NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.Kelsey Found 5 matches. 2020EP03 Phys.Rev. D 102, 012006 (2020) C.S.Epstein, R.Johnston, S.Lee, J.C.Bernauer, R.Corliss, K.Dow, P.Fisher, I.Friscic, D.Hasell, R.G.Milner, P.Moran, S.G.Steadman, Y.Wang, J.Dodge, E.Ihloff, J.Kelsey, C.Vidal, C.M.Cooke Measurement of Moller scattering at 2.5 MeV NUCLEAR REACTIONS C(E, E'), E=2.5 MeV; measured reaction products, Eβ, Iβ; deduced σ(θ). Comparison with GEANT4 simulations.
doi: 10.1103/PhysRevD.102.012006
1998HO20 Phys.Rev. C58, 3205 (1998) M.Holtrop, D.Jordan, T.McIlvain, R.Alarcon, R.Beck, W.Bertozzi, V.Bhushan, W.Boeglin, J.P.Chen, D.Dale, G.Dodson, S.Dolfini, K.Dow, J.Dzengeleski, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, K.Joo, J.Kelsey, W.Kim, R.Laszewski, R.Lourie, J.Mandeville, D.J.Margaziotis, D.Martinez, R.Miskimen, C.Papanicolas, S.Penn, W.Sapp, A.J.Sarty, D.Tieger, C.Tschalaer, W.Turchinetz, G.Warren, L.Weinstein, S.Williamson Measurement of the Interference Structure Function RLT for the 12C(e, e'p) Reaction in the Quasielastic Region NUCLEAR REACTIONS 12C(e, e'p), E=576 MeV; measured ep-coin, σ(E, θ(e), θ(p)); deduced interference structure function R(LT) vs missing energy. HF-RPA calculations.
doi: 10.1103/PhysRevC.58.3205
1996JO09 Phys.Rev.Lett. 76, 1579 (1996) D.Jordan, T.McIlvain, R.Alarcon, R.Beck, W.Bertozzi, V.Bhushan, W.Boeglin, J.P.Chen, D.Dale, G.Dodson, S.Dolfini, K.Dow, J.Dzengeleski, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, K.Joo, J.Kelsey, W.Kim, R.Laszewski, R.Lourie, J.Mandeville, D.Margaziotis, D.Martinez, R.Miskimen, C.N.Papanicolas, S.Penn, W.Sapp, A.J.Sarty, D.Tieger, C.Tschalaer, W.Turchinetz, G.Warren, L.Weinstein, S.Williamson Measurement of the Longitudinal, Transverse, and Longitudinal-Transverse Structure Functions in the 2H(e, e'p)n Reaction NUCLEAR REACTIONS 2H(e, e'p), E=577, 292 MeV; measured σ(θ(e'), θ(np)) vs energy transfer; deduced longitudinal, transverse, longitudinal-transverse interference structure function.
doi: 10.1103/PhysRevLett.76.1579
1995BL25 Nucl.Instrum.Methods Phys.Res. A354, 437 (1995) C.Bloch, J.Doskow, C.D.Goodman, W.W.Jacobs, M.Leuschner, H.O.Meyer, B.von Przewoski, T.Rinckel, G.Savopulos, A.Smith, J.Sowinski, F.Sperisen, W.K.Pitts, D.DeSchepper, R.Ent, J.-O.Hansen, J.Kelsey, W.Korsch, L.H.Kramer, K.Lee, N.C.R.Makins, R.G.Milner, S.F.Pate, C.Tschalar, T.P.Welch, D.Marchlenski, E.Sugarbaker, W.Lorenzon, P.V.Pancella, J.F.J.van den Brand, H.J.Bulten, C.E.Jones, M.A.Miller, J.Neal, O.Unal, Z.-L.Zhou Spin-Dependent Scattering of Polarized Protons from a Polarized 3He Internal Gas Target NUCLEAR REACTIONS 3He(polarized p, p), E=197-414 MeV; measured (θp, E(3He)) correlation. 3He(p, 2p), E=197 MeV; measured E(recoil), missing momentum correlation, other features. Laser optically pumped polarized target, circulating proton beams.
doi: 10.1016/0168-9002(94)01057-9
1995KR22 Nucl.Instrum.Methods Phys.Res. A365, 49 (1995) L.H.Kramer, J.F.Kelsey, R.G.Milner, P.Winn, J.McGuire A Cryogenic Storage Cell for Polarized Internal Gas Targets
doi: 10.1016/0168-9002(95)00498-X
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