, p-wave parity nonconserving matrix element rms value, spreading width.
doi: 10.1103/PhysRevC.46.768
1991BR21 Phys.Rev. C44, 2031 (1991) B.Brinkmoller, C.L.Blilie, D.Dehnhard, M.K.Jones, G.M.Martinez, S.K.Nanda, S.M.Sterbenz, Y.-F.Yen, L.G.Atencio, S.J.Greene, C.L.Morris, S.J.Seestrom, G.R.Burleson, K.S.Dhuga, J.A.Faucett, R.W.Garnett, K.Maeda, C.F.Moore, S.Mordechai, A.Williams, S.H.Yoo, L.C.Bland Elastic Scattering of π+ and π- from 4He between 90 and 240 MeV NUCLEAR REACTIONS 4He(π+, π+), (π-, π-), E=90-240 MeV; measured σ(θ); deduced phase shifts. Optical model analysis.
doi: 10.1103/PhysRevC.44.2031
1991FR08 Phys.Rev.Lett. 67, 564 (1991) C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Sign Correlations and Parity Nonconservation for Neutron Resonances in 232Th NUCLEAR REACTIONS 232Th(polarized n, n), E ≈ 8.3-392 eV; measured longitudinal analyzing power vs E, transmission yield. 232Th resonances deduced parity violation evidence statistical significance. High confidence limit measurement.
doi: 10.1103/PhysRevLett.67.564
1991KN05 Phys.Rev. C44, 2869 (1991) J.N.Knudson, C.L.Morris, J.D.Bowman, W.C.Sailor, S.J.Seestrom, I.Supek, M.E.Sadler, L.D.Isenhower Search for Neutral Pions from the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured π0 spectra following SF-decay; deduced π0 branching ratio upper limit.
doi: 10.1103/PhysRevC.44.2869
1991LI35 Phys.Rev. C44, 2413 (1991) R.A.Lindgren, B.L.Clausen, G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, B.H.Wildenthal, R.Gilman, J.A.Carr Pion Scattering to 6- Stretched States in 24Mg and 26Mg NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=116-180 MeV; measured pion spectra, σ(θ). 26,24Mg levels deduced stretched configuration isoscalar, isovector strength.
doi: 10.1103/PhysRevC.44.2413
1991OA01 Phys.Rev. C44, 2058 (1991) D.S.Oakley, R.J.Peterson, S.J.Seestrom, C.L.Morris, M.A.Plum, J.D.Zumbro, A.L.Williams, M.A.Bryan, J.W.McDonald, C.F.Moore Energy Dependence of Pion Inelastic Scattering from 208Pb NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=120, 250 MeV; calculated σ(θ). 208Pb levels deduced proton, neutron matrix elements ratio. Different structure models.
doi: 10.1103/PhysRevC.44.2058
1991SZ05 Nucl.Phys. A527, 701c (1991) J.J.Szymanski, C.D.Bowman, J.D.Bowman, J.Knudson, S.Penttila, S.J.Seestrom, V.W.Yuan, J.E.Bush, C.M.Frankle, C.R.Gould, D.G.Haase, G.E.Mitchell, P.P.J.Delheij, H.Postma, N.R.Roberson, X.Zhu Parity and Time Reversal Symmetry Nonconservation in Neutron-Nucleus Interactions NUCLEAR REACTIONS 238U(polarized n, X), E=60-72 eV; measured transmission, resonance σ helicity dependence. 239U deduced p-, s-wave states mixing parity-violating rms matrix element, parity violating spreading width.
doi: 10.1016/0375-9474(91)90217-T
1991YU02 Phys.Rev. C44, 2187 (1991) V.W.Yuan, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, X.Zhu Parity Nonconservation in Polarized-Neutron Transmission Through 139La NUCLEAR REACTIONS 139La(polarized n, X), E=0.5-1 eV; measured transmission. 140La resonance deduced asymmetry. Parity nonconservation, longitudinal beam polarization.
doi: 10.1103/PhysRevC.44.2187
1990BL04 Phys.Rev. C41, 1625 (1990) G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, R.A.Lindgren, B.H.Wildenthal, R.Gilman Pion Elastic and Inelastic Scattering from 24Mg and 26Mg NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=150, 180 MeV; measured σ(θ), σ(E(π)). 26,24Mg levels deduced deformation parameters, neutron, proton matrix elements.
doi: 10.1103/PhysRevC.41.1625
1990BO26 Phys.Rev.Lett. 65, 1192 (1990) J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu Parity Nonconservation for Neutron Resonances in 238U NUCLEAR REACTIONS 238U(n, X), E=epithermal; measured transmission, σ(E) vs helicity. 239U levels deduced parity nonconservation.
doi: 10.1103/PhysRevLett.65.1192
1990PE19 J.Phys.(Paris), Colloq.C-6, 523 (1990) S.Penttila, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.M.Yuan, X.Zhu Parity Violation in 239U Neutron Resonances NUCLEAR REACTIONS 238U(polarized n, X), E ≤ 250 eV; measured asymmetry in transmission; deduced parity violating matrix element rms value, effective NN-interaction parameter. 239U resonances deduced parity-violating spreading width.
1990YO02 J.Phys.(London) G16, L89 (1990) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom, M.Jones, S.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 208Pb(π±, π±'n) Reaction in the Giant-Resonance Region NUCLEAR REACTIONS 208Pb(π+, π+'n), (π-, π-'n), E=180 MeV; measured σ(θn, θπ), missing mass spectra. 208Pb deduced giant resonance neutron decay features.
doi: 10.1088/0954-3899/16/5/002
1989HO11 Z.Phys. A333, 39 (1989) D.J.Horen, J.Lisantti, R.L.Auble, F.E.Bertrand, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson T = 1, Spin-Dipole Strength in 40Ca NUCLEAR REACTIONS 40Ca(p, p'), E=500 MeV; measured σ(θ), σ(Ep). 40Ca deduced T=1 spin-dipole transition strength distribution.
1989LI03 Phys.Rev. C39, 568 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Collective Model Distored-Wave Born Approximation Analysis of 500-MeV Proton Scattering form 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; analyzed σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca levels deduced deformation lengths, multipole matrix elements. Relativistic, non-relativistic DWBA analysis.
doi: 10.1103/PhysRevC.39.568
1989LI15 Phys.Rev. C40, 211 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Giant Resonance Strength Distribution in 40Ca from Inelastic Scattering of 500 MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; measured σ(θp, Ep), σ(θ). 40Ca deduced giant resonance strength distribution.
doi: 10.1103/PhysRevC.40.211
1989YO06 Phys.Rev.Lett. 63, 738 (1989) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom-Morris, M.K.Jones, S.M.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 12C(π±, π±'p)11B Reaction Near the Giant Dipole Region NUCLEAR REACTIONS 12C(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θ(p), E(π)); deduced σ(π+, π+p)/σ(π-, π-p) near GDR. DWIA analysis.
doi: 10.1103/PhysRevLett.63.738
1988HA14 Phys.Rev. C37, 1554 (1988) A.C.Hayes, S.Chakravarti, D.Dehnhard, P.J.Ellis, D.B.Holtkamp, L.-P.Lung, S.J.Seestrom-Morris, H.Baer, C.L.Morris, S.J.Greene, C.J.Harvey Structure of the Low-Lying 2+ States in 14C from Inelastic Pion Scattering NUCLEAR STRUCTURE 14C, 14N, 14O; calculated levels, B(λ). Shell model. NUCLEAR REACTIONS 14C(π, π'), E=164 MeV; analyzed σ(θ). 14C level deduced isovector component quenching.
doi: 10.1103/PhysRevC.37.1554
1988MO01 Phys.Rev.Lett. 60, 408 (1988) S.Mordechai, N.Auerbach, G.R.Burleson, K.S.Dhuga, M.Dwyer, J.A.Faucett, H.T.Fortune, R.Gilman, S.J.Greene, C.Laymon, C.F.Moore, C.L.Morris, D.S.Oakley, M.A.Plum, S.J.Seestrom-Morris, P.A.Seidl, M.J.Smithson, Z.F.Wang, J.D.Zumbro Giant Dipole Resonances Built on Isobaric Analog States in Pion Double Charge Exchange NUCLEAR REACTIONS 56Fe, 80Se, 208Pb(π+, π-), E at 292 MeV/c; measured σ(E(π-), θ(π-)), σ(θ(π-)). 56Ni, 80Kr, 208Po deduced giant dipole resonance parameters. Coupled-channel impulse approximation calculations.
doi: 10.1103/PhysRevLett.60.408
1988OA01 Phys.Rev. C37, 866 (1988) D.S.Oakley, M.J.Smithson, S.Mordechai, C.F.Moore, P.A.Seidl, C.L.Morris, S.J.Seestrom-Morris, R.Gilman, J.D.Zumbro, H.T.Fortune, K.S.Dhuga Pion Inelastic Scattering from 48,50Ti, 52Cr, and 54,56Fe: Higher-lying states NUCLEAR REACTIONS 48,50Ti, 52Cr, 54,56Fe(π+, π+), (π+, π+'), E=180 MeV; measured σ(θ). 48,50Ti, 52Cr, 54,56Fe levels deduced neutron, proton matrix elements.
doi: 10.1103/PhysRevC.37.866
1988SE04 Phys.Rev. C37, 2057 (1988) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, D.B.Holtkamp, C.L.Blilie, C.L.Morris, J.D.Zumbro, H.T.Fortune Pion Inelastic Scattering to the Three Lowest 2+ States of 18O NUCLEAR REACTIONS 18O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ). 18O levels deduced matrix elements, transition densities. Gas Target. DWIA analysis.
doi: 10.1103/PhysRevC.37.2057
1988WE06 J.Phys.(London) G14, Supplement S417 (1988) S.A.Wender, S.J.Seestrom-Morris, R.O.Nelson A White Neutron Source from 1 to 400 MeV NUCLEAR REACTIONS 12C(n, n'γ), E=5-25 meV; measured σ(E).
doi: 10.1088/0305-4616/14/S/041
1987CH14 Phys.Rev. C35, 2197 (1987) S.Chakravarti, D.Dehnhard, M.A.Franey, S.J.Seestrom-Morris, D.B.Holtkamp, C.L.Blilie, A.C.Hayes, C.L.Morris, D.J.Millener Distorted-Wave Impulse Approximation and Coupled-Channels Analysis of Inelastic Pion Scattering from 18O NUCLEAR REACTIONS 18O(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; calculated σ(θ). 18O levels deduced transition densities. DWIA, coupled-channels calculations.
doi: 10.1103/PhysRevC.35.2197
1987DH01 Phys.Rev. C35, 1148 (1987) K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, Z.F.Wang, J.W.McDonald, C.F.Moore, S.Mordechai, A.L.Williams, P.A.Seidl, M.A.Bryan, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro Sensitivity of Large-Angle Pion Elastic Scattering to Medium Modifications NUCLEAR REACTIONS 12C, 16O(π+, π+), E=100-240 MeV; measured σ(θ); deduced model parameter modifications. Optical model.
doi: 10.1103/PhysRevC.35.1148
1987MO07 Phys.Rev. C35, 1388 (1987) C.L.Morris, S.J.Seestrom-Morris, D.Dehnhard, C.L.Blilie, R.Gilman, G.P.Gilfoyle, J.D.Zumbro, M.G.Burlein, S.Mordechai, H.T.Fortune, L.C.Bland, M.Brown, D.P.Saunders, P.A.Seidl, C.F.Moore, K.Maeda, G.S.Blanpied, B.A.Brown Neutron and Proton Matrix Elements for 2+1 Transitions in T = 1 Nuclei from Pion Inelastic Scattering NUCLEAR REACTIONS 18O, 22Ne, 26Mg, 30Si, 34S(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ). 18O, 22Ne, 26Mg, 30Si, 34S transitions deduced neutron, proton quadrupole matrix elements. DWIA analysis.
doi: 10.1103/PhysRevC.35.1388
1987MO25 Phys.Rev. C36, 1950 (1987) S.Mordechai, C.Harvey, W.B.Cottingame, P.A.Seidl, C.F.Moore, L.C.Bland, M.Carchidi, H.T.Fortune, S.J.Seestrom-Morris, C.L.Morris Inelastic Pion Scattering to Low-Lying Excited States of 44Ca NUCLEAR REACTIONS 44Ca(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ), missing mass spectrum. 44Ca levels deduced neutron, proton matrix elements. DWIA analysis.
doi: 10.1103/PhysRevC.36.1950
1987OA01 Phys.Rev. C35, 1392 (1987) D.S.Oakley, M.J.Smithson, S.Mordechai, C.F.Moore, C.L.Morris, G.C.Idzorek, Z.F.Wang, R.Gilman, J.D.Zumbro, H.T.Fortune, S.J.Seestrom-Morris, K.S.Dhuga, D.L.Watson Pion Elastic and Inelastic Scattering from 48,50Ti, 52Cr, and 54,56Fe at 180 MeV: Determination of neutron and proton multipole matrix elements NUCLEAR REACTIONS 48,50Ti, 52Cr, 54,56Fe(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(E(π)), σ(θ). 48,50Ti, 52Cr, 54,56Fe deduced levels, neutron, proton multipole matrix elements, ground state density distribution parameters.
doi: 10.1103/PhysRevC.35.1392
1987OA02 Phys.Rev. C36, 1074 (1987) D.S.Oakley, M.A.Machuca, M.J.Smithson, S.Mordechai, C.F.Moore, P.A.Seidl, C.L.Morris, Z.F.Wang, R.Gilman, J.D.Zumbro, H.T.Fortune, S.J.Seestrom-Morris, K.S.Dhuga, D.L.Watson Pion Elastic and Inelastic Scattering from 51V at 180 MeV NUCLEAR REACTIONS 51V(π+, π+), (π+, π+'), E=180 MeV; measured σ(θ). 51V deduced levels, J, π, B(λ), proton, neutron matrix elements.
doi: 10.1103/PhysRevC.36.1074
1986AD02 Phys.Rev. C33, 2054 (1986) G.S.Adams, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, D.Cook Inelastic Proton Excitation of High-Lying Giant Resonances NUCLEAR REACTIONS 208Pb, 144Sm, 116Sn(p, p'), E=800 MeV; measured σ(Ep'), σ(θ). 208Pb, 144Sm, 116Sn deduced giant resonances, parameters, J, π, EWSR. DWBA analysis.
doi: 10.1103/PhysRevC.33.2054
1986BE14 Phys.Rev. C34, 45 (1986) F.E.Bertrand, E.E.Gross, D.J.Horen, R.O.Sayer, T.P.Sjoreen, D.K.McDaniels, J.Lisantti, J.R.Tinsley, L.W.Swenson, J.B.McClelland, T.A.Carey, K.Jones, S.J.Seestrom-Morris Giant Resonance Structure in 208Pb Measured using the (p, p') Reaction at 334 MeV NUCLEAR REACTIONS 208Pb(polarized p, p'), E=334 MeV; measured σ(Ep), σ(θ); deduced model parameters. 208Pb deduced giant resonances, Γ, L, EWSR, B(λ). DWBA analysis.
doi: 10.1103/PhysRevC.34.45
1986BL07 Phys.Rev.Lett. 57, 543 (1986) C.L.Blilie, D.Dehnhard, D.B.Holtkamp, S.J.Seestrom-Morris, S.K.Nanda, W.B.Cottingame, D.Halderson, C.L.Morris, C.F.Moore, P.A.Seidl, H.Ohnuma, K.Maeda Measurement of Isospin Mixing in 4He and Its Implications for Charge-Symmetry Breaking NUCLEAR REACTIONS 4He(π+, π+'), (π-, π-'), E=180 MeV; measured σ(E(π), θ(π)); deduced σ(π+)/σ(π-). 4He deduced very weak 1- state isospin mixing. DWIA analysis.
doi: 10.1103/PhysRevLett.57.543
1986BU13 Nucl.Instrum.Methods Phys.Res. A247, 327 (1986) G.R.Burleson, W.B.Cottingame, K.S.Dhuga, J.A.Faucett, C.P.Fontenla, J.F.Amann, R.L.Boudrie, S.J.Greene, C.L.Morris, N.Tanaka, Z.F.Wang, D.Yusnukis, M.Brown, R.R.Kiziah, E.C.Milner, C.F.Moore, S.Mordechai, D.Oakley, P.A.Seidl, C.L.Blilie, D.Dehnhard, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro, K.Maeda A Large-Angle Pion-Nucleus Scattering Facility for EPICS at LAMPF NUCLEAR REACTIONS 12C(π+, π+), E=162 MeV; 16O(π-, π-), E=114 MeV; measured σ(θ), θ=115°-180°. Energetic pion channel, spectrometer.
doi: 10.1016/0168-9002(86)91314-8
1986MO26 Phys.Lett. 182B, 151 (1986) C.L.Morris, K.W.Jones, J.A.McGill, M.A.Bryan, C.F.Moore, R.Gilman, C.Glashausser, S.J.Seestrom-Morris The Observation of Energetic Protons in Coincidence with Pion-Induced Double Charge Exchange on 12C and 48Ca NUCLEAR REACTIONS 12C, 48Ca(π+, π-p), (π+, π+p), (π-, π-p), E=250 MeV; measured σ(θ(π), θp) vs pion momentum. Enriched Ca target, energetic pion spectrometer.
doi: 10.1016/0370-2693(86)91567-4
1986SE01 Phys.Rev. C33, 1847 (1986) S.J.Seestrom-Morris, C.L.Morris, J.M.Moss, T.A.Carey, D.Drake, J.-C.Dousse, L.C.Bland, G.S.Adams Measurement of π+/π- Cross Section Ratio for the Giant Quadrupole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(π+, π+'), (π-, π-'), E=162 MeV; measured σ(E, θ), σ(θ). 208Pb deduced GQR σ(π-)/σ(π+), neutron, proton matrix element ratio.
doi: 10.1103/PhysRevC.33.1847
1985HO07 Phys.Rev. C31, 957 (1985); Erratum Phys.Rev. C41, 1319 (1990) D.B.Holtkamp, S.J.Seestrom-Morris, D.Dehnhard, H.W.Baer, C.L.Morris, S.J.Greene, C.J.Harvey, D.Kurath, J.A.Carr Pion Scattering to 4- States in 14C NUCLEAR REACTIONS 14C(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 14C deduced levels, J, π, neutron, proton amplitudes, ratios. DWIA, shell model wave functions.
doi: 10.1103/PhysRevC.31.957
1985HO14 Phys.Rev. C31, 2049 (1985) D.J.Horen, F.E.Bertrand, E.E.Gross, T.P.Sjoreen, D.K.McDaniels, J.R.Tinsley, J.Lisantti, L.W.Swenson, J.B.McClelland, T.A.Carey, S.J.Seestrom-Morris, K.Jones Cross Sections and Analyzing Powers for Quenched Spin Excitations in 40,48Ca at E(p) = 334 MeV NUCLEAR REACTIONS 40,48Ca(polarized p, p'), E=334 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. 40Ca level deduced B(M2). Microscopic DWIA.
doi: 10.1103/PhysRevC.31.2049
1985SE06 Phys.Rev. C31, 923 (1985) S.J.Seestrom-Morris, D.Dehnhard, C.L.Morris, L.C.Bland, R.Gilman, H.T.Fortune, D.J.Millener, D.P.Saunders, P.A.Seidl, R.R.Kiziah, C.F.Moore M4 Transitions Observed in Pion Inelastic Scattering on 15N NUCLEAR REACTIONS 15N(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; measured σ(θ(π), E(π)), σ(θ). 15N levels deduced M4 transition strength, form factors.
doi: 10.1103/PhysRevC.31.923
1984BL12 Phys.Lett. 144B, 328 (1984) L.C.Bland, R.Gilman, G.S.Stephans, G.P.Gilfoyle, H.T.Fortune, C.L.Morris, S.J.Seestrom-Morris, S.J.Greene, P.A.Seidl, R.R.Kiziah, C.F.Moore Forward-Peaked Angular Distributions Observed in (π, π') on Light Nuclei NUCLEAR REACTIONS 12C(π+, π+'), E=170 MeV; 28Si(π+, π+'), E=162 MeV; calculated σ(θ, E(π)). 12C, 28Si deduced resonances, Γ, possible multipole character.
doi: 10.1016/0370-2693(84)91271-1
1984BL17 Phys.Rev. C30, 1989 (1984) C.L.Blilie, D.Dehnhard, M.A.Franey, D.H.Gay, D.B.Holtkamp, S.J.Seestrom-Morris, P.J.Ellis, C.L.Morris, D.J.Millener Isospin Structure of Transitions in 17O from Inelastic Pion Scattering at 164 MeV NUCLEAR REACTIONS 16,17O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 17O deduced M4, E2 transition strength distribution. Microscopic DWIA calculations.
doi: 10.1103/PhysRevC.30.1989
1984DE19 Phys.Rev. C30, 242 (1984) D.Dehnhard, D.H.Gay, C.L.Blilie, S.J.Seestrom-Morris, M.A.Franey, C.L.Morris, R.L.Boudrie, T.S.Bhatia, C.F.Moore, L.C.Bland, H.Ohnuma Excitation of the 1+ State in 48Ca(10.2 MeV) by Inelastic Scattering of π- and π+ NUCLEAR REACTIONS 48Ca(π+, π+'), (π-, π-'), E=116-180 MeV; measured σ(E(π)), σ(θ). 48Ca level deduced σ(π-)/σ(π+), isoscalar, isovector rescaling factor dependence. DWIA analysis.
doi: 10.1103/PhysRevC.30.242
1984HI10 Phys.Rev. C30, 1976 (1984) N.M.Hintz, M.A.Franey, M.M.Gazzaly, D.Cook, G.S.Kyle, D.Dehnhard, S.J.Seestrom-Morris, G.W.Hoffmann, M.Barlett, G.S.Blanpied, J.A.McGill, J.B.McClelland, R.L.Boudrie, F.Irom, G.Pauletta High Spin States in 28Si and 58Ni NUCLEAR REACTIONS 28Si, 58Ni(p, p'), E=333, 498, 800 MeV; measured σ(θ), σ(Ep). 28Si, 58Ni levels deduced transition densities. DWIA, other (p, p'), (e, e') data analysis.
doi: 10.1103/PhysRevC.30.1976
1984HO16 Phys.Rev. C30, 709 (1984) D.J.Horen, F.E.Bertrand, E.E.Gross, T.P.Sjoreen, D.K.McDaniels, J.R.Tinsley, J.Lisantti, L.W.Swenson, J.B.McClelland, T.A.Carey, S.J.Seestrom-Morris, K.Jones Excitation of E2 Transitions in 40Ca by 334-MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=334 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca deduced levels, J, π, L admixture, deformation lengths, B(E2). Macroscopic DWBA analysis.
doi: 10.1103/PhysRevC.30.709
1984MO14 J.Phys.(Paris), Colloq.C4, 327 (1984); See 1984Mo33 C.L.Morris, S.J.Seestrom-Morris, L.C.Bland Excitation of Giant Resonances in Pion Inelastic Scattering
1984MO18 Phys.Rev. C30, 662 (1984) C.L.Morris, N.Tanaka, R.L.Boudrie, L.C.Bland, H.T.Fortune, R.Gilman, S.J.Seestrom-Morris, C.F.Moore, D.Dehnhard Small Angle Pion Inelastic Scattering from 12C at 162 MeV NUCLEAR REACTIONS 12C(π+, π+), (π+, π+'), E=162 MeV; measured σ(θ), missing mass spectra. DWIA analysis.
doi: 10.1103/PhysRevC.30.662
1984MO33 J.Phys.(Paris), Colloq.C-4, 327 (1984) C.L.Morris, S.J.Seestrom-Morris, L.C.Bland Excitation of Giant Resonances in Pion Inelastic Scattering NUCLEAR REACTIONS 12C, 28Si, 208Pb(π+, π+'), E=162, 164 MeV; 152Sm(π+, π+), (π+, π+'), E=180 MeV; measured σ(E(π+), θ(π+)), σ(θ(π+)). 12C, 28Si deduced spin dipole resonances. 208Pb deduced σ(π+), σ(π-) asymmetries in continuum.
1984NA02 Phys.Rev. C29, 660 (1984) S.K.Nanda, C.Glashausser, K.W.Jones, J.A.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, J.R.Comfort, S.Levenson, R.Segel, H.Ohnuma 10.23 MeV M1 Transition in the 48Ca(p(pol), p'(pol))48Ca Reaction at 319 MeV NUCLEAR REACTIONS 48Ca(polarized p, p'), E=319 MeV; measured σ(θ), analyzing power, spin-flip probability vs θ. 48Ca deduced M1 transition strength, energy. DWIA analysis.
doi: 10.1103/PhysRevC.29.660
1984NA14 J.Phys.(Paris), Colloq.C4, 459 (1984); See 1984Na29 S.K.Nanda, C.Glashausser, K.W.Jones, J.S.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, J.R.Comfort, S.Levenson, R.Segel, H.Ohnuma Spin Flip Strength at High Excitation Energy in the 90Zr(p(pol), p(pol)')90Zr Reaction
1984NA29 J.Phys.(Paris), Colloq.C-4, 459 (1984) S.K.Nanda, C.Glashausser, K.W.Jones, J.S.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, J.R.Comfort, S.Levenson, R.Segel, H.Ohnuma Spin Flip Strength at High Excitation Energy in the 90Zr(p(pol), p(pol)')90Zr Reaction NUCLEAR REACTIONS 90Zr(polarized p, p'), E=319 MeV; measured σ(Ep', θp'), σ(θ), analyzing power, spin-flip σ, probability. 90Zr deduced possible M1 transitions. DWIA calculations.
1984SE12 Phys.Rev. C30, 270 (1984) S.J.Seestrom-Morris, M.A.Franey, D.Dehnhard, D.B.Holtkamp, R.L.Boudrie, J.F.Amann, G.C.Idzorek, C.A.Goulding 13C(p(pol), p')13C Reaction at T(p) = 547 MeV NUCLEAR REACTIONS 13C(polarized p, p'), E=547 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. DWIA analysis, shell model transition densities.
doi: 10.1103/PhysRevC.30.270
1983JO08 Phys.Lett. 128B, 281 (1983) K.W.Jones, C.Glashausser, S.Nanda, R.de Swiniarski, T.A.Carey, W.Cornelius, J.M.Moss, J.B.McClelland, S.J.Seestrom-Morris, J.R.Comfort, J.-L.Escudie, M.Gazzaly, N.Hintz, G.Igo, M.Haji-Saeid, C.A.Whitten Study of the 18.30 and 19.40 MeV States in 12C in Intermediate Energy Proton Scattering NUCLEAR REACTIONS 12C(p, p'), (polarized p, p'), E=398, 597, 698 MeV; measured σ(θ), analyzing power, spin-flip probabilities vs momentum transfer. 12C levels deduced J, π, T. DWIA analysis, shell model wave functions.
doi: 10.1016/0370-2693(83)90260-5
1983MO04 Phys.Lett. 123B, 37 (1983) C.L.Morris, J.F.Amann, S.J.Seestrom-Morris, J.A.McGill, C.Glashausser, K.Jones, S.Nanda, M.Barlett, G.W.Hoffmann, C.Milner, C.F.Moore, J.R.Comfort, L.C.Bland, R.Gilman Low-Momentum Delta Production in the 13C(p, d)12C Reaction NUCLEAR REACTIONS 13C(p, d), E=800 MeV; measured inclusive deuteron production σ, dp-, dπ-, dpp-coin; deduced isobar-hole admixtures in 12C.
doi: 10.1016/0370-2693(83)90953-X
1983MO18 Phys.Rev. C28, 2165 (1983) C.L.Morris, S.J.Seestrom-Morris, P.A.Seidl, R.R.Kiziah, S.J.Greene Pion Elastic and Inelastic Scattering from 152Sm NUCLEAR REACTIONS 152Sm(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ). 152Sm level deduced deformation parameters β2(p), β2(n) equality. DWIA, coupled-channels.
doi: 10.1103/PhysRevC.28.2165
1983NA20 Phys.Rev.Lett. 51, 1526 (1983) S.K.Nanda, C.Glashausser, K.W.Jones, J.A.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, H.Ohnuma, M.Franey, M.Gazzaly, N.Hintz Fine Structure and Spin Excitations in the Giant Resonance Region of 90Zr NUCLEAR REACTIONS 90Zr(polarized p, p'), E=319 MeV; measured σ(θ), σ(Ep'), analyzing power vs θ, spin-flip probabilities. 90Zr deduced M1 giant resonance, fine structure.
doi: 10.1103/PhysRevLett.51.1526
1983SE15 Phys.Rev. C28, 1301 (1983) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, C.L.Morris, R.L.Boudrie, H.A.Thiessen Analysis of Elastic and Inelastic Scattering of 162 MeV Pions from 13C by an Optical Potential and a Collective Model NUCLEAR REACTIONS 13C(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=162 MeV; measured σ(θ). 13C levels deduced neutron, proton B(λ) components. Optical, collective model analyses.
doi: 10.1103/PhysRevC.28.1301
1982BL01 Phys.Rev. C25, 422 (1982) G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray Elastic and Inelastic Scattering of 0.8 GeV Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), (p, p'), E=0.8 GeV; measured σ(θ). 24,26Mg deduced deformation lengths, multipole moments. Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.25.422
1982CA08 Phys.Rev.Lett. 49, 266 (1982) T.A.Carey, J.M.Moss, S.J.Seestrom-Morris, A.D.Bacher, D.W.Miller, H.Nann, C.Olmer, P.Schwandt, E.J.Stephenson, W.G.Love Polarization and Analyzing-Power Differences in the Excitation of 1+ States in 12C at 150 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=150 MeV; measured polarization, analyzing power difference vs θ. 12C level deduced transition density matrix elements. Q2DM magnetic spectrometer.
doi: 10.1103/PhysRevLett.49.266
1982MO01 Phys.Lett. 108B, 172 (1982) C.L.Morris, W.B.Cottingame, S.J.Greene, C.J.Harvey, C.F.Moore, D.B.Holtkamp, S.J.Seestrom-Morris, H.T.Fortune Indication of Δ-Hole Configurations in 12C(15.11 MeV) NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=100, 180, 230 MeV; measured σ(θ, E(π)). 12C level deduced isobar-hole configuration component. DWIA, Cohen-Kurath transition densities, Fermi momentum corrections.
doi: 10.1016/0370-2693(82)91168-6
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