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Search: Author = R.A.Arndt

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2012WO06      Phys.Rev. C 86, 035202 (2012)

R.L.Workman, R.A.Arndt, W.J.Briscoe, M.W.Paris, I.I.Strakovsky

Parameterization dependence of T-matrix poles and eigenphases from a fit to πN elastic scattering data

doi: 10.1103/PhysRevC.86.035202
Citations: PlumX Metrics


2011LA16      J.Korean Phys.Soc. 59, 995s (2011)

A.B.Laptev, R.C.Haight, R.A.Arndt, W.J.Briscoe, M.W.Paris, I.I.Strakovsky, R.L.Workman

The Recent Absolute Total np and pp Cross Section Determinations: Quality of Data Description and Prediction of Experimental Observables

NUCLEAR REACTIONS 1H(p, p), E=0-3000 MeV;1H(n, n), E=0-1300 MeV; calculated, analyzed np and pp SAID facility scattering σ; evaluated σ using partial-wave analysis.

doi: 10.3938/jkps.59.995
Citations: PlumX Metrics


2009AR07      Nucl.Sci.Eng. 162, 312 (2009)

R.A.Arndt, W.J.Briscoe, A.B.Laptev, I.I.Strakovsky, R.L.Workman

Absolute Total np and pp Cross-Section Determinations

doi: 10.13182/NSE162-312
Citations: PlumX Metrics


2009WO02      Phys.Rev. C 79, 038201 (2009)

R.L.Workman, R.A.Arndt, M.W.Paris

Resonance parameters from K-matrix and T-matrix poles

doi: 10.1103/PhysRevC.79.038201
Citations: PlumX Metrics


2007AR22      Phys.Rev. C 76, 025209 (2007)

R.A.Arndt, W.J.Briscoe, I.I.Strakovsky, R.L.Workman

Updated analysis of NN elastic scattering to 3 GeV

doi: 10.1103/PhysRevC.76.025209
Citations: PlumX Metrics


2006AR20      Phys.Rev. C 74, 045205 (2006)

R.A.Arndt, W.J.Briscoe, I.I.Strakovsky, R.L.Workman

Extended partial-wave analysis of πN scattering data

NUCLEAR REACTIONS 1H(π+, π+), (π-, π-), (π-, π0), E=threshold-2.6 GeV; analyzed data; deduced partial wave amplitudes, resonance features.

doi: 10.1103/PhysRevC.74.045205
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2006WO01      Phys.Atomic Nuclei 69, 90 (2006)

R.L.Workman, R.A.Arndt, D.M.Manley, J.Tulpan, I.I.Strakovsky

Constraints on Narrow Exotic States from K+p and K0Lp Scattering Data

NUCLEAR REACTIONS 1H(K+, K+), (K0, K0), E ≈ 1500-1700 MeV; analyzed σ; deduced no narrow exotic resonances.

doi: 10.1134/S1063778806010121
Citations: PlumX Metrics


2005AR14      Nucl.Phys. A754, 261c (2005)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

K+N scattering data and exotic Z+ resonances

doi: 10.1016/j.nuclphysa.2004.12.069
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2005AR28      Phys.Rev. C 72, 045202 (2005)

R.A.Arndt, W.J.Briscoe, T.W.Morrison, I.I.Strakovsky, R.L.Workman, A.B.Gridnev

Low-energy ηN interactions: Scattering lengths and resonance parameters

NUCLEAR REACTIONS 1H(π-, X), E at 684.5-770 MeV/c; analyzed η-meson production σ(θ); deduced scattering lengths, resonance parameters.

doi: 10.1103/PhysRevC.72.045202
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2005AR29      Phys.Rev. C 72, 058203 (2005)

R.A.Arndt, W.J.Briscoe, I.I.Strakovsky, R.L.Workman

Helicity-dependent photoabsorption cross sections on the nucleon

NUCLEAR REACTIONS 1n, 1H(γ, X), E ≈ 500-2000 MeV; analyzed single-pion and single-η photoabsorbtion data, contributions to sum rule.

doi: 10.1103/PhysRevC.72.058203
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2005AZ10      Eur.Phys.J. A 26, 79 (2005)

Ya.I.Azimov, R.A.Arndt, I.I.Strakovsky, R.L.Workman, K.Goeke

Search for higher flavor multiplets in partial-wave analyses

doi: 10.1140/epja/i2005-10150-y
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2004AR08      Phys.Rev. C 69, 035208 (2004)

R.A.Arndt, Ya.I.Azimov, M.V.Polyakov, I.I.Strakovsky, R.L.Workman

Nonstrange and other flavor partners of the exotic Θ+ baryon

doi: 10.1103/PhysRevC.69.035208
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2004AR09      Phys.Rev. C 69, 035213 (2004)

R.A.Arndt, W.J.Briscoe, I.I.Strakovsky, R.L.Workman

Dispersion relation constrained partial wave analysis of πN elastic and πN → ηN scattering data: The baryon spectrum

NUCLEAR REACTIONS 1H(π+, π+), (π-, π-), (π-, π0), (π-, X), E=threshold-2.1 GeV; analyzed elastic, charge-exchange, and η production data; deduced parameters, resonance features. Dispersion relation constrained partial wave analysis.

doi: 10.1103/PhysRevC.69.035213
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2004BR48      Fizika(Zagreb) B 13, 115 (2004)

W.J.Briscoe, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Production of pseudoscalar mesons


2004WO15      Phys.Rev. C 70, 028201 (2004)

R.L.Workman, R.A.Arndt, I.I.Strakovsky, D.M.Manley, J.Tulpan

Effect of exotic S = +1 resonances on K0Lp scattering data

NUCLEAR REACTIONS 1H(K0, X), E at 250-550 MeV/c; analyzed σ; deduced exotic resonance contribution.

doi: 10.1103/PhysRevC.70.028201
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2003AR05      Phys.Rev. C 67, 048201 (2003)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Effect of double-polarization data in fits to single-pion photoproduction

NUCLEAR REACTIONS 1H(γ, π0X), E=800-2000 MeV; analyzed polarization transfer observables, multipole amplitudes.

doi: 10.1103/PhysRevC.67.048201
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2003AR25      Phys.Rev. C 68, 042201 (2003); Erratum Phys.Rev. C 69, 019901 (2004)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

K+-nucleon scattering and exotic S = +1 baryons

NUCLEAR REACTIONS 1n, 1H(K+, K+), E < 2.65 GeV; analyzed invariant mass spectra; deduced resonance features.

doi: 10.1103/PhysRevC.68.042201
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2003AR28      Nucl.Phys. A721, 769c (2003)

R.A.Arndt, W.J.Briscoe, G.V.O'Rielly, I.I.Strakovsky, R.L.Workman

Photoproduction of Pseudoscalar Mesons

NUCLEAR REACTIONS 1H(γ, X), E ≈ 0.4-1.4 GeV; analyzed pseudoscalar meson production σ, σ(θ).

doi: 10.1016/S0375-9474(03)01177-1
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2003AZ06      Phys.Rev. C 68, 045204 (2003)

Ya.I.Azimov, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Light baryon resonances: Restrictions and perspectives

doi: 10.1103/PhysRevC.68.045204
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2002AR18      Phys.Rev. C 66, 055213 (2002)

R.A.Arndt, W.J.Briscoe, I.I.Strakovsky, R.L.Workman

Analysis of pion photoproduction data

NUCLEAR REACTIONS 1n(π0, γX), (π+, γX), E=1-2 GeV; 1H(π0, γX), (π-, γX), E=1-2 GeV; analyzed σ(θ), partial wave amplitudes.

doi: 10.1103/PhysRevC.66.055213
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2002KA67      Phys.Rev. C 66, 065206 (2002)

S.S.Kamalov, L.Tiator, D.Drechsel, R.A.Arndt, C.Bennhold, I.I.Strakovsky, R.L.Workman

Dispersion relation analysis of neutral pion photoproduction and electroproduction at threshold

NUCLEAR REACTIONS 1H(γ, π0), (e, e'π0), E ≈ threshold; analyzed data; deduced multipole contributions. Dispersion relation analysis.

doi: 10.1103/PhysRevC.66.065206
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2001AD05      Phys.Rev. C63, 054606 (2001)

F.V.Adamian, A.Yu.Buniatian, G.S.Frangulian, P.I.Galumian, V.H.Grabsky, A.V.Hairapetian, H.H.Hakopian, V.K.Hoktanian, J.V.Manukian, A.M.Sirunian, A.H.Vartapetian, H.H.Vartapetian, V.G.Volchinsky, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Measurement of the Cross Section Asymmetry of the Reaction γp → π0p in the Resonance Energy Region Eγ = 0.5-1.1 GeV

NUCLEAR REACTIONS 1H(polarized γ, π0), E=0.5-1.1 GeV; measured cross section asymmetry Σ. Comparison with previous work, model predictions.

doi: 10.1103/PhysRevC.63.054606
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2000AR12      Phys.Scr. T87, 62 (2000)

R.A.Arndt, I.I.Strakovsky, R.L.Workman, M.M.Pavan

Sensitivity to the Pion-Nucleon Coupling Constant in Partial-Wave Analyses of πN → πN, NN → NN, and γN → πN

doi: 10.1238/Physica.Topical.087a00062
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2000AR14      Phys.Rev. C62, 034005 (2000)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Nucleon-Nucleon Elastic Scattering to 3 GeV

NUCLEAR REACTIONS 1H(n, n), (p, p), E < 3 GeV; analyzed polarized, unpolarized data; deduced partial wave amplitudes, phase shift parameters.

doi: 10.1103/PhysRevC.62.034005
Citations: PlumX Metrics


2000PA46      Phys.Scr. T87, 65 (2000)

M.M.Pavan, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Determination of the πNN Coupling Constant in the VPI/GWU πN → πN Partial-Wave and Dispersion Relation Analysis

doi: 10.1238/Physica.Topical.087a00065
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2000WO10      Phys.Rev. C62, 048201 (2000)

R.Workman, R.A.Arndt, I.I.Strakovsky

Extraction of the D13(1520) Photon-Decay Couplings from Pion- and η-Photproduction data

NUCLEAR REACTIONS 1H(γ, π0), E=762 MeV; analyzed σ(θ), recoil polarization; deduced D13 resonance decay couplings, related features. Comparison with η-production data.

doi: 10.1103/PhysRevC.62.048201
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1999DA06      Phys.Rev. C59, 1059 (1999)

R.M.Davidson, N.C.Mukhopadhyay, M.S.Pierce, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Problems with Extraction of the Nucleon to Δ(1232) Photonic Amplitudes

NUCLEAR REACTIONS 1H(γ, π0), E=340 MeV; analyzed σ(θ); deduced little model dependence.

doi: 10.1103/PhysRevC.59.1059
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1999WO02      Phys.Rev. C59, 1810 (1999)

R.L.Workman, R.A.Arndt

Stability of the E2/M1 Ratio at the T-Matrix Pole

doi: 10.1103/PhysRevC.59.1810
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1998AR18      Phys.Rev. C58, 3636 (1998)

R.A.Arndt, A.M.Green, R.L.Workman, S.Wycech

Energies and Residues of the Nucleon Resonances N(1535) and N(1650)

NUCLEAR STRUCTURE 1n, 1H; calculated resonances E, Γ, pole positions.

doi: 10.1103/PhysRevC.58.3636
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1997AL07      Phys.Rev. C55, 2049 (1997)

I.G.Alekseev, V.P.Kanavets, B.V.Morozov, D.N.Svirida, S.P.Kruglov, A.A.Kulbardis, V.V.Sumachev, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Influence of Spin-Rotation Measurements on Partial-Wave Analyses of Elastic Pion-Nucleon Scattering

NUCLEAR REACTIONS 1H(π+, π+), E=1.3 GeV; analyzed spin rotation parameter vs θ, partial wave amplitudes; deduced Barrelet transformation, spin rotation influences on amplitude.

doi: 10.1103/PhysRevC.55.2049
Citations: PlumX Metrics


1997AR11      Phys.Rev. C56, 577 (1997)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Pion Photoproduction in the Δ Resonance Region

doi: 10.1103/PhysRevC.56.577
Citations: PlumX Metrics


1997AR12      Phys.Rev. C56, 579 (1997)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Comment on ' Measurement of the π+p(pol) Analyzing Power at 68.3 MeV '

NUCLEAR REACTIONS 1H(π+, π+), E=68.3 MeV; analyzed data analyses; deduced analyzing power role f2, Σ amplitude. Polarized target.

doi: 10.1103/PhysRevC.56.579
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1997AR26      Phys.Rev. C56, 3005 (1997)

R.A.Arndt, H.O.Chang, I.I.Strakovsky, R.L.Workman, F.Dohrmann

Nucleon-Nucleon Elastic Scattering Analysis to 2.5 GeV

NUCLEAR REACTIONS 1H(p, p), E=0-2400 MeV; compiled, analyzed isovector, isoscalar partial wave amplitudes, total σ, σ(θ) for some energies.

doi: 10.1103/PhysRevC.56.3005
Citations: PlumX Metrics


1997CH20      Phys.Rev. C56, 635 (1997)

H.O.Chang, R.A.Arndt, I.I.Strakovsky, R.L.Workman

Combined Analysis of the Reactions pp → pp, πd → πd, and πd → pp

NUCLEAR REACTIONS 1H(p, X), (p, p), E ≈ 2-2.4 GeV; analyzed elastic, total σ vs E. 2H(π, π), (π, 2p), E ≈ 2-2.4 GeV; analyzed amplitudes vs E.

doi: 10.1103/PhysRevC.56.635
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1996AR01      Phys.Rev. C53, 430 (1996)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Updated Resonance Photodecay Amplitudes to 2 GeV

doi: 10.1103/PhysRevC.53.430
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1995AR20      Phys.Rev. C52, 2120 (1995)

R.A.Arndt, I.I.Strakovsky, R.L.Workman, M.M.Pavan

Updated Analysis of πN Elastic Scattering Data to 2.1 GeV: The baryon spectrum

NUCLEAR REACTIONS 1H(π-, π-), (π+, π+), E ≤ 2.1 GeV; analyzed energy-angle distribution data; deduced resonance parameters. Breit-Wigner fits.

doi: 10.1103/PhysRevC.52.2120
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1995AR21      Phys.Rev. C52, 2246 (1995)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Extraction of the πNN Coupling Constant from NN Scattering Data

NUCLEAR REACTIONS 1n(p, p), E < 350 MeV; analyzed σ(θ); deduced πNN-coupling constant.

doi: 10.1103/PhysRevC.52.2246
Citations: PlumX Metrics


1994AR05      Phys.Rev. C49, 2729 (1994)

R.A.Arndt, R.L.Workman, M.M.Pavan

Pion-Nucleon Partial-Wave Analysis with Fixed-t Dispersion Relation Constraints

doi: 10.1103/PhysRevC.49.2729
Citations: PlumX Metrics


1994AR16      Phys.Rev. C50, 1796 (1994)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Analysis of πd Elastic Scattering Data to 500 MeV

NUCLEAR REACTIONS 2H(π+, π+), (π-, π-), E ≤ 500 MeV; analyzed σ(θ), σ(E), analyzing power data.

doi: 10.1103/PhysRevC.50.1796
Citations: PlumX Metrics


1994AR18      Phys.Rev. C50, 2731 (1994)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Update Analysis of NN Elastic Scattering Data to 1.6 GeV

NUCLEAR REACTIONS 1n, 1H(p, p), E ≤ 1.6 GeV; analyzed data; deduced πNN coupling constant dependence.

doi: 10.1103/PhysRevC.50.2731
Citations: PlumX Metrics


1993AR04      Phys.Rev. C48, 474 (1993)

R.A.Arndt, I.I.Strakovsky, R.L.Workman

Does the πNN Coupling ' Constant ' Vary with Energy ( Question )

NUCLEAR REACTIONS 1H(p, p), E ≤ 800 MeV; analyzed recent data analyses; deduced NΔ-channel role in πNN-coupling constant extraction.

doi: 10.1103/PhysRevC.48.474
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1993AR11      Phys.Rev. C48, 1926 (1993); Erratum Phys.Rev. C49 1229 (1994)

R.A.Arndt, I.I.Strakovsky, R.L.Workman, D.V.Bugg

Analysis of the Reaction π+d → pp to 500 MeV

NUCLEAR REACTIONS 2H(π+, 2p), E=500 MeV; analyzed σ(θ), deuteron vector analyzing power, 2p-spin correlation parameter; deduced dominant partial wave amplitude characteristics. Energy-dependent approach.

doi: 10.1103/PhysRevC.48.1926
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1992AR16      Phys.Rev. D45, 3995 (1992)

R.A.Arndt, L.D.Roper, R.L.Workman, M.W.McNaughton

Nucleon-Nucleon Partial-Wave Analysis to 1.6 GeV

NUCLEAR REACTIONS 1n, 1H(p, p), E < 1.6 GeV; analyzed data; deduced 1D2, 3F3, 3P2, 3F2 partial wave structure. Energy dependent, energy independent analyses.

doi: 10.1103/PhysRevD.45.3995
Citations: PlumX Metrics


1992AR22      Phys.Rev. D46, 1192 (1992)

R.A.Arndt, R.L.Workman

Uncertainties in np Cross Sections from 25-225 MeV

NUCLEAR REACTIONS 1H(n, n), E=25-225 MeV; analyzed σ(θ), polarization data; deduced limits on overall uncertainities.

doi: 10.1103/PhysRevD.46.1192
Citations: PlumX Metrics


1992HY01      Phys.Rev. D46, 961 (1992)

J.S.Hyslop, R.A.Arndt, L.D.Roper, R.L.Workman

Partial-Wave Analysis of K+-Nucleon Scattering

NUCLEAR REACTIONS 2H(K+, X), (K+, K+), E < 2.65 GeV; analyzed data; deduced scattering lengths.

doi: 10.1103/PhysRevD.46.961
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1990AR15      Phys.Rev. C42, 1853 (1990)

R.A.Arndt, R.L.Workman, Z.Li, L.D.Roper

Partial-Wave Analysis of Pion Photoproduction

NUCLEAR REACTIONS 1H(γ, pπ0), (γ, nπ+), 1n(γ, nπ0), (γ, pπ-), E ≤ 1 GeV; analyzed photo pion production data; deduced energy dependent solutions. Energy dependent partial wave analysis.

doi: 10.1103/PhysRevC.42.1853
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1990AR16      Phys.Rev. C42, 1864 (1990)

R.A.Arndt, R.L.Workman, Z.Li, L.D.Roper

Pion Photoproduction Resonance Couplings in the Second Resonance Region

NUCLEAR REACTIONS 1H(γ, pπ), (γ, nπ), 1n(γ, pπ), (γ, nπ), E ≤ 1 GeV; analyzed data; deduced resonance couplings.

doi: 10.1103/PhysRevC.42.1864
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1988AR13      Phys.Rev.Lett. 61, 529 (1988)

R.A.Arndt

Single-Channel Dominance of p-p Inelasticity Near 1 GeV: Parametrizing spin-coupled waves

NUCLEAR REACTIONS 1H(p, p), E=0.8-1.25 GeV; analyzed data; deduced single channel dominance. K-matrix approach.

doi: 10.1103/PhysRevLett.61.529
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1987AR01      Phys.Rev. D35, 128 (1987)

R.A.Arndt, J.S.Hyslop III, L.D.Roper

Nucleon-Nucleon Partial-Wave Analysis to 1100 MeV

NUCLEAR REACTIONS 1H, 1n(p, p), (polarized p, p), E ≤ 1100 MeV; calculated σ(θ), σ(E), partial wave amplitudes vs E; deduced nucleon-nucleon phases. Partial wave analysis.

doi: 10.1103/PhysRevD.35.128
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1983AR27      Phys.Rev. D 28, 97 (1983)

R.A.Arndt, L.D.Roper, R.A.Bryan, R.B.Clark, B.J.VerWest, P.Signell

Nucleon-nucleon partial-wave analysis to 1 GeV

NUCLEAR REACTIONS 1H(p, p), E<1 GeV; analyzed available data; deduced recommended σ.

doi: 10.1103/PhysRevD.28.97
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1983BA05      Phys.Rev. C27, 682 (1983)

M.L.Barlett, G.W.Hoffmann, J.A.McGill, B.Hoistad, L.Ray, R.W.Fergerson, E.C.Milner, J.A.Marshall, J.F.Amann, B.E.Bonner, J.B.McClelland, G.S.Blanpied, R.A.Arndt

Forward-Angle Elastic and Quasielastic Proton-Nucleon Cross Sections and Analyzing Powers at 0.8 GeV

NUCLEAR REACTIONS 1H(p, p), (polarized p, p), E=800 MeV; measured σ(θ), analyzing power vs θ. 2H(polarized p, 2p), (polarized p, pn), E=800 MeV; measured analyzing power vs θ, quasielastic scattering; deduced proton nucleus amplitudes. Liquid hydrogen, deuterium, CH, CH2 targets. 40Ca(polarized p, p), E=800 MeV; analyzed σ(θ), analyzing power data; deduced medium correction effects. Kerman-McManus-Thaler formalism, amplitude input from present data.

doi: 10.1103/PhysRevC.27.682
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0661.


1981BH01      Phys.Rev.Lett. 46, 1111 (1981)

R.Bhandari, R.A.Arndt, L.D.Roper, B.J.VerWest

Existence of Dibaryon Resonances in I=1, 1D2 and 3F3 Nucleon-Nucleon Scattering

NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-1.2 GeV; analyzed phase shift data; deduced dibaryon resonances.

doi: 10.1103/PhysRevLett.46.1111
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1977AR02      Phys.Rev. C15, 1002 (1977)

R.A.Arndt, R.H.Hackman, L.D.Roper

Nucleon-Nucleon Scattering Analyses. II. Neutron-Proton Scattering from 0 to 425 MeV and Proton-Proton Scattering from 1 to 500 MeV

NUCLEAR REACTIONS 1H(n, n), E=1-425 MeV; 1H(p, p), E=1-500 MeV; analyzed data.

doi: 10.1103/PhysRevC.15.1002
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1977AR03      Phys.Rev. C15, 1021 (1977)

R.A.Arndt, R.H.Hackman, L.D.Roper

Nucleon-Nucleon Scattering Analyses. III. np Phase-Shift Analyses: Complex Structure and Multiple Solutions at 50 and 325 MeV

NUCLEAR REACTIONS 1H(n, n), E ≈ 50, 325 MeV; analyzed data.

doi: 10.1103/PhysRevC.15.1021
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1974AR02      Phys.Rev. C9, 555 (1974)

R.A.Arndt, R.H.Hackman, L.D.Roper

Nucleon-Nucleon Scattering Analyses. I. Proton-Proton Scattering, from 1 to 500 MeV

NUCLEAR REACTIONS 1H(p, p), energy-dependent, energy-independent phase-shift analyses of 1-500 MeV p-p scattering data.

doi: 10.1103/PhysRevC.9.555
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1974AR11      Phys.Rev. C9, 2050 (1974)

R.A.Arndt, R.H.Hackman, L.D.Roper

Effects of Coulomb Rotation on the p-p Forward Scattering Amplitude from 0-500 MeV

NUCLEAR REACTIONS 1H(p, p), E=0-500 MeV; calculated Coulomb rotation effects on forward nuclear amplitude, from analytic partial-wave representation of elastic data.

doi: 10.1103/PhysRevC.9.2050
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1972BR10      Phys.Rev. C5, 761 (1972)

W.B.Broste, G.S.Mutchler, J.E.Simmons, R.A.Arndt, L.D.Roper

Polarization Measurements and Analysis in n-4He Scattering from 11.0 to 30.3 MeV

NUCLEAR REACTIONS 4He(n, n), E=11, 17.7, 23.8, 25.7, 27.3, 30.3 MeV; measured P(n)(E;θ); deduced phase shifts.

doi: 10.1103/PhysRevC.5.761
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10163.


1971AR20      Phys.Rev. C3, 2100 (1971)

R.A.Arndt, L.D.Roper, R.L.Shotwell

Analyses of Elastic Proton-Alpha Scattering

NUCLEAR REACTIONS 4He(p, p), E < 25 MeV; measured nothing; analyzed σ(θ); deduced phase shifts.

doi: 10.1103/PhysRevC.3.2100
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