NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.E.Warner Found 100 matches. 2006WA18 Phys.Rev. C 74, 014605 (2006) R.E.Warner, F.Carstoiu, J.A.Brown, F.D.Becchetti, D.A.Roberts, B.Davids, A.Galonsky, R.M.Ronningen, M.Steiner, M.Horoi, J.J.Kolata, A.Nadasen, C.Samanta, J.Schwarzenberg, K.Subotic Reaction and proton-removal cross sections of 6Li, 7Be, 10B, 9, 10, 11C, 12N, 13, 15O, and 17Ne on Si at 15 to 53 MeV/nucleon NUCLEAR REACTIONS Si(6Li, X), (7Be, X), (10B, X), (9C, X), (10C, X), (11C, X), (12N, X), (13O, X), (15O, X), (17Ne, X), E=15-53 MeV/nucleon; measured reaction and proton-removal σ. 6Li, 7Be, 10B, 9,10,11C, 12N, 13,15O, 17Ne deduced radii. Comparison with Glauber model predictions.
doi: 10.1103/PhysRevC.74.014605
2004WA06 Phys.Rev. C 69, 024612 (2004) R.E.Warner, F.D.Becchetti, J.A.Brown, A.Galonsky, J.H.Kelley, A.Nadasen, R.M.Ronningen, J.A.Tostevin, J.S.Winfield, P.Zecher Proton removal from 8B, 9C, and 12C on Si at 20-70 MeV/nucleon NUCLEAR REACTIONS Si(8B, 7BeX), (9C, 8BX), (9C, 7BeX), (12C, 11BX), E=20-70 MeV/nucleon; measured one- and two-proton removal σ; deduced quenching factors. Shell model calculations, eikonal reaction theory.
doi: 10.1103/PhysRevC.69.024612
2002RO14 Phys.Rev. C65, 044605 (2002) D.A.Roberts, F.D.Becchetti, J.Janecke, M.Y.Lee, T.W.O'Donnell, K.Pham, J.A.Brown, R.E.Warner, R.M.Ronningen, H.W.Wilschut Energy Dependence of the Total Reaction Cross Section of Isomeric 18Fm on Silicon below 400 MeV NUCLEAR REACTIONS Si(18F, X), E < 400 MeV; measured reaction σ for metastable beam. Si(18F, X), (16O, X), (14N, X), E < 400 MeV; measured reaction σ. RADIOACTIVITY 18mF(IT) [from 12C(17O, 11B)]; measured Eγ, Iγ.
doi: 10.1103/PhysRevC.65.044605
2002WA04 Phys.Rev. C65, 034306 (2002) J.Wang, A.Galonsky, J.J.Kruse, E.Tryggestad, R.H.White-Stevens, P.D.Zecher, Y.Iwata, K.Ieki, A.Horvath, F.Deak, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, R.E.Warner, H.Schelin Dissociation of 6He NUCLEAR REACTIONS C, Al, Cu, Sn, Pb, U(6He, 2nα), (6He, αX), E=23.9 MeV/nucleon; measured Eα, En, nα-coin, parallel momentum distributions, angular correlations, two-neutron removal σ; deduced Coulomb contribution, other reaction mechanism features. 6He deduced halo neutron correlations. Comparisons with model predictions.
doi: 10.1103/PhysRevC.65.034306
2002WA08 Phys.Rev. C65, 044617 (2002) R.E.Warner, I.J.Thompson, J.A.Tostevin Effects of the In-Medium NN Interaction on Total Reaction and Neutron Removal Cross Sections NUCLEAR REACTIONS 12C(12C, X), E=10-1000 MeV/nucleon; 12C(6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), E=800 MeV/c; calculated total reaction σ; 12C(11Li, X), E=800 MeV/c; calculated two-neutron removal σ; deduced in-medium effects.
doi: 10.1103/PhysRevC.65.044617
2001WA40 Phys.Rev. C64, 044611 (2001) R.E.Warner, M.H.McKinnon, J.S.Needleman, N.C.Shaner, F.D.Becchetti, D.A.Roberts, A.Galonsky, R.M.Ronningen, M.Steiner, J.A.Brown, J.J.Kolata, A.Nadasen, K.Subotic Total Reaction and Neutron-Removal Cross Sections of (30-60)A MeV Be Isotopes on Si and Pb NUCLEAR REACTIONS Si(7Be, X), (9Be, X), (10Be, X), (11Be, X), (12Be, X), (14Be, X), Pb(10Be, X), (11Be, X), (12Be, X), E=30-60 MeV/nucleon; measured reaction σ, neutron-removal σ. 7,9,10,11,12,14Be deduced radii. Glauber model calculations.
doi: 10.1103/PhysRevC.64.044611
2000IN07 Nucl.Phys. A676, 3 (2000) A.Ingemarsson, J.Nyberg, P.U.Renberg, O.Sundberg, R.F.Carlson, A.J.Cox, A.Auce, R.Johansson, G.Tibell, D.T.Khoa, R.E.Warner New Results for Reaction Cross Sections of Intermediate Energy α-Particles on Targets from 9Be to 208Pb NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(α, X), E=69.6-192.4 MeV; measured reaction σ(θ), non-elastic σ(θ); deduced reduced interaction radius. Comparison with Optical model and Glauber model calculations. 58Ni(α, p), (α, 3He), (α, d), (α, t), E=80-160 MeV; calculated breakup σ(θ) from fragment spectra.
doi: 10.1016/S0375-9474(00)00200-1
2000IW05 Phys.Rev. C62, 064311 (2000) Y.Iwata, K.Ieki, A.Galonsky, J.J.Kruse, J.Wang, R.H.White-Stevens, E.Tryggestad, P.D.Zecher, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, R.E.Warner, H.Schelin Dissociation of 8He NUCLEAR REACTIONS Al(8He, n6He), Sn, Pb(8He, 2n6He), E=24 MeV/nucleon; measured invariant mass spectra, relative momentum distributions; deduced sequential decay contribution, dipole strength function, sum rules. 8He deduced excited state J, π, Γ. Secondary beam from 16O fragmentation.
doi: 10.1103/PhysRevC.62.064311
2000RA17 Phys.Rev. C62, 014607 (2000) K.A.G.Rao, A.Nadasen, D.Sisan, W.Yuhasz, D.Mercer, S.M.Austin, P.G.Roos, R.E.Warner 4He + 4He Elastic Scattering at 280 and 620 MeV NUCLEAR REACTIONS 4He(α, α), E=280, 620 MeV; measured σ(θ); deduced α-α interaction features. Optical model analysis, Woods-Saxon potential.
doi: 10.1103/PhysRevC.62.014607
2000WA23 Phys.Rev. C62, 024608 (2000) R.E.Warner, M.H.McKinnon, N.C.Shaner, F.D.Becchetti, A.Nadasen, D.A.Roberts, J.A.Brown, A.Galonsky, J.J.Kolata, R.M.Ronningen, M.Steiner, K.Subotic Total Reaction and Neutron-Removal Cross Sections of (30-60)A MeV He and Li Isotopes on Pb NUCLEAR REACTIONS Pb(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), E=30-60 MeV/nucleon; measured total σ. Pb(11Li, 9Li), (6He, α), (8He, α), (8He, 6He), E=30-60 MeV/nucleon; measured neutron-removal σ; deduced role of electromagnetic dissociation. Microscopic model calculations. Secondary beams from 18O fragmentation.
doi: 10.1103/PhysRevC.62.024608
1999NA05 Phys.Rev. C59, 760 (1999) A.Nadasen, J.Brusoe, J.Farhat, K.A.G.Rao, D.Sisan, J.Williams, P.G.Roos, F.Adimi, T.Gu, M.Khayat, R.E.Warner (α, 2α) Cluster Knockout Reaction on 9Be and 12C at 580 MeV NUCLEAR REACTIONS 9Be, 12C(α, 2α), E=580 MeV; measured σ(θ(1), θ(2), E); deduced dominance of quasifree knockout mechanism. DWIA calculations.
doi: 10.1103/PhysRevC.59.760
1999WA03 Phys.Rev. C59, 1215 (1999) R.E.Warner, M.H.McKinnon, H.Thirumurthy, A.Nadasen Trajectory-Modification and Correlation Effects on Light-Ion Total Reaction Cross Sections NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 60Ni, 124Sn, 208Pb(d, X), E=25-200 MeV; calculated reaction σ; deduced trajectory-modification, correlation effects.
doi: 10.1103/PhysRevC.59.1215
1998WA16 Nucl.Phys. A635, 292 (1998) R.E.Warner, H.Thirumurthy, J.Woodroffe, F.D.Becchetti, J.A.Brown, B.S.Davids, A.Galonsky, J.J.Kolata, J.J.Kruse, M.Y.Lee, A.Nadasen, T.W.O'Donnell, D.A.Roberts, R.M.Ronningen, C.Samanta, P.Schwandt, J.von Schwarzenberg, M.Steiner, K.Subotic, J.Wang, J.A.Zimmerman Reaction Cross Sections in Si of Light Proton-Halo Candidates 12N and 17Ne NUCLEAR REACTIONS Si(12N, X), (15O, X), (17Ne, X), E=29-53 MeV/nucleon; measured total reaction σ, charge-removal σ; deduced dependence on proton separation energy. Radioactive beams, Glauber model, proton-halo nuclei.
doi: 10.1016/S0375-9474(98)00163-8
1998YO09 Nucl.Phys. A641, 3 (1998) T.Yoshimura, A.Okihana, R.E.Warner, N.S.Chant, P.G.Roos, C.Samanta, S.Kakigi, N.Koori, M.Fujiwara, N.Matsuoka, K.Tamura, E.Kubo, K.Ushiro Alpha Spectroscopic Factors for 6Li, 7Li, 9Be and 12C from the (p(pol), pα) Reaction at 296 MeV NUCLEAR REACTIONS 6,7Li, 9Be, 12C(polarized p, pα), E=296 MeV; measured σ(θ(p), θ(α), Ep), Ay; deduced alpha spectroscopic factor. Projected energy spectrum, analyzing power distributions, quasifree scattering, distorted wave impulse approximation.
doi: 10.1016/S0375-9474(98)00432-1
1998ZE01 Phys.Rev. C57, 959 (1998) P.D.Zecher, A.Galonsky, S.J.Gaff, J.J.Kruse, G.Kunde, E.Tryggestad, J.Wang, R.E.Warner, D.J.Morrissey, K.Ieki, Y.Iwata, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, H.Schelin Measurement of the 8Li(n, γ)9Li Cross Section at Astrophysical Energies by Reverse Kinematics NUCLEAR REACTIONS U, Pb(9Li, n8Li), E=30 MeV/nucleon; measured σ. 8Li(n, γ), E=0.25, 0.75 MeV; deduced σ upper limit. Astrophysical implications discussed. Radioactive beam.
doi: 10.1103/PhysRevC.57.959
1997WA02 Phys.Rev. C55, 298 (1997) Nuclear and Coulomb Contributions to 6,8He + Si Dissociation Reactions at Low Energy NUCLEAR REACTIONS Si(6He, xn), (8He, xn), E=0-55 MeV/nucleon; 12C(8He, xn), (6He, xn), E=800 MeV/nucleon; calculated two-, four-neutron removal σ.
doi: 10.1103/PhysRevC.55.298
1997WA30 Phys.Rev. C56, 2694 (1997) Total Reaction Cross Sections for 20 to 100 MeV Deuterons from a Microscopic Model NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40,48Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(d, X), E=38, 65, 97 MeV; analyzed reaction σ; deduced Coulomb, nuclear effects, deuteron form factor dependence. Microscopic model calculations.
doi: 10.1103/PhysRevC.56.2694
1996GA08 Nucl.Phys. A599, 353c (1996) A.Galonsky, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.Orr, J.Ottarson, D.Sackett, B.M.Sherrill, J.Wang, J.Winger, P.Zecher, K.Ieki, Y.Iwata, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, H.Schelin, D.L.Humphrey Soft Dipole Resonance in Exotic Nuclei ( Question ) NUCLEAR REACTIONS Pb(11Li, X), E=30 MeV/nucleon; measured projectile three-body breakup energy spectrum, three-particle momenta; deduced no soft dipole resonance. 11Li deduced no dineutron. Virtual photon induced photodisintegration of 11Li.
doi: 10.1016/0375-9474(96)00078-4
1996IE01 Phys.Rev. C54, 1589 (1996) K.Ieki, A.Galonsky, D.Sackett, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Is There a Bound Dineutron in 11Li ( Question ) NUCLEAR REACTIONS 208Pb(11Li, 2n9Li), E=28 MeV/nucleon; measured 9Li(2n)-coin; deduced angular correlation between two neutrons in the rest frame of 11Li. 11Li level deduced no bound dineutron evidence.
doi: 10.1103/PhysRevC.54.1589
1996WA27 Phys.Rev. C54, 1700 (1996) R.E.Warner, R.A.Patty, P.M.Voyles, A.Nadasen, F.D.Becchetti, J.A.Brown, H.Esbensen, A.Galonsky, J.J.Kolata, J.Kruse, M.Y.Lee, R.M.Ronningen, P.Schwandt, J.von Schwarzenberg, B.M.Sherrill, K.Subotic, J.Wang, P.Zecher Total Reaction and 2n-Removal Cross Sections of 20-60A MeV 4,6,8He, 6-9,11Li, and 10Be on Si NUCLEAR REACTIONS, ICPND Si(6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), (10Be, X), (α, X), (6He, X), (8He, X), E=20-60 MeV/nucleon; measured reaction σ, 2n-removal σ for some projectiles. 4,6,8He, 6,7,8,9,11Li, 10Be deduced matter distributions. Microscopic, strong absorption optical models.
doi: 10.1103/PhysRevC.54.1700
1995BR05 Phys.Rev. C51, 1312 (1995) J.A.Brown, F.D.Becchetti, J.Janecke, D.A.Roberts, D.W.Litzenberg, T.W.O'Donnell, R.E.Warner, N.A.Orr, R.M.Ronningen Proton Scattering from an Excited Nucleus (18mF, J(π) = 5+, E(α) = 1.1 MeV) Using a γ-Ray-Tagged Secondary Isomeric Nuclear Beam NUCLEAR REACTIONS 18F(p, p), E(cm) ≈ 20 MeV; measured Eγ, Iγ, target in isomeric state, σ(θ). Secondary isomeric beam, γ-ray tagging.
doi: 10.1103/PhysRevC.51.1312
1995NA16 Phys.Rev. C52, 1894 (1995) A.Nadasen, J.Brusoe, J.Farhat, T.Stevens, J.Williams, L.Nieman, J.S.Winfield, R.E.Warner, F.D.Becchetti, J.W.Janecke, T.Annakkage, J.Bajema, D.Roberts, H.S.Govinden Unique Potentials for the Elastic Scattering of 350 MeV 7Li from 12C and 28Si NUCLEAR REACTIONS 12C, 28Si(7Li, 7Li), E=350 MeV; measured σ(θ); deduced optical model parameters. Double-folding calculations.
doi: 10.1103/PhysRevC.52.1894
1995RO14 Nucl.Phys. A588, 247c (1995) D.A.Roberts, F.D.Becchetti, J.A.Brown, J.Janecke, K.Pham, T.W.O'Donnell, R.E.Warner, R.M.Ronningen, H.W.Wilschut Unusual Energy Dependence of the Total Nuclear Reaction Cross Section for a Secondary Isomeric Nuclear Beam (18mF, Jπ = 5+, E(x) = 1.1 MeV) NUCLEAR REACTIONS Si(18F, X), E=22.3 MeV/nucleon; measured total reaction σ, projectile in ground, isomeric states; deduced unusual features for σ obtained from 18mF beam. Secondary 18,18mF beam from 12C(17O, 18F) reaction.
doi: 10.1016/0375-9474(95)00147-S
1995WA01 Phys.Rev. C51, 178 (1995) R.E.Warner, F.D.Becchetti, J.W.Janecke, D.A.Roberts, D.Butts, C.L.Carpenter, J.M.Fetter, A.Muthukrishnan, J.J.Kolata, K.Lamkin, M.Belbot, M.Zahar, A.Galonsky, K.Ieki, P.Zecher Elastic Scattering of 10 MeV 6He from 12C, (nat)Ni, and 197Au NUCLEAR REACTIONS 12C, Ni, 197Au(6He, 6He), E=10 MeV; measured σ(θ). Optical model analysis.
doi: 10.1103/PhysRevC.51.178
1995WA19 Phys.Rev. C52, R1166 (1995) R.E.Warner, J.H.Kelley, P.Zecher, F.D.Becchetti, J.A.Brown, C.L.Carpenter, A.Galonsky, J.Kruse, A.Muthukrishnan, A.Nadasen, R.M.Ronningen, P.Schwandt, B.M.Sherrill, J.Wang, J.S.Winfield Evidence for a Proton Halo in 8B: Enhanced total reaction cross sections at 20 to 60 MeV/nucleon NUCLEAR REACTIONS, ICPND Si(8B, X), (12C, X), (14N, X), E=20-60 MeV/nucleon; measured total reaction σ. 8B deduced proton halo. Si is both target and detector.
doi: 10.1103/PhysRevC.52.R1166
1994NA03 Phys.Rev. C49, 2258 (1994) A.Nadasen, J.Winfield, P.Schwandt, J.Farhat, L.Nieman, R.E.Warner, F.D.Becchetti, J.W.Janecke, N.Anantaraman Reply to ' Comment on ' Elastic Scattering of 318 MeV 6Li from 12C and 28Si: Unique phenomenological and folding-model potentials ' and the validity of the M3Y effective interaction ' NUCLEAR REACTIONS 12C(6Li, 6Li), E=35, 53 MeV/nucleon; analyzed σ(θ) analyses; deduced renormalization related features in folding model with M3Y interaction.
doi: 10.1103/PhysRevC.49.2258
1994WA06 Phys.Rev. C49, 1534 (1994) R.E.Warner, J.M.Fetter, R.A.Swartz, A.Okihana, T.Konishi, T.Yoshimura, P.D.Kunz, M.Fujiwara, K.Fukunaga, S.Kakigi, T.Hayashi, J.Kasagi, N.Koori 4He(4He, 3He)5He(g.s.) Reaction at 118 MeV, and Its Distorted Wave Born Approximation Interpretation NUCLEAR REACTIONS 4He(α, 3He), E=118 MeV; measured σ(θ); deduced model parameters. DWBA analysis.
doi: 10.1103/PhysRevC.49.1534
1993AY01 Nucl.Phys. A562, 1 (1993) Z.Ayer, S.E.Darden, S.Sen, R.E.Warner Spin Polarization Effects in the 3He(d, 3Hep)n and the 3He(d, tp)p Reactions at E(d) = 17 MeV NUCLEAR REACTIONS 3He(polarized d, p3He), (polarized d, pt), E=17 MeV; measured σ(θp, θ(3He)), σ(θp, θt) vs E(particle), vector, tensor analyzing power vs θ. Plane wave, distorted wave impulse approximation calculations.
doi: 10.1016/0375-9474(93)90029-W
1993BE22 Phys.Rev. C48, 308 (1993) F.D.Becchetti, W.Z.Liu, K.Ashktorab, J.F.Bajema, J.A.Brown, J.W.Janecke, D.A.Roberts, J.J.Kolata, K.L.Lamkin, A.Morsad, R.J.Smith, X.J.Kong, R.E.Warner Systematics of 8Li-Induced Radioactive Beam Reactions: E = 13-20 MeV NUCLEAR REACTIONS 2H, 9Be, 13,12C, 14N, 27Al, 58Ni(8Li, 7Li), (8Li, 8Li), E ≈ 13-20 MeV; 9Be, 12C(8Li, α), E ≈ 13-20 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.48.308
1993IE01 Phys.Rev.Lett. 70, 730 (1993) K.Ieki, D.Sackett, A.Galonsky, C.A.Bertulani, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, H.Schulz, B.M.Sherrill, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Coulomb Dissociation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured nn-correlation following projectile dissociation; deduced dissociation mechanism.
doi: 10.1103/PhysRevLett.70.730
1993NA01 Phys.Rev. C47, 674 (1993) A.Nadasen, T.Stevens, J.Farhat, J.Brusoe, P.Schwandt, J.S.Winfield, G.Yoo, N.Anantaraman, F.D.Becchetti, D.Brown, D.Hotz, J.W.Janecke, D.Roberts, R.E.Warner Elastic Scattering of 318 MeV 6Li from 12C and 28Si: Unique phenomenological and folding-model potentials NUCLEAR REACTIONS 12C, 28Si(6Li, 6Li), E=318 MeV; measured σ(θ). Phenomenological, folding model potentials interpretation.
doi: 10.1103/PhysRevC.47.674
1993SA21 Phys.Rev. C48, 118 (1993) D.Sackett, K.Ieki, A.Galonsky, C.A.Bertulani, H.Esbensen, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, H.Schulz, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Electromagnetic Excitation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured 9Li(n)-, γ(9Li)-coin following 11Li Coulomb dissociation; deduced dissociation σ, photonuclear σ(E1), breakup mechanism.
doi: 10.1103/PhysRevC.48.118
1993WA12 Phys.Rev. C48, 245 (1993) R.E.Warner, C.L.Carpenter, J.M.Fetter, W.F.Waite, H.W.Wilschut, J.M.Hoogduin Total Nuclear Reaction Probability of 270 to 390 MeV 14N Ions in Si and CsI NUCLEAR REACTIONS I, Cs(14N, X), E=265, 385 MeV; I, Cs(α, X), E=116 MeV; Si(14N, X), E=271, 390 MeV; measured total reaction probability; deduced average reaction σ. Optical, strong absorption model predictions comparison.
doi: 10.1103/PhysRevC.48.245
1992BE46 Nucl.Phys. A550, 507 (1992) F.D.Becchetti, J.A.Brown, W.Z.Liu, J.W.Janecke, D.A.Roberts, J.J.Kolata, R.J.Smith, K.Lamkin, A.Morsad, R.E.Warner, R.N.Boyd, J.D.Kalen Reaction Rates for 8Li(p, α) and 8Li(p, n, α) and Their Effect on Primordial Nucleosynthesis NUCLEAR REACTIONS 1H(8Li, α), E(cm)=1.5 MeV; measured σ(Eα), σ(θ); deduced 8Li destruction thermonuclear reaction rate, p+8Li total reaction rate. Radioactive beam.
doi: 10.1016/0375-9474(92)90020-K
1992OK01 Nucl.Phys. A549, 1 (1992) A.Okihana, T.Konishi, R.E.Warner, D.Francis, M.Fujiwara, N.Matsuoka, K.Fukunaga, S.Kakigi, T.Hayashi, J.Kasagi, N.Koori, M.Tosaki, M.Greenfield Quasifree Scattering in the 6Li(α, 2α)2H Reaction at E(α) between 77 and 119 MeV NUCLEAR REACTIONS 6Li(α, 2α), E=77-119 MeV; measured σ(θα1, θα2, Eα1). 6Li deduced dα-breakup spectroscopic factor. Projected energy spectrum, quasifree scattering, distorted wave impulse approxiation.
doi: 10.1016/0375-9474(92)90064-Q
1992WA09 Phys.Rev. C45, 2328 (1992) R.E.Warner, A.Okihana, M.Fujiwara, N.Matsuoka, S.Kakigi, S.Hayashi, K.Fukunaga, J.Kasagi, M.Tosaki 7Li(α, 2α)3H Reaction from 77 to 119 MeV NUCLEAR REACTIONS 7Li(α, 2α), E=77-119 MeV; measured absolute σ(θ1, θ2, E1); deduced reaction mechanism. 7Li deduced triton momentum distribution.
doi: 10.1103/PhysRevC.45.2328
1992WA13 Nucl.Instrum.Methods Phys.Res. A314, 113 (1992) R.E.Warner, R.J.Orr, W.F.Waite, C.P.Browne, S.E.Darden, A.Rollefson, J.J.Kolata, L.Van Wormer, A.Galonsky, D.Sackett, F.D.Becchetti Measurement of the 6Li + (nat)Si Reaction Cross Section at 18 to 28 MeV with a Magnetic Spectrograph and Position-Sensitive Si Detector NUCLEAR REACTIONS, ICPND Si(6Li, X), E=18-28 MeV; measured average reaction σ. Two-dimensional position-sensitive Si detector in magnetic spectrograph focal plane.
doi: 10.1016/0168-9002(92)90503-V
1992WA18 Phys.Rev. C46, 616 (1992) R.E.Warner, A.Okihana, M.Fujiwara, N.Matsuoka, S.Hayashi, S.Kakigi, K.Fukunaga, J.Kasagi, M.Tosaki, M.B.Greenfield Energy Dependence of the 6Li(α, 2α)pn Reaction from 77 to 119 MeV NUCLEAR REACTIONS 6Li(α, 2α), E=77-119 MeV; measured σ(θ1, θ2, E1, E2); deduced reaction mechanism, spectral functions.
doi: 10.1103/PhysRevC.46.616
1991BE49 Nucl.Instrum.Methods Phys.Res. B56/57, 554 (1991) F.D.Becchetti, J.A.Brown, K.Ashktorab, J.W.Janecke, W.Z.Liu, D.A.Roberts, R.J.Smith, J.J.Kolata, K.Lamkin, A.Morsad, R.E.Warner Production and Use of 6He, 7Be, 8Li, 12B and Metastable Nuclear Beams NUCLEAR REACTIONS 9Be(7Li, 8Li), (7Li, α), (7Li, 6He), E=17 MeV; 1H(10B, 7Be), E=23.5 MeV; 9Be(7Li, 6He), E=14.63 MeV; 1H(10B, 7Be), E=23.5 MeV; 12C(3He, 7Be), E=22.5 MeV; 10B(6Li, 7Be), E=23 MeV; 12C(17O, 18F), E=70 MeV; measured secondary beam production yields. 197Au, C, Ni(8Li, 8Li), (8Li, 8Li'), E=13.8-14.9 MeV; measured σ(E(8Li)). 197Au, Ti, 2H, 27Al, C, 9Be(6He, 6He), E=8.8-9.3 MeV; measured σ(θ). Other reactions discussed.
doi: 10.1016/0168-583X(91)96094-2
1991BR14 Phys.Rev.Lett. 66, 2452 (1991) J.A.Brown, F.D.Becchetti, J.W.Janecke, K.Ashktorab, D.A.Roberts, J.J.Kolata, R.J.Smith, K.Lamkin, R.E.Warner Coulomb Excitation of 8Li NUCLEAR REACTIONS Ni(8Li, 8Li'), (8Li, 8Li), E ≈ 14.6 MeV; measured σ(θ) following Coulomb excittion. 8Li deduced level excitation probability, B(E2).
doi: 10.1103/PhysRevLett.66.2452
1991SM02 Phys.Rev. C43, 2346 (1991) R.J.Smith, J.J.Kolata, K.Lamkin, A.Morsad, F.D.Becchetti, J.A.Brown, W.Z.Liu, J.W.Janecke, D.A.Roberts, R.E.Warner Elastic and Inelastic Scattering of 8Li from 12C NUCLEAR REACTIONS C, 197Au(8Li, 8Li), (8Li, 8Li'), E=14 MeV; measured σ(θ); deduced model parameters. 8Li level deduced B(E2).
doi: 10.1103/PhysRevC.43.2346
1991WA03 Phys.Rev. C43, 1313 (1991) R.E.Warner, H.W.Wilschut, W.F.Rulla, G.N.Felder Average Reaction Cross Sections for 74- to 112-MeV α Particles on 127I and 133Cs NUCLEAR REACTIONS, ICPND 127I, 133Cs(α, α), E=84, 100, 120 MeV; measured average reaction σ. Magnetic spectrograph, CSI scintillation detector.
doi: 10.1103/PhysRevC.43.1313
1990BE31 Phys.Rev. C42, R801 (1990) F.D.Becchetti, K.Ashktorab, J.A.Brown, J.W.Janecke, D.A.Roberts, J.van Klinken, W.Z.Liu, J.J.Kolata, K.Lamkin, R.J.Smith, R.E.Warner Production of an Isomeric, Excited Radioactive Nuclear Beam NUCLEAR REACTIONS 12C(17O, 18F), E=50-80 MeV; measured σ, production rate of 18mF.
doi: 10.1103/PhysRevC.42.R801
1990WA12 Nucl.Phys. A516, 416 (1990) R.E.Warner, K.M.Berland, W.F.Rulla, D.A.Francis, J.J.Kolata, Z.Ayer, S.E.Darden, X.J.Kong, G.Liu, A.Morsad, S.McGimpsey, A.A.Rollefson, A.Galonsky, A.Nadasen, J.S.Winfield, F.D.Becchetti Total Nuclear Reaction Probabilities and Average Cross Sections for 16 to 23 MeV 6Li in Silicon NUCLEAR REACTIONS, ICPND Si(6Li, X), E=15.6, 20.3, 23 MeV; measured reaction probabilities, energy averaged total reaction σ.
doi: 10.1016/0375-9474(90)90316-E
1990WA17 Phys.Rev. C42, 2143 (1990) R.E.Warner, E.Cheung, C.F.Perdrisat, V.Punjabi, C.A.Davis, R.Helmer, A.Galonsky, L.Heilbronn, D.Krofcheck, S.E.Darden, J.J.Kolata, F.D.Becchetti, P.Schwandt Spectral Function of p-n Pairs in 6Li, from the 6Li(p, pα)pn Reaction at 200 MeV NUCLEAR REACTIONS 6Li(polarized p, pα), E=200 MeV; measured σ(θp, θα, Ep, Eα) vs (pn)-internal momentum. 6Li deduced dα-cluster probability.
doi: 10.1103/PhysRevC.42.2143
1990WA18 Phys.Rev. C42, 2252 (1990) Microscopic Calculations of Low-Energy Reaction Cross Sections NUCLEAR REACTIONS Ge, Si(d, X), Si(3He, X), (α, X), E=2-53 MeV/nucleon; calculated reaction σ, probabilities. Microscopic calculations.
doi: 10.1103/PhysRevC.42.2252
1989BE28 Phys.Rev. C40, R1104 (1989) F.D.Becchetti, W.Z.Liu, D.A.Roberts, J.W.Janecke, J.J.Kolata, A.Morsad, X.J.Kong, R.E.Warner Measurements of Discrete Nuclear Reactions Induced by a Radioactive 8Li Beam NUCLEAR REACTIONS 12C, 9Be(8Li, 7Li), E=13 MeV; measured σ(θ), σ(E(7Li)); deduced astrophysical abundance implications.
doi: 10.1103/PhysRevC.40.R1104
1989KO17 Nucl.Instrum.Methods Phys.Res. B40/41, 503 (1989) J.J.Kolata, A.Morsad, X.J.Kong, R.E.Warner, F.D.Becchetti, W.Z.Liu, D.A.Roberts, J.W.Janecke A Radioactive Beam Facility Using a Large Superconducting Solenoid NUCLEAR REACTIONS 9Be(8Li, 7Li), E=11 MeV; measured residuals spectra, σ(θ). 9Be, 197Au(8Li, 8Li), E=not given; measured σ(θ).
doi: 10.1016/0168-583X(89)91032-X
1989NA02 Phys.Rev. C39, 536 (1989) A.Nadasen, M.McMaster, M.Fingal, J.Tavormina, P.Schwandt, J.S.Winfield, M.F.Mohar, F.D.Becchetti, J.W.Janecke, R.E.Warner Unique 6Li-Nucleus Optical Potentials from Elastic Scattering of 210 MeV 6Li Ions by 28Si, 40Ca, 90Zr, and 208Pb NUCLEAR REACTIONS 28Si, 40Ca, 90Zr, 208Pb(6Li, 6Li), E=210 MeV; measured σ(θ); deduced optical model parameters, target mass and energy dependence.
doi: 10.1103/PhysRevC.39.536
1989NA11 Phys.Rev. C40, 1237 (1989) A.Nadasen, M.McMaster, M.Fingal, J.Tavormina, J.S.Winfield, R.M.Ronningen, P.Schwandt, F.D.Becchetti, J.W.Janecke, R.E.Warner Inelastic Scattering of 210 MeV 6Li Ions from 12C, 28Si, and 58Ni: Test of unique 6Li potentials NUCLEAR REACTIONS 12C, 28Si, 58Ni(6Li, 6Li'), E=210 MeV; measured σ(θ). 12C, 28Si, 58Ni level deduced deformation length, quadrupole moments. DWBA, coupled-channels analyses.
doi: 10.1103/PhysRevC.40.1237
1989WA26 Nucl.Phys. A503, 161 (1989) R.E.Warner, A.Okihana, M.Fujiwara, N.Matsuoka, K.Tamura, M.Tosaki, T.Ohsawa, K.Fukunaga, S.Kakigi, J.Kasagi, N.Koori Joint Momentum Distribution of p + n in 6Li NUCLEAR REACTIONS 6Li(α, 2α), E=118 MeV; measured σ(θ1, θ2, E1, E2); deduced p+n joint momentum distribution in 6Li. Enriched target. PWIA analysis.
doi: 10.1016/0375-9474(89)90259-5
1989WA27 Phys.Rev. C40, 2473 (1989) R.E.Warner, A.M.van den Berg, K.M.Berland, J.D.Hinnefeld, Z.Zhang, Y.T.Zhu, X.Q.Hu, S.Li Total Nuclear Reaction Probabilities and Average Cross Sections for 27 to 92 MeV α particles in Silicon NUCLEAR REACTIONS, ICPND Si(α, X), E=27-92 MeV; measured average reaction σ(E), energy integrated reaction probabilities. Optical model analysis.
doi: 10.1103/PhysRevC.40.2473
1988NA02 Phys.Rev. C37, 132 (1988) A.Nadasen, M.McMaster, G.Gunderson, A.Judd, S.Villanueva, P.Schwandt, J.S.Winfield, J.van der Plicht, R.E.Warner, F.D.Becchetti, J.W.Janecke Elastic Scattering of 210 MeV 6Li Ions from 12C and 58Ni and Unique 6Li-Nucleus Optical Potentials NUCLEAR REACTIONS 12C, 58Ni(6Li, 6Li), E=210 MeV; measured σ(θ); deduced unique potentials energy dependence. Optical model.
doi: 10.1103/PhysRevC.37.132
1988WA09 Phys.Rev. C37, 1884 (1988) R.E.Warner, C.P.Browne, S.E.Darden, J.J.Kolata, A.Rollefson, P.A.Kimoto, A.Galonsky Total Nuclear Reaction Probabilities for 2 to 6 MeV/Nucleon d and 3He in Si NUCLEAR REACTIONS Si(d, X), E=4-13 MeV; Si(3He, X), E=5-18 MeV; measured energy integrated, energy averaged total reaction σ. Optical model comparison.
doi: 10.1103/PhysRevC.37.1884
1988WA29 Phys.Rev. C38, 2945 (1988) R.E.Warner, A.Okihana, M.Fujiwara, N.Matsuoka, K.Tamura, M.Tosaki, T.Ohsawa, K.Fukunaga, P.A.Kimoto, N.Koori Spectral Function of the p3/2 Nucleons in 6Li NUCLEAR REACTIONS 6Li(α, 2α), E=118 MeV; measured (p+n) spectral function. Plane wave impulse approximation. Enriched target.
doi: 10.1103/PhysRevC.38.2945
1987WA21 Nucl.Phys. A470, 339 (1987) R.E.Warner, B.A.Vaughan, J.A.Ditusa, J.W.Rovine, R.S.Wakeland, C.P.Browne, S.E.Darden, S.Sen, A.Nadasen, A.Basak, T.R.Donoghue, T.Rinckel, K.Sale, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster The Mechanism of the 7Li(d, 2α)n Reaction from E(d) = 3 to 15 MeV NUCLEAR REACTIONS, MECPD 7Li(d, 2α), E=3-15 MeV; measured σ(θ1, θ2) vs energy difference; deduced reaction mechanism. 8Be deduced levels. Enriched 7LiF targets.
doi: 10.1016/0375-9474(87)90006-6
1987WA25 Nucl.Phys. A472, 522 (1987) R.E.Warner, F.G.Johnson, C.P.Browne, A.Rollefson, A.Galonsky, A.Nadasen The 9Be(3He, 2α)α Reaction from 12 to 24 MeV and Coherent Sequential Decay NUCLEAR REACTIONS, MECPD 9Be(3He, 2α), E=12-24 MeV; measured σ(E1, θ1, θ2). 8Be deduced level α-decay mechanism. 9Be deduced cluster characteristics.
doi: 10.1016/0375-9474(87)90043-1
1986WA11 Nucl.Phys. A453, 605 (1986) R.E.Warner, B.A.Vaughan, D.L.Friesel, P.Schwandt, J.-Q.Yang, G.Caskey, A.Galonsky, B.Remington, A.Nadasen The Noncoplanar 7Li(p, pd)5He and 7Li(p, pt)4He Reactions at E(p)=200 MeV, and Evidence for Deuteron Clustering in 7Li NUCLEAR REACTIONS 7Li(p, pd), (p, pt), E=200 MeV; measured σ(Ed, θp, θd, φ), σ(Ep, θp, θt, φ); deduced optical model parameters, d+5He momentum distribution width. 7Li deduced deuteron spectroscopic factors. Enriched target, Ge detectors. DWIA calculations.
doi: 10.1016/0375-9474(86)90254-X
1985WA13 Phys.Rev. C31, 1662 (1985) C.W.Wang, P.G.Roos, N.S.Chant, G.Ciangaru, F.Khazaie, D.J.Mack, A.Nadasen, S.J.Mills, R.E.Warner, E.Norbeck, F.D.Becchetti, J.W.Janecke, P.M.Lister 9Be(p, pα)5He Cluster Knockout Reaction with 150 MeV Polarized Protons NUCLEAR REACTIONS 9Be(polarized p, pα), E=150 MeV; measured quasifree σ(θ), analyzing power vs θ, σ(θp, Ep), energy sharing σ; deduced optical potentials parameters. 9Be deduced Sα for cluster breakup. DWIA, cluster knockout.
doi: 10.1103/PhysRevC.31.1662
1985WA25 Nucl.Phys. A443, 64 (1985) R.E.Warner, J.-Q.Yang, D.L.Friesel, P.Schwandt, G.Caskey, A.Galonsky, B.Remington, A.Nadasen, N.S.Chant, F.Khazaie, C.Wang Comparison of the Noncoplanar 6Li(p, pd)4He Reactions at 120 and 200 MeV NUCLEAR REACTIONS 6Li(p, pd), E=200.2 MeV; measured σ(E(d), θ(p), θ(d), φ); deduced potentials. 6Li level deduced spectroscopic factor. Enriched target, Ge detectors.
doi: 10.1016/0375-9474(85)90321-5
1984WA09 Nucl.Phys. A422, 205 (1984) R.E.Warner, R.S.Wakeland, J.-Q.Yang, D.L.Friesel, P.Schwandt, G.Caskey, A.Galonsky, B.Remington, A.Nadasen The Noncoplanar 6Li(p, pd)4He Reaction at 120 MeV, and the 6Li Cluster Momentum Wave Function NUCLEAR REACTIONS 6Li(p, pd), E=119.6 MeV; measured σ(Ed, θd, Ep, φ); deduced reaction mechanism. 6Li deduced α-d cluster spectroscopic factor, momentum distribution. Enriched target. DWIA calculations.
doi: 10.1016/0375-9474(84)90514-1
1983DO07 Phys.Rev. C28, 875 (1983) T.R.Donoghue, E.Sugarbaker, M.Wiescher, T.C.Rinckel, K.E.Sale, C.P.Browne, E.D.Berners, R.W.Tarara, R.E.Warner Measurement of the Electron Capture Branching Ratio of 7Be NUCLEAR REACTIONS 10B(p, α), E=1.5, 4.5 MeV; measured σ(E(7Be)). RADIOACTIVITY 7Be(EC) [from 10B(p, α), E=1.5, 4.5 MeV]; measured Eγ, Iγ. 7Li level deduced EC-branching ratio.
doi: 10.1103/PhysRevC.28.875
1983WA09 Nucl.Phys. A401, 521 (1983) R.E.Warner, K.Blum, D.Friesel, P.Schwandt, P.P.Singh, A.Galonsky Multibody Final States of the 6Li + 6Li Reaction at 97 MeV NUCLEAR REACTIONS 6Li(6Li, 2α), 6Li(6Li, 2d), E=97.5 MeV; measured σ(θ1, θ2, E1, E2) for two-, three-α breakup; deduced reaction mechanisms. Single, double spectator pole models.
doi: 10.1016/0375-9474(83)90363-9
1982BE33 Phys.Rev. C26, 720 (1982) K.B.Beard, J.Kasagi, E.Kashy, B.H.Wildenthal, D.L.Freisel, H.Nann, R.E.Warner (d, 2He) Reaction at E(d) = 99 MeV NUCLEAR REACTIONS 12C(d, 2p), E=99.2 MeV; measured σ(E(2He)), σ(θ). Sum, difference spectra, Watson-Migdal final state interaction.
doi: 10.1103/PhysRevC.26.720
1982LY01 Phys.Lett. 108B, 274 (1982) W.G.Lynch, L.W.Richardson, M.B.Tsang, R.E.Ellis, C.K.Gelbke, R.E.Warner In-Plane Correlations between Protons and Deuterons for 16O-Induced Reactions on 27Al and 197Au at 310 MeV NUCLEAR REACTIONS 27Al, 197Au(16O, p), (16O, 2p), (16O, pd), E=310 MeV; measured σ(θp, Ep), (particle)(particle)(θ); deduced kinematic correlation role. Moving source, isotropic particle emission model.
doi: 10.1016/0370-2693(82)91191-1
1982WA07 Nucl.Phys. A379, 191 (1982) Extended PWBA Treatment of the 6Li + 6Li → 2α + 2d Reaction NUCLEAR REACTIONS 6Li(6Li, 2α), (6Li, 2d), E=36-47 MeV; calculated σ(θ1, θ2, E1, E2). Extended PWBA model.
doi: 10.1016/0375-9474(82)90563-2
1981CU10 Can.J.Phys. 59, 1233 (1981) B.Cujec, A.J.Ferguson, O.Hausser, D.Horn, R.E.Warner Cross Sections for the 16O(16O, 8Be(g.s.))24Mg Reaction and Mechanisms of α-Rearrangement Reactions NUCLEAR REACTIONS 16O(16O, 8Be), E=53 MeV; measured 24Mg(α)-coin; deduced reaction mechanism. ΔE-E heavy-ion telescope.
1981WA15 Nucl.Phys. A365, 142 (1981) R.E.Warner, G.C.Ball, W.G.Davies, J.S.Forster Double Spectator Poles Observed in a Double Coincidence Study of the 6Li + 6Li → 2α + 2d Reaction NUCLEAR REACTIONS 6Li(6Li, 2α), (6Li, 2d), E=36-47 MeV; measured σ(θ1, θ2, E1, E2); deduced reaction mechanisms. Isotopic target.
doi: 10.1016/0375-9474(81)90392-4
1981WA29 Phys.Rev. C24, 2759 (1981) Reinterpretation of the 2H(d, pp)nn Reaction at 80 MeV NUCLEAR REACTIONS 2H(d, 2p), E=80 MeV; calculated σ(E1, E2, θ1, θ2). Neutron, proton final state interactions.
doi: 10.1103/PhysRevC.24.2759
1980RE03 Nucl.Sci.Eng. 75, 140 (1980) P.L.Reeder, L.J.Alquist, R.L.Kiefer, F.H.Ruddy, R.E.Warner Energy Spectra of Delayed Neutrons from the Separated Precursors Rubidium-93, -94, -95, and Cesium-143 RADIOACTIVITY 93,94,95Rb, 143Cs [from on-line mass separation]; measured β-delayed E(n). Helium-3 spectrometer.
doi: 10.13182/NSE80-A21303
1980WA10 Nucl.Phys. A341, 483 (1980) R.E.Warner, W.T.Conner, G.C.Ball, W.G.Davies, A.J.Ferguson Mechanism of the 6Li(6Li, 2α)α Reaction from 36 to 46 MeV NUCLEAR REACTIONS 6Li(6Li, 2α), E=36-46 MeV; measured αα-coin, σ(Eα1, Eα2); deduced reaction mechanism. 8Be deduced levels. Isotopic target.
doi: 10.1016/0375-9474(80)90379-6
1979WA02 Phys.Rev. C19, 293 (1979) R.E.Warner, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Search for αα* Rotational Levels in 8Be NUCLEAR REACTIONS 2H(6Li, α), E=10-31 MeV; measured σ(θ). 8Be deduced evidence for rotational band around 24-28 MeV excitation.
doi: 10.1103/PhysRevC.19.293
1979WA13 Nucl.Phys. A326, 209 (1979) R.E.Warner, D.C.Martin, G.C.Ball, W.G.Davies, A.J.Ferguson, D.Horn Double Spectator Poles and Quasi-Free Inelastic Scattering in the 6Li + 6Li → 2α + 2d Reaction NUCLEAR REACTIONS 6Li(6Li, d2α), (6Li, 2dα), E=45 MeV; observed triple coin energy spectra; deduced reaction mechanism. Isotopic target.
doi: 10.1016/0375-9474(79)90376-2
1977DA11 Phys.Rev.Lett. 38, 1119 (1977) W.G.Davies, G.C.Ball, A.J.Ferguson, J.S.Forster, D.Horn, R.E.Warner Search for High-Energy Deuterons in the 3He + 3He Reaction and the Solar Neutrino Problem NUCLEAR REACTIONS 3He(3He, d), E=15, 25 MeV; measured σ for production of high energy deuterons; deduced upper, lower σ limits.
doi: 10.1103/PhysRevLett.38.1119
1976DA18 Nucl.Phys. A269, 477 (1976) W.G.Davies, R.M.DeVries, G.C.Ball, J.S.Forster, W.McLatchie, D.Shapira, J.Toke, R.E.Warner A Comparison of α-Transfer and α-Decay in the Lead Region NUCLEAR REACTIONS 204,207,208Pb, 209Bi(16O, 12C), E=93 MeV; measured σ(θ). 208,211,212Po, 213At levels deduced S, Γα. DWBA analysis, resolution 200 keV, θ=60-104°.
doi: 10.1016/0375-9474(76)90694-1
1976WA12 Nucl.Phys. A269, 286 (1976) R.E.Warner, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Three-Body Final States of the 3He + 7Li Reaction and Clustering in 7Li NUCLEAR REACTIONS 7Li(3He, t3He), (3He, d3He), (3He, t6Li), (3He, 3He6Li), 7Li(3He, 3He6He), E=37.5 MeV; measured absolute coin σ(E1, θ1, θ2). Enriched target. Modified PWBA analysis. Cluster probabilities, momentum distributions.
doi: 10.1016/0375-9474(76)90681-3
1975WA09 Nucl.Phys. A243, 189 (1975) R.E.Warner, S.B.Di Cenzo, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Final-State Interactions in the 2H(d, pp)nn Reaction NUCLEAR REACTIONS 2H(d, 2p), E=23.15 MeV; measured absolute σ(θ), pp-coin; deduced 2n, 2p relative energy spectra. Watson-Migdal, double distorted wave analysis. Enriched target.
doi: 10.1016/0375-9474(75)90243-2
1975WA31 Nucl.Phys. A255, 95 (1975) R.E.Warner, R.L.Ruyle, W.G.Davies, G.C.Ball, A.J.Ferguson, J.S.Forster Initial-State Distortion and Final-State Interactions in the 2H(3He, 3He p)n and 2H(3He, 3H p)p Reactions NUCLEAR REACTIONS 2H(3He, p3He), (3He, pt), E=35.9 MeV; measured absolute coin σ(E1, θ1, θ2). Enriched target. Antisymmetrized DWBA, PWBA-FSI analysis of present, previous 26.8, 35.9 MeV data for same reactions.
doi: 10.1016/0375-9474(75)90150-5
1974HA34 Nucl.Phys. A225, 425 (1974) O.Hausser, D.B.Fossan, A.Olin, D.Ward, W.Witthuhn, R.E.Warner The l-Forbidden 3p3/2 → 2f5/2 M1 Transition in 207Pb NUCLEAR REACTIONS 207Pb(α, α'γ), E=15 MeV; measured Eγ, Iγ, γγ-coin. 207Pb level deduced γ-branching, B(M1).
doi: 10.1016/0375-9474(74)90350-9
1974WA06 Nucl.Phys. A221, 593 (1974) R.E.Warner, S.A.Gottlieb, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Effects of Exchange and Final-State Interactions in the Reactions 2H(3He, 3H p)p and 2H(3He, 3He p)n NUCLEAR REACTIONS 2H(3He, 3Hep), (3He, pt), E=35.9 MeV; measured absolute coin σ(E1, θ(1), θ(2)). Enriched target.
doi: 10.1016/0375-9474(74)90485-0
1973HA47 Nucl.Phys. A212, 613 (1973) O.Hausser, A.B.McDonald, T.K.Alexander, A.J.Ferguson, R.E.Warner E1 Polarization in Coulomb Excitation of 7Li NUCLEAR REACTIONS 208Pb(7Li, 7Li'γ), E=18-30 MeV; measured σ(E;E(7Li)', Eγ, θ). 7Li levels deduced E1 interference effects, B(E2); enriched targets.
doi: 10.1016/0375-9474(73)90826-9
1973RA09 Phys.Lett. 44B, 36 (1973) W.L.Randolph, N.Ayres de Campos, J.R.Beene, J.Burde, M.A.Grace, D.F.H.Start, R.E.Warner A Time-Differential Measurement of the Hyperfine Structure of the 6.13 MeV State in Highly Ionized 16O Atoms NUCLEAR REACTIONS 1H(19F, αγ), E=49 MeV; measured αγ(t). 16O level deduced g.
doi: 10.1016/0370-2693(73)90293-1
1973ST08 Nucl.Phys. A206, 207 (1973) D.F.H.Start, N.A.Jelley, J.Burde, D.A.Hutcheon, W.L.Randolph, B.Y.Underwood, R.E.Warner Gamma-Ray Transitions from the Lowest T = 2 States of 24Na and 28Al NUCLEAR REACTIONS 22Ne(3He, pγ), E=9.0 MeV; 26Mg(3He, pγ), E=8.0 MeV; measured σ(E;Eγ, θ(pγ)). 24Na, 28Al deduced levels, branching ratios, T. Enriched targets.
doi: 10.1016/0375-9474(73)90617-9
1973WA13 Nucl.Phys. A204, 433 (1973) Effects of Exchange, Final-State Interactions, and Distorted Waves in the Reactions 2H(3He, 3H p)p and 2H(3He, 3He p)n NUCLEAR REACTIONS 2H(3He, tp), (3He, 3Hep); analyzed σ(Et), σ(E(3He)).
doi: 10.1016/0375-9474(73)90386-2
1972HA06 Phys.Lett. 38B, 75 (1972) O.Hausser, A.B.McDonald, T.K.Alexander, A.J.Ferguson, R.E.Warner Nuclear Polarizability of 7Li from Coulomb Excitation NUCLEAR REACTIONS 208Pb(7Li, 7Li), 208Pb(7Li, Xγ), E=18-30 MeV; measured σ(E;θ), σ(E;Eγ, θ). 7Li deduced nuclear polarizability.
doi: 10.1016/0370-2693(72)90743-5
1972WA22 Nucl.Phys. A192, 341 (1972) R.E.Warner, G.R.Flierl, W.G.Davies, G.C.Ball, A.J.Ferguson, J.S.Forster, S.A.Gottlieb Coincidence Study and DWBA Analysis of the 3He+d → d+d+p Reaction NUCLEAR REACTIONS 2H(3He, dd)p, 2H(3He, dp)d, E=26.8 MeV; measured absolute coin σ(E1, θ(1), θ(2)); deduced reaction mechanisms. Enriched target.
doi: 10.1016/0375-9474(72)90264-3
1971CH55 Nucl.Phys. A178, 39 (1971) L.A.Charlton, S.M.Kelso, R.E.Warner A DWBA Treatment of the Reaction 3He(d, tp)p NUCLEAR REACTIONS 3He(d, tp), E < 12 MeV; calculated σ(E). DWBA.
doi: 10.1016/0375-9474(71)90183-7
1971CO26 Nucl.Phys. A174, 468 (1971) B.E.Corey, R.E.Warner, R.W.Bercaw Coincidence Study of the Reaction 2H(d, dp)n NUCLEAR REACTIONS 2H(d, dp), E=20.7 MeV; measured absolute coin σ(Ed, θ(d), θ(p)); deduced reaction mechanisms. Enriched target.
doi: 10.1016/0375-9474(71)90397-6
1971DI19 Phys.Rev.Lett. 27, 1391 (1971) D.L.Disdier, G.C.Ball, O.Hausser, R.E.Warner Projectile Polarization in the Coulomb Breakup of 6Li NUCLEAR REACTIONS 208Pb(6Li, αd), E=24, 27 MeV; measured σ(Eα, Ed, θ); deduced sequential excitation, breakup process. 6Li level deduced B(E2).
doi: 10.1103/PhysRevLett.27.1391
1971WA18 Phys.Rev.Lett. 27, 961 (1971) R.E.Warner, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Charge-Exchange and/or Knockout Spectator Poles in the Reaction D(3He, tp)p NUCLEAR REACTIONS 2H(3He, tp), E=27 MeV; 2H(3He, 3Hep), E=27 MeV; measured σ(Et, Ep), σ(E(3He), Ep).
doi: 10.1103/PhysRevLett.27.961
1970BE24 Phys.Rev. C2, 297 (1970) Study of the Odd Strontium Isotopes with Stripping and Pickup Reactions NUCLEAR REACTIONS 84,86,88Sr(d, p), (d, t), E=20.65 MeV; measured σ(θ). 83Sr deduced mass excess. 83,85,87Sr deduced levels, L(n), J, S.
doi: 10.1103/PhysRevC.2.297
1970WA15 Nucl.Phys. A148, 503 (1970) R.E.Warner, B.E.Corey, E.L.Petersen, R.W.Bercaw, J.E.Poth p-p and p-t Final State Interactions in the Reaction 3He(d, tp)p NUCLEAR REACTIONS 3He(d, tp), E=20.7 MeV; measured absolute coin σ(Ep, θ(p), θ(t)), σ(Et, θ(t), θ(p)); deduced reaction mechanisms. Enriched target.
doi: 10.1016/0375-9474(70)90644-5
1968WA01 Nucl.Phys. A109, 205(1968) Deuteron Break-up by 42 MeV Alpha Particles NUCLEAR REACTIONS 2H(α, α'p) E=42 MeV; measured σ(Eα', θ(α'), θ(p)) deduced reaction mechanism. Enriched target.
doi: 10.1016/0375-9474(68)90569-1
1967WA01 Phys.Letters 24B, 91 (1967) R.E.Warner, J.S.Vincent, E.T.Boschitz A Search for Unbound T = 1/2 Levels in 3He NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
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1967WA08 Phys.Letters 24B, 517 (1967) The Mechanism of the α+d→α+p+n Reaction NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90413-3
1966WA05 Can.J.Phys. 44, 1225 (1966) Bremsstrahlung Production in 48-MeV p-p Collisions NUCLEAR STRUCTURE 1H; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p66-105
1963WA24 Phys.Rev. 132, 2621 (1963) Inelastic Scattering of 18.2-MeV Protons by Deuterons NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.2621
1959WA07 Phys.Rev. 114, 1338 (1959) Polarization of 6- and 7-MeV Protons Elastically Scattering by Nuclei
doi: 10.1103/PhysRev.114.1338
1958AL88 Bull.Am.Phys.Soc. 3, No.3, 205, R8 (1958) Polarization of 5.7 MeV Protons Elastically Scattered from Nickel
1958WA04 Bull.Am.Phys.Soc. 3, No.3, 204, R6 (1958) Carbon Polarimeter for 6 MeV Proton Polarization Measurements
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