NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.J.Ernst Found 47 matches. 2012BU11 Phys.Rev. C 85, 068501 (2012) H.R.Burroughs, B.K.Cogswell, J.Escamilla Roa, D.C.Latimer, D.J.Ernst Calculating error bars for neutrino mixing parameters
doi: 10.1103/PhysRevC.85.068501
2010ES01 Phys.Rev. C 81, 015501 (2010) J.Escamilla Roa, D.C.Latimer, D.J.Ernst Implications of the Super-K atmospheric, long baseline, and reactor data for the mixing angles φ13 and φ23
doi: 10.1103/PhysRevC.81.015501
2010ES04 Phys.Rev. C 82, 028501 (2010) J.Escamilla Roa, D.C.Latimer, D.J.Ernst Impact of hierarchy upon the values of neutrino mixing parameters
doi: 10.1103/PhysRevC.82.028501
2007LA13 Phys.Rev. C 75, 042501 (2007) D.C.Latimer, J.Escamilla, D.J.Ernst Measuring the mass of a sterile neutrino with a very short baseline reactor experiment
doi: 10.1103/PhysRevC.75.042501
2007LA35 Phys.Rev. C 76, 055502 (2007) D.C.Latimer, J.Escamilla, D.J.Ernst Detecting CP violation in a single neutrino oscillation channel at very long baselines
doi: 10.1103/PhysRevC.76.055502
2005LA16 Phys.Rev. C 71, 062501 (2005) Neutrino oscillations: Measuring Θ13 including its sign
doi: 10.1103/PhysRevC.71.062501
2005LA31 Phys.Rev. C 72, 045502 (2005) Correlations between θ13 and θ23 in a very long baseline neutrino oscillation experiment
doi: 10.1103/PhysRevC.72.045502
2001ER06 Phys.Rev. C64, 035201 (2001) Mesonic Cloud Contribution to the Nucleon and Δ Masses
doi: 10.1103/PhysRevC.64.035201
2001MA09 Phys.Rev. C63, 024902 (2001) D.E.Malov, A.S.Umar, D.J.Ernst, D.J.Dean Relativistic Heavy-Ion Collisions in the Dynamical String-Parton Model NUCLEAR REACTIONS S, 197Au(p, X), E=200 GeV; S(S, X), E=200 GeV/nucleon; Pb(Pb, X), E=156 GeV/nucleon; calculated fragment rapidity distributions. Dynamical string-parton model, comparisons with data.
doi: 10.1103/PhysRevC.63.024902
2000ER11 Acta Phys.Hung.N.S. 11, 239 (2000) D.J.Ernst, D.E.Malov, A.S.Umar Classical Strings and Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 1H(p, X), E(cm)=30.4 GeV; S, Ar, Au(p, X), E=200 GeV/nucleon; S(S, X), E=200 GeV/nucleon; calculated multiplicity and rapidity distributions. Comparison with data. String-parton model.
1999CH10 Phys.Rev. C59, 2627 (1999) C.M.Chen, D.J.Ernst, M.B.Johnson Phenomenology of K+-Nucleus Scattering NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, X), E at 488-714 MeV/c; analyzed total σ; 6Li, 12C(K+, K+), E at 714 MeV/c; analyzed σ(θ); deduced potential parameters, phenomenological density term.
doi: 10.1103/PhysRevC.59.2627
1999GU10 Ann.Phys.(New York) 272, 7 (1999) M.C.Guclu, J.Li, A.S.Umar, D.J.Ernst, M.R.Strayer Electromagnetic Lepton-Pair Production in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E=160 GeV/nucleon; 197Au(S, X), E=200 GeV/nucleon; calculated lepton pair production σ(E); deduced impact parameter dependence. Two-photon external filed model, hybrid Monte Carlo technique. Comparison with data.
doi: 10.1006/aphy.1998.5876
1999MA17 Phys.Rev. C59, 2289 (1999) D.E.Malov, A.S.Umar, D.J.Ernst, D.J.Dean Hadronic Structure Functions as Distributions of Classical Strings
doi: 10.1103/PhysRevC.59.2289
1999MA74 Int.J.Mod.Phys. E8, 299 (1999) D.E.Malov, A.S.Umar, D.J.Ernst, D.J.Dean Particle Identification in the Dynamical String-Parton Model of Relativistic Heavy-Ion Collisions
doi: 10.1142/S0218301399000215
1998CH42 Phys.Rev. C58, 3500 (1998) C.M.Chen, M.B.Johnson, D.J.Ernst Forward Elastic Amplitudes of High-Energy Pions and Kaons on Nuclei NUCLEAR REACTIONS 12C(π+, π+), E at 610 MeV/c; calculated scattering amplitudes. 12C(π-, π-), E at 500-1100 MeV/c; analyzed total σ; deduced nuclear medium effects in forward scattering amplitudes.
doi: 10.1103/PhysRevC.58.3500
1997KA22 Phys.Rev. C55, 2533 (1997) G.Kahrimanis, G.Burleson, C.M.Chen, B.C.Clark, K.Dhuga, D.J.Ernst, J.A.Faucett, H.T.Fortune, S.Hama, A.Hussein, M.F.Jiang, K.W.Johnson, L.Kurth Kerr, S.Mathews, J.McGill, C.F.Moore, S.Mordechai, C.L.Morris, J.O'Donnell, M.Snell, M.Rawool-Sullivan, L.Ray, C.Whitley, A.L.Williams Pion-Nucleus Elastic Scattering on 12C, 40Ca, 90Zr, and 208Pb at 400 and 500 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(π+, π+), (π-, π-), E=400, 500 MeV; 90Zr(π+, π+), E=400, 500 MeV; 90Zr(π-, π-), E=400 MeV; measured σ(θ). 208Pb(π+, π+), (π-, π-), E=662.7 MeV; 40Ca(π+, π+), (π-, π-), 12C(π+, π+), E=672.5 MeV; 12C(π-, π-), E=672.5, 486.2 MeV; analyzed σ(θ). Impulse approximation approach.
doi: 10.1103/PhysRevC.55.2533
1997MC03 Phys.Lett. 410B, 67 (1997) Off-Shell Behavior of the Crossed Nucleon Pole in Pion-Nucleus Scattering
doi: 10.1016/S0370-2693(97)00941-6
1996MI13 Phys.Lett. 382B, 29 (1996) R.Michael, M.B.Barakat, S.Bart, R.E.Chrien, B.C.Clark, D.J.Ernst, S.Hama, K.H.Hicks, W.Hinton, E.V.Hungerford, M.G.Jiang, T.Kishimoto, C.M.Kormanyos, L.J.Kurth, L.Lee, B.Mayes, R.J.Peterson, L.Pinsky, R.Sawafta, R.Sutter, L.Tang, J.E.Wise K+ Elastic Scattering from C and 6Li at 715 MeV/c NUCLEAR REACTIONS 12C, 6Li(K+, K+), E at 715 MeV/c; measured σ(θ). Parameter-free impluse approximation.
doi: 10.1016/0370-2693(96)00664-8
1995CH33 Phys.Rev. C52, R485 (1995) C.M.Chen, D.J.Ernst, M.F.Jiang, M.B.Johnson Pion-Nucleus Scattering and Baryon Resonances in the Nuclear Medium NUCLEAR REACTIONS 238U(γ, X), E=0.2-1.2 GeV; 12C(π, X), E=0.4-1 GeV; analyzed σ(E); deduced baryon resonances induced medium modifications role.
doi: 10.1103/PhysRevC.52.R485
1995JI02 Phys.Rev. C51, 857 (1995) M.F.Jiang, D.J.Ernst, C.M.Chen Target Dependence of K+-Nucleus Total Cross Sections NUCLEAR REACTIONS 2H(K+, X), E at 400-1000 MeV/c; 12C(K+, X), E at 400-1000 MeV/c; calculated σ. Relativistic optical model, momentum representation.
doi: 10.1103/PhysRevC.51.857
1995JI03 Phys.Rev. C51, 1037 (1995) Relativistic Momentum-Space Optical Model and Meson-Deuteron Scattering NUCLEAR REACTIONS 2H(K+, K+), (π+, π+), E at 400-1000 MeV/c; calculated σ vs momentum. 2H(K+, K+), E=0.4-1 GeV; calculated σ(θ).
doi: 10.1103/PhysRevC.51.1037
1994MC01 Phys.Rev. C49, 1087 (1994) Double-Doorway Model for Pion-Nucleon Elastic Scattering in the S11 Channel
doi: 10.1103/PhysRevC.49.1087
1994RA02 Phys.Rev. C49, 627 (1994) M.W.Rawool-Sullivan, C.L.Morris, J.M.O'Donnell, R.M.Whitton, B.K.Park, G.R.Burleson, D.L.Watson, J.Johnson, A.L.Williams, D.A.Smith, D.J.Ernst, C.M.Chen Pion Elastic Scattering on 28Si at T(π) = 400 MeV NUCLEAR REACTIONS 28Si(π+, π+), (π-, π-), E=400 MeV; measured σ(θ), σ(E(π), θ(π)). Momentum-space first-order optical model.
doi: 10.1103/PhysRevC.49.627
1993CH04 Phys.Rev. C47, R9 (1993) C.M.Chen, D.J.Ernst, M.B.Johnson Microscopic Approach to Pion-Nucleus Dynamics NUCLEAR REACTIONS 12C(π+, π+), E=80-226 MeV; calculated σ(θ). First-order optical potential, second-order corrections microscopic estimates.
doi: 10.1103/PhysRevC.47.R9
1993CH25 Phys.Rev. C48, 841 (1993) C.M.Chen, D.J.Ernst, M.B.Johnson High-Energy Pion-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca(π-, π-), E=180-780 MeV; 12C(π+, π+), (π-, π-), E at 800 MeV/c; calculated σ(θ). A 'model-exact' calculation, lowest-order microscopic optical model.
doi: 10.1103/PhysRevC.48.841
1992CH11 Phys.Rev. C45, 2019 (1992) K+-Nucleus Scattering and the Nucleon in the Nuclear Medium NUCLEAR REACTIONS 12C, 40Ca(K+, K+), E=446 MeV; calculated σ(θ). 12C(K+, X), E at ≈ 400-750 MeV/c; calculated σ vs momentum. Covariant, momentum space optical potential.
doi: 10.1103/PhysRevC.45.2019
1990ER01 Phys.Lett. 237B, 164 (1990) Delta-Nucleus Coulomb Interaction in Resonant-Energy Pion-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca(π+, π+), (π-, π-), E=180 MeV; analyzed σ(θ); deduced Δ-nucleus potential parameters. Mean-spectral approximation.
doi: 10.1016/0370-2693(90)91422-8
1990ER06 Nucl.Phys. A518, 658 (1990) D.J.Ernst, G.E.Parnell, C.Assad Doorway-Resonance Model for Pion-Nucleon D- and F-Wave Scattering NUCLEAR REACTIONS 12C(π+, π+), E=50 MeV; calculated σ(θ). Doorway resonance model.
doi: 10.1016/0375-9474(90)90184-N
1988ER01 J.Phys.(London) G14, L37 (1988) Inclusive γ and π0 Cross Sections in Heavy-Ion Reactions NUCLEAR REACTIONS Ni(14N, π0X), (14N, γX), E=35 MeV/nucleon; calculated pion, γ-production σ.
doi: 10.1088/0305-4616/14/1/008
1988ER04 Phys.Rev. C37, 2651 (1988) Delta-Hole Model in the Local-Density Approximation NUCLEAR REACTIONS 12C, 40Ca, 16O(π+, π+), E=162 MeV; calculated σ(θ). Isobar-hole model.
doi: 10.1103/PhysRevC.37.2651
1988PA06 Phys.Lett. 205B, 135 (1988) G.E.Parnell, D.J.Ernst, D.R.Giebink Pion-Nucleus Single-Charge Exchange above the Δ Resonance NUCLEAR REACTIONS 14C, 90Zr(π+, π-), E ≈ 50-500 MeV; calculated σ(θ). Microscopic, momentum, isospin invariant optical potential.
doi: 10.1016/0370-2693(88)91635-8
1986ER11 Phys.Lett. 182B, 242 (1986) D.J.Ernst, D.R.Giebink, M.B.Johnson Dispersive Effects in Low Energy Pion-Nucleus Scattering NUCLEAR REACTIONS 16O(π+, π+), E=40, 60 MeV; calculated σ(θ); deduced pion nucleus scattering dispersive effects. Three calculational methods.
doi: 10.1016/0370-2693(86)90082-1
1985DH01 Phys.Rev. C32, 2208 (1985) K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, N.Tanaka, Z.F.Wang, S.Nanda, D.Dehnhard, J.D.Zumbro, S.Mordechai, C.F.Moore, D.J.Ernst Large-Angle Elastic Scattering of π+ and π- from 16O at 114 MeV NUCLEAR REACTIONS 16O(π+, π+), (π-, π-), E=114 MeV; measured σ(θ); deduced large σ(π+)/σ(π-) differences. First-, second-order optical model calculations.
doi: 10.1103/PhysRevC.32.2208
1985ER03 Phys.Rev. C32, 940 (1985) Dispersive Effects in Pion-Nucleus Scattering NUCLEAR REACTIONS 40Ca(π, π), E=165 MeV; calculated potentials. 16O(π+, π+), E=114, 163, 240 MeV; calculated σ(θ). 16O(π, π), (π, π'), E ≈ 40-280 MeV; calculated elastic, inelastic, total σ(E). Impulse approximation, dispersive medium effects.
doi: 10.1103/PhysRevC.32.940
1984UM02 Phys.Lett. 140B, 290 (1984) A.S.Umar, M.R.Strayer, D.J.Ernst A Time-Dependent External-Field Model for Particle Emission in Heavy-Ion Reactions NUCLEAR REACTIONS 93Nb(16O, nX), E=204 MeV; calculated inclusive nonequilibrium neutron emission probability vs t. Time-dependent external field model.
doi: 10.1016/0370-2693(84)90755-X
1984UM05 Phys.Rev. C30, 1934 (1984) A.S.Umar, M.R.Strayer, D.J.Ernst, K.R.Sandhya Devi Mean-Field Theory of Prompt, High-Energy Nucleon Emission NUCLEAR REACTIONS 93Nb(16O, X), E=204 MeV; calculated σ(θn, En) following fragment neutron emission. Time-dependent mean field theory.
doi: 10.1103/PhysRevC.30.1934
1983ER04 Phys.Rev. C27, 2733 (1983) D.J.Ernst, G.A.Miller, D.L.Weiss Fermi Integration in the Pion-Nucleus Optical Potential NUCLEAR REACTIONS 16O(π+, π+), E=79, 162, 240 MeV; 208Pb(π+, π+), E=80, 162 MeV; calculated σ(θ). First-order optical potential, factorization approximation correction, Fermi integration.
doi: 10.1103/PhysRevC.27.2733
1982WE09 Phys.Rev. C26, 605 (1982) Kinematic Aspects of Pion-Nucleus Elastic Scattering NUCLEAR REACTIONS 4He(π+, π+), E=60, 180, 260 MeV; 12C(π+, π+), E=180 MeV; calculated σ(θ). Relativistic kinematics, target recoil, impulse approximation.
doi: 10.1103/PhysRevC.26.605
1980ER02 Phys.Rev. C21, 1472 (1980) Relativistic Kinematics for Elastic Pion-Nucleus Scattering NUCLEAR REACTIONS 12C(π+, π+), E=60, 120, 162, 180 MeV; calculated σ(θ). Impulse approximation, time-reversal invariance, relativistic kinematic transformations.
doi: 10.1103/PhysRevC.21.1472
1980ER07 Phys.Rev. C22, 651 (1980) Simple Model of Pion-Nucleon Elastic Scattering NUCLEAR REACTIONS 1H(π, π), E=1.2 GeV; calculated s-, p-, d-, f-, wave phase shifts. Extended Chew-Low models, separable potential.
doi: 10.1103/PhysRevC.22.651
1979AN03 Phys.Rev. C19, 905 (1979) B.D.Anderson, P.R.Bevington, F.H.Cverna, M.W.McNaughton, H.B.Willard, R.J.Barrett, N.S.P.King, D.J.Ernst Proton Total Reaction Cross Section Measurements for 40,44,48Ca at 700 MeV NUCLEAR REACTIONS 40,44,48Ca(p, X), E=700 MeV; measured total reaction σ; deduced matter radii differences.
doi: 10.1103/PhysRevC.19.905
1979ER02 Phys.Rev. C19, 896 (1979) Total Reaction Cross Sections and the Matter Density of Finite Nuclei NUCLEAR REACTIONS 12C, 16O, 40,44,48Ca, 208Pb(p, X), E=100 MeV-1 GeV; calculated total reaction σ. Impulse approximation with eikonal propogator.
doi: 10.1103/PhysRevC.19.896
1979JO06 Phys.Rev. C20, 1064 (1979) Off-Shell Sensitivity in Relativistic Schrodinger and Klein-Gordon Optical Models of Pion-Nucleus Interactions NUCLEAR REACTIONS 12C(π0, π0), E=40, 160, 180 MeV; calculated σ(θ), total, reaction σ; deduced sensitivity to (3-3) resonance energy. Relativistic Schrodinger, Klein-Gordon equations.
doi: 10.1103/PhysRevC.20.1064
1975ER08 Phys.Rev. C12, 1962 (1975) Implications of High Energy Pion-Nucleon Scattering Data for Pion-Nucleus Scattering NUCLEAR REACTIONS 12C(π+, π+), E=75, 150, 250 MeV; 40Ca(π+, π+), E=75 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.12.1962
1975NA07 Phys.Rev. C11, 1167 (1975) M.A.Nagarajan, W.L.Wang, D.J.Ernst, R.M.Thaler Relation between the Watson and Kerman-McManus-Thaler Multiple Scattering Formalisms NUCLEAR REACTIONS 4He, 12C, 40Ca(p, p), E=90, 310, 1050 MeV; calculated σ.
doi: 10.1103/PhysRevC.11.1167
1973ER10 Phys.Rev. C8, 440 (1973) D.J.Ernst, C.M.Shakin, R.M.Thaler Center-of-Mass Motion and Angular Momentum Projection NUCLEAR STRUCTURE 12C, 20Ne, 28Si, 36Ar; calculated rotational energies.
doi: 10.1103/PhysRevC.8.440
1972ER07 Phys.Rev. C6, 1522 (1972) Pauli Principle and the Linked Cluster Expansion for the Nuclear Optical Potential
doi: 10.1103/PhysRevC.6.1522
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