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NSR database version of April 27, 2024.

Search: Author = A.Warwick

Found 7 matches.

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1984GU15      Phys.Lett. 142B, 141 (1984)

H.-A.Gustafsson, H.H.Gutbrod, B.Kolb, H.Lohner, B.Ludewigt, A.M.Poskanzer, T.Renner, H.Riedesel, H.G.Ritter, A.Warwick, H.Wieman

Thermalization in High Energy Nuclear Collisions

NUCLEAR REACTIONS Ca(40Ca, X), (40Ca, pX), E=400, 1050 MeV/nucleon; 93Nb(93Nb, X), (93Nb, pX), E=400, 650 MeV/nucleon; measured σ(θp, Ep), fragment yield isotropy vs charge multiplicity.

doi: 10.1016/0370-2693(84)91249-8
Citations: PlumX Metrics


1982KA33      Phys.Rev. C26, 2694 (1982)

S.B.Kaufman, M.S.Freedman, D.J.Henderson, E.P.Steinberg, B.D.Wilkins, A.Baden, H.H.Gutbrod, M.R.Maier, J.Peter, H.G.Ritter, H.Stelzer, A.I.Warwick, H.H.Wieman, F.Weik

Momentum Transfer to the Target in Peripheral Collisions of Relativistic Heavy Ions

NUCLEAR REACTIONS 197Au(p, F), (α, F), E=5 GeV; 197Au(20Ne, F), E=5-42 GeV; measured fission (fragment)(fragment)(θ); deduced momentum transfer to target.

doi: 10.1103/PhysRevC.26.2694
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2496.


1982WA26      Nucl.Phys. A391, 9 (1982)

A.Warwick, R.Chapman, J.L.Durell, J.N.Mo

Proton Orbit Sizes of the Isotopes of Tin

NUCLEAR REACTIONS 112,116,118,120,124Sn(t, α), E=4.75, 5, 5.25 MeV; measured σ(θ). 112,116,118,120,124Sn deduced rms radii of lg9/2, 2p1/2, 2p3/2 proton orbits. 111,115,117,119,123In level deduced J, π, L, S. Enriched targets.

doi: 10.1016/0375-9474(82)90216-0
Citations: PlumX Metrics


1981WA03      Nucl.Phys. A356, 33 (1981)

A.Warwick, R.Chapman, J.L.Durell, J.N.Mo, J.A.Kuehner, P.Skensved

The 1h9/2 Proton Orbit Size in 209Bi

NUCLEAR REACTIONS 209Bi(t, α), E=8.5, 9 MeV; measured σ(θ). 209Bi deduced rms radius, asymptotic amplitude of the 1h9/2 proton wave function. Zero-range, finite-range DWBA analysis.

doi: 10.1016/0375-9474(81)90116-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1565.


1981WO03      Nucl.Phys. A363, 322 (1981)

P.Woods, R.Chapman, J.L.Durell, J.N.Mo, S.Sen, A.I.Warwick

The 48Ti(t, d)49Ti Reaction: A comparison with magnetic electron scattering

NUCLEAR REACTIONS 48Ti(t, d), E=2.75, 3 MeV; 48Ti(t, t), E=2-3.5 MeV; 49Ti(d, d), E=4-5 MeV; measured σ(θ); deduced optical model parameters, normalization factor. 49Ti level deduced rms radius of 2p3/2 orbit. Optical model, DWBA analyses.

doi: 10.1016/0375-9474(81)90260-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1755.


1979WA17      Phys.Lett. 87B, 335 (1979)

A.Warwick, R.Chapman, J.L.Durell, J.N.Mo

Radii of Single-Proton States in Isotopes of Tin

NUCLEAR REACTIONS 112,116,118,120,124Sn(t, α), E=4.5-5.25 MeV; measured σ(Eα, θ); deduced rms radii of proton single-particle orbits.

doi: 10.1016/0370-2693(79)90548-3
Citations: PlumX Metrics


1979WA20      Phys.Lett. 88B, 55 (1979)

A.Warwick, R.Chapman, J.L.Durell, J.N.Mo, S.Sen

Proton Orbit Sizes and the Electric Monopole Matrix Element in 90Zr

NUCLEAR REACTIONS 90Zr(t, α), E=4.5, 4.75 MeV; measured σ(Eα, θ); deduced rms radii for 2p, 1g proton orbits, E0 matrix element, proton effective charge.

doi: 10.1016/0370-2693(79)90112-6
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter A.Warwick: , A.I.WARWICK