NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = C.L.Hollas Found 44 matches. 1989NE01 Phys.Rev. C39, 965 (1989) C.R.Newsom, C.L.Hollas, R.D.Ransome, P.J.Riley, B.E.Bonner, J.G.J.Boissevain, J.J.Jarmer, M.W.McNaughton, J.E.Simmons, T.S.Bhatia, G.Glass, J.C.Hiebert, L.C.Northcliffe, W.B.Tippens Neutron-Proton Analyzing Power Measurements from 375 to 775 MeV NUCLEAR REACTIONS 1H(n, n), E=375-775 MeV; measured analyzing power. Polarized proton target, unpolarized neutron beam.
doi: 10.1103/PhysRevC.39.965
1989SH26 Phys.Rev. C40, 2203 (1989) R.L.Shypit, D.V.Bugg, A.H.Sanjari, D.M.Lee, M.W.McNaughton, R.R.Silbar, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis Spin Dependence of pp → npπ+ from 492 to 796 MeV NUCLEAR REACTIONS 1H(polarized p, pπ+), E=492-796 MeV; measured spin correlation parameters; deduced no dibaryon evidence. Longitudinally polarized target.
doi: 10.1103/PhysRevC.40.2203
1988SH06 Phys.Rev.Lett. 60, 901 (1988) R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis Evidence against Broad Dibaryons NUCLEAR REACTIONS 1H(polarized p, π+n), E=492-796 MeV; measured spin correlation parameters; deduced no broad dibaryons. Isobar analysis.
doi: 10.1103/PhysRevLett.60.901
1988SH09 Nucl.Phys. A477, 541 (1988) R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis A(SL), A(LL) and A(N0) for NN → πD at 492, 729 and 796 MeV NUCLEAR REACTIONS 1H(polarized p, π+), E=492-796 MeV; measured spin correlation parameters A(LL), A(SL), A(N0). Longitudinally polarized propanediol target.
doi: 10.1016/0375-9474(88)90404-6
1987HO10 Nucl.Instrum.Methods Phys.Res. B24/25, 503 (1987) C.L.Hollas, D.A.Close, C.E.Moss Analysis of Fissionable Material using Delayed Gamma Rays from Photofission NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(γ, F)138Cs/94Sr/136I/89Rb/90Kr/97Y, E=10 MeV bremsstrahlung; measured fission product Iγ ratios. Enriched 235U, 239Pu targets.
doi: 10.1016/0168-583X(87)90695-1
1987RI06 Phys.Lett. 197B, 23 (1987) P.J.Riley, M.Bachman, C.L.Hollas, K.H.McNaughton, S.-W.Xu, B.E.Bonner, O.B.Van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet Polarization Observables for the Reaction pp → ppπ0 at 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ0), E=647, 733, 800 MeV; measured induced polarization, analyzing power, Wolfenstein parameters. Orthogonal beam polarization.
doi: 10.1016/0370-2693(87)90334-0
1985HO16 Phys.Rev.Lett. 55, 29 (1985) C.L.Hollas, K.H.McNaughton, P.J.Riley, Shen-wu Xu, B.E.Bonner, O.B.van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet Wolfenstein Polarization Observables for the Reaction p(pol)p → p(pol)πn at 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ+), E=650, 733, 800 MeV; measured Wolfenstein polarization parameters, induced polarization, σ(θ1, θ2) vs proton momentum.
doi: 10.1103/PhysRevLett.55.29
1985MA06 Phys.Rev. D31, 966 (1985) W.P.Madigan, D.A.Bell, J.A.Buchanan, M.M.Calkin, J.M.Clement, M.Copel, M.D.Corcoran, K.A.Johns, J.D.Lesikar, H.E.Miettinen, G.S.Mutchler, C.J.Naudet, G.P.Pepin, G.C.Phillips, J.B.Roberts, S.E.Turpin, E.V.Hungerford, B.W.Mayes, A.D.Hancock, L.S.Pinsky, K.K.Sekharan, C.L.Hollas, P.J.Riley, J.C.Allred, B.E.Bonner, P.Cameron, S.T.Linn, W.von Witsch, M.Furic, V.Valkovic Transverse-Spin Dependence of the p-p Total Cross Section Δσ(T) from 0.8 to 2.5 GeV/c NUCLEAR REACTIONS 1H(polarized p, p), E at 0.8-2.5 GeV/c; measured σ asymmetry, transverse spin dependence. Polarized target.
doi: 10.1103/PhysRevD.31.966
1985MC07 Nucl.Instrum.Methods 241, 435 (1985) M.W.McNaughton, B.E.Bonner, H.Ohnuma, O.B.Van Dijk, Sun Tsu-Hsun, C.L.Hollas, D.J.Cremans, K.H.McNaughton, P.J.Riley, R.F.Rodebaugh, Shen-Wu Xu, S.E.Turpin, B.Aas, G.S.Weston The p-C Analyzing Power between 100 and 750 MeV NUCLEAR REACTIONS C(polarized p, pX), E=80-584 MeV; measured inclusive analyzing power vs θ. Large solid angle polarimeter.
doi: 10.1016/0168-9002(85)90595-9
1985SU02 Phys.Rev. C31, 515 (1985) Sun Tsu-hsun, B.E.Bonner, M.W.McNaughton, H.Ohnuma, O.B.van Dyck, G.S.Weston, B.Aas, E.Bleszynski, M.Bleszynski, G.J.Igo, D.J.Cremans, C.L.Hollas, K.H.McNaughton, P.J.Riley, R.F.Rodebaugh, Shen-wu Xu, S.E.Turpin Measurements of the Spin-Rotation Parameters for (p(pol)d → p(pol)d) Elastic Scattering at 496, 647, and 800 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=496, 647, 800 MeV; measured spin rotation parameters, induced polarization, analyzing power vs θ. Liquid 2H target, noneikonal multiple-scattering theory.
doi: 10.1103/PhysRevC.31.515
1984HO19 Phys.Lett. 143B, 343 (1984) C.L.Hollas, D.J.Cremans, R.D.Ransome, P.J.Riley, B.E.Bonner, M.W.McNaughton, S.Wood The Energy Dependence of the 90° pp Elastic Scattering Depolarization Parameter and Amplitudes between 0.9 and 1.5 GeV/c NUCLEAR REACTIONS 1H(polarized p, p), E=386-790 MeV; measured depolarization parameter vs E; deduced transversity amplitudes vs E.
doi: 10.1016/0370-2693(84)91479-5
1984HO20 Phys.Rev. C30, 1251 (1984) C.L.Hollas, D.J.Cremans, K.H.McNaughton, P.J.Riley, R.F.Rodebaugh, Shen-wu Xu, B.E.Bonner, M.W.McNaughton, H.Ohnuma, O.B.van Dyck, Sun Tsu-hsun, S.E.Turpin, B.Aas, G.S.Weston D(SS), D(LL), D(SL), D(LS), and P for pp → pp at 600 to 800 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=600-800 MeV; measured spin parameters D(SS), D(LL), D(SL), D(LS), polarization, K(SS), K(LL), K(SL), K(LS), vs θ; deduced phase shifts.
doi: 10.1103/PhysRevC.30.1251
1983BA17 Nucl.Phys. A397, 21 (1983) C.M.Bartle, D.W.Gebbie, C.L.Hollas Total Cross Sections for the 6Li(n, α)3H Reaction between 12 and 18 MeV NUCLEAR REACTIONS 6Li(n, α), E=12-18.2 MeV; measured σ(E). Enriched target.
doi: 10.1016/0375-9474(83)90076-3
1983BO01 Phys.Rev. D27, 497 (1983) B.E.Bonner, C.L.Hollas, C.R.Newsom, P.J.Riley, G.Glass, M.Jain, B.J.VerWest Zero-Degree Measurements of the Inclusive Reaction np → pX in the Energy Range 400 to 800 MeV NUCLEAR REACTIONS 1H(n, X), E at 950-1430 MeV/c; measured inclusive σ(θp) vs proton momentum. Field theoretical peripheral model, meson exchange, nucleon-nucleon, nucleon-isobar intermediate states.
doi: 10.1103/PhysRevD.27.497
1983GL04 Phys.Rev. D28, 1045 (1983) G.Glass, M.Jain, L.C.Northcliffe, C.L.Hollas, C.R.Newsom, P.J.Riley, B.E.Bonner, J.E.Simmons Inclusive Inelastic Reaction np → pX at 795 MeV NUCLEAR REACTIONS 1H(n, X), E=795 MeV; measured inclusive σ(θ) vs proton momentum. One pion exchange, statistical models.
doi: 10.1103/PhysRevD.28.1045
1983GL06 Phys.Lett. 129B, 27 (1983) G.Glass, T.S.Bhatia, J.C.Hiebert, L.C.Northcliffe, W.B.Tippens, B.J.Verwest, C.L.Hollas, C.R.Newsom, R.D.Ransome, P.J.Riley, G.P.Pepin, B.E.Bonner, J.E.Simmons The Measurement of K(NN) and K(LL) in p(pol)p → n(pol)X at 800 MeV NUCLEAR REACTIONS 1H(polarized p, nX), E=800 MeV; measured σ(θn) vs neutron momentum, spin transfer parameters, polarized neutrons.
doi: 10.1016/0370-2693(83)90721-9
1982BH01 Phys.Rev.Lett. 48, 227 (1982) T.S.Bhatia, G.Glass, J.C.Hiebert, L.C.Northcliffe, W.B.Tippens, B.E.Bonner, J.E.Simmons, C.L.Hollas, C.R.Newsom, P.J.Riley, R.D.Ransome Difference between Polarization and Analyzing Power for 800-MeV n-p Elastic Scattering: Test of time-reversal invariance NUCLEAR REACTIONS 2H(p, n), E=800 MeV; measured P(θn); deduced no time reversal invariance evidence. Analyzing power data input, quasifree scattering. Liquid deuterium target.
doi: 10.1103/PhysRevLett.48.227
1982HO08 Phys.Rev. C25, 2614 (1982) C.L.Hollas, C.R.Newsom, P.J.Riley, B.E.Bonner, G.Glass Deuteron Spectrum in np → d(ππ)0 at 1.46 GeV/c NUCLEAR REACTIONS 1H(n, d), E=795 MeV; measured σ(θ) vs deuteron momentum, missing mass spectra.
doi: 10.1103/PhysRevC.25.2614
1982MC04 Phys.Rev. C25, 1967 (1982) M.W.McNaughton, B.E.Bonner, W.D.Cornelius, E.W.Hoffman, O.B.van Dyck, R.L.York, R.D.Ransome, C.L.Hollas, P.J.Riley, K.Toshioka Spin Transfer Measurements for pp → pp at 800 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=800 MeV; measured spin depolarization, transfer parameters.
doi: 10.1103/PhysRevC.25.1967
1982MC07 Phys.Rev. C26, 249 (1982) M.W.McNaughton, B.E.Bonner, E.W.Hoffman, O.B.van Dyck, C.L.Hollas, P.J.Riley, K.H.McNaughton, K.Imai, K.Toshioka, J.Roberts, S.E.Turpin, B.Aas, A.Rahbar Spin Transfer Measurements for pp → pp at 647 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=647 MeV; measured spin depolarization, spin transfer parameters vs θ.
doi: 10.1103/PhysRevC.26.249
1982RA20 Nucl.Instrum.Methods 201, 315 (1982) R.D.Ransome, C.L.Hollas, P.J.Riley, B.E.Bonner, W.D.Cornelius, O.B.van Dyck, E.W.Hoffman, S.A.Wood, K.Toshioka Measurement of the p-C Analyzing Power between 100 and 750 MeV and the p-Be Analyzing Power at 780 MeV NUCLEAR REACTIONS C(polarized p, pX), E=100-750 MeV; Be(polarized p, pX), E=780 MeV; measured analyzing power vs θ. Inclusive reaction.
doi: 10.1016/0167-5087(82)90558-0
1982RA34 Phys.Rev.Lett. 48, 781 (1982) R.D.Ransome, C.L.Hollas, P.J.Riley, B.E.Bonner, W.R.Gibbs, M.W.McNaughton, J.E.Simmons, T.S.Bhatia, G.Glass, J.C.Hiebert, L.C.Northcliffe, W.B.Tippens Spin Dependence In Neutron-Proton Charge Exchange At 790 Mev NUCLEAR REACTIONS 1H(n, n), E=790 MeV; measured products, Ep, Ip; deduced polarization data. Data were imported from EXFOR entry 13538.
doi: 10.1103/PhysRevLett.48.781
1981BH03 Phys.Rev. C24, 796 (1981) T.S.Bhatia, G.Glass, J.C.Hiebert, L.C.Northcliffe, W.B. Tippens, B.E.Bonner, J.E.Simmons, C.L.Hollas, C.R.Newsom, P.J.Riley, R.D.Ransome Zero-Crossing Angle in the np Analyzing Power at Medium Energies and Its Relation to Charge Symmetry NUCLEAR REACTIONS 1H(polarized n, p), E=425, 565, 665 MeV; measured A(E, θ); deduced zero-crossing angle.
doi: 10.1103/PhysRevC.24.796
1981HO21 Phys.Rev. C24, 1561 (1981) C.L.Hollas, C.R.Newsom, P.J.Riley, B.E.Bonner, G.Glass Test of Charge Symmetry in the np → dπ0 Reaction at 795 MeV NUCLEAR REACTIONS 1H(n, d), E=795 MeV; measured σ(θ); deduced f-wave pion-deuteron final state. Legendre polynomial analysis.
doi: 10.1103/PhysRevC.24.1561
1981RI06 Phys.Lett. 103B, 313 (1981) P.J.Riley, C.L.Hollas, C.R.Newsom, R.D.Ransome, B.E.Bonner, J.E.Simmons, T.S.Bhatia, G.Glass, J.C.Hiebert, L.C.Northcliffe, W.B.Tippens The Measurement of K(NN), K(LL) in p(pol)d → n(pol)X and p(pol)9Be → n(pol)X at 800 MeV NUCLEAR REACTIONS 2H, 9Be(polarized p, n), E=800 MeV; measured polarization transfer parameters. Liquid deuterium target.
doi: 10.1016/0370-2693(81)90231-8
1979BA61 Nucl.Phys. A331, 502 (1979) L.O.Barbopoulos, D.W.Gebbie, J.Nurzynski, M.Borsaru, C.L.Hollas Single-Neutron Transfer Reactions 76,78,80,82Se(p, d)75,77,79,81Se at E = 33 MeV NUCLEAR REACTIONS 76,78,80,82Se(p, d), E=33 MeV; measured σ(Ed, θ), Q. 75,77,79,81Se deduced levels, L, S. Enriched targets.
doi: 10.1016/0375-9474(79)90356-7
1978AN10 Nucl.Phys. A303, 154 (1978) K.A.Aniol, D.W.Gebbie, C.L.Hollas, J.Nurzynski The 50, 52, 54Cr(α, p)53, 55, 57Mn Reactions at E = 18 and 26 MeV NUCLEAR REACTIONS 50,52,54Cr(α, p), E=18, 26 MeV; measured σ(Ep, θ); deduced Q. 53,55,57Mn deduced levels, J, π, L, relative strengths. Enriched targets.
doi: 10.1016/0375-9474(78)90049-0
1978FR11 Z.Phys. A286, 307 (1978) A.D.Frawley, G.M.Crawley, C.L.Hollas Fluctuations in Inelastic Proton Scattering from 58Ni in the Energy Range 17.1 to 20.6 MeV NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=17.1-20.6 MeV; measured σ(E, θ). 59Cu levels deduced Γ. Enriched target.
doi: 10.1007/BF01408262
1977BO18 Nucl.Phys. A284, 379 (1977) M.Borsaru, D.W.Gebbie, J.Nurzynski, C.L.Hollas, L.O.Barbopoulos, A.R.Quinton A Study of the 78,76Se(p, t)76,74Se Reactions at E = 33 MeV NUCLEAR REACTIONS 78,76Se(p, t), E=33 MeV; measured σ(Et, θ). 76,74Se deduced levels, J, π, L, enhancement coefficients. Enriched targets.
doi: 10.1016/0375-9474(77)90391-8
1977BO25 Phys.Rev.Lett. 39, 1253 (1977) B.E.Bonner, C.L.Hollas, C.R.Newsom, P.J.Riley, G.Glass nd Scattering at 180° for Neutron Energies from 200 to 800 MeV NUCLEAR REACTIONS 2H(n, n), E=200-800 MeV; measured σ(E, θ).
doi: 10.1103/PhysRevLett.39.1253
1977HO02 Nucl.Phys. A276, 1 (1977) C.L.Hollas, K.A.Aniol, D.W.Gebbie, M.Borsaru, J.Nurzynski, L.O.Barbopoulos States in 97,101Ru Observed in the Reactions 96,100Ru(d, p) NUCLEAR REACTIONS 96,100Ru(d, p), E=11.5 MeV; measured σ(Ep, θ); deduced Q. 97,101Ru deduced levels, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(77)90155-5
1975BO01 Nucl.Phys. A237, 93 (1975) M.Bonsaru, J.Nurzynski, D.W.Gebbie, C.L.Hollas, S.Whineray, N.H.Merrill, L.O.Barbopoulos, A.R.Quinton (d, t) Reactions on 54Cr, 67,68Zn Nuclei NUCLEAR REACTIONS 54Cr, 67,68Zn(d, t), E=12 MeV; measured σ(Et, θ). 53Cr, 66,67Zn deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(75)90465-0
1973ME24 Nucl.Phys. A216, 61 (1973) N.H.Merrill, S.Whineray, W.M.Zuk, D.C.Weisser, C.L.Hollas, M.Borsaru Isobaric Analogue Resonance Studies in Some Rare-Earth Nuclei NUCLEAR REACTIONS 160Gd, 162,164Dy, 166,168,170Er, 174Yb(p, p), E=10-12 MeV; measured σ(E, θ); 161Tb, 163,165Ho, 166,168,170Tm deduced IAR, L, π, level-width, Nilsson coefficients, Coulomb displacement energy. Enriched targets.
doi: 10.1016/0375-9474(73)90518-6
1972HO15 Phys.Rev. C5, 1641 (1972) C.L.Hollas, H.R.Hiddleston, V.D.Mistry, S.Sen, P.J.Riley Study of Core Coupling in 87Rb Through Isobaric-Analog Resonances. I NUCLEAR REACTIONS 86Kr(p, p), E=4.76-10.10 MeV; measured σ(E). 87Rb deduced isobaric analog resonances, level-width, S, L.
doi: 10.1103/PhysRevC.5.1641
1972HO16 Phys.Rev. C5, 1646 (1972) C.L.Hollas, H.R.Hiddleston, V.D.Mistry, S.Sen, P.J.Riley Study of Core Coupling in 87Rb Through Isobaric-Analog Resonances. II NUCLEAR REACTIONS 86Kr(p, p'), E=4.76-10.10 MeV; measured σ(E;Ep', θ). 87Rb deduced isobaric analog resonances, level-width. 86Kr deduced levels, isobaric analogs.
doi: 10.1103/PhysRevC.5.1646
1972HO28 Nucl.Phys. A190, 362 (1972) J.L.Horton, C.L.Hollas, P.J.Riley, S.A.S.Zaidi, C.M.Jones, J.L.C.Ford, Jr. The 90Zr(d, n)91Nb and 96Zr(d, n)97Nb Reactions NUCLEAR REACTIONS 90Zr(d, n)91Nb, 96Zr(d, n)97Nb, E=12 MeV; measured σ(En, θ). 91Nb, 97Nb levels deduced angular momentum transfer values, S.
doi: 10.1016/0375-9474(72)90147-9
1972SE04 Phys.Rev. C5, 1278 (1972) S.Sen, C.L.Hollas, C.W.Bjork, P.J.Riley Reaction 38Ar(d, p)39Ar NUCLEAR REACTIONS 38Ar(d, p), E=10.064 MeV; measured σ(Ep, θ). 39Ar deduced levels, L(n), J, π, S.
doi: 10.1103/PhysRevC.5.1278
1971CO21 Phys.Rev. C4, 836 (1971) W.R.Coker, C.L.Hollas, P.J.Riley, S.Sen 86Kr(d, n)87Rb(A) Threshold Cusp and the Systematic Appearance of Charge-Exchange Cusps NUCLEAR REACTIONS 86Kr(d, n), E=5-10.5 MeV; measured σ(E); deduced charge-exchange effects coupled-channel Born approximation.
doi: 10.1103/PhysRevC.4.836
1971HI02 Phys.Rev. C3, 905 (1971) H.R.Hiddleston, C.L.Hollas, V.D.Mistry, P.J.Riley Isobaric Analog Resonances in Proton Elastic and Inelastic Scattering from 130Te NUCLEAR REACTIONS 130Te(p, p), E=7.8-12 MeV; measured nothing; analyzed σ(E). 131I deduced isobaric analog resonances, J, π, level-width, S. 130Te(p, p'), E=7.8-12 MeV; measured σ(E;Ep', θ). 130Te deduced levels, J, π.
doi: 10.1103/PhysRevC.3.905
1971RI12 Phys.Rev. C4, 1864 (1971) P.J.Riley, J.L.Horton, C.L.Hollas, S.A.A.Zaidi, C.M.Jones, J.L.C.Ford, Jr. Spectroscopy of 93,95,97Tc through the (d, n) Reaction NUCLEAR REACTIONS 92,94,96Mo(d, n), E=12 MeV; measured σ(En, θ). 93,95,97Tc deduced levels, J, π, L(p), S.
doi: 10.1103/PhysRevC.4.1864
1971SE04 Phys.Rev. C3, 2314 (1971) Reaction 36Ar(d, p)37Ar NUCLEAR REACTIONS 36Ar(d, p), E=9.162 MeV; measured σ(Ep, θ). 37Ar deduced levels, L(n), J, π, S.
doi: 10.1103/PhysRevC.3.2314
1970HA16 Phys.Rev. C1, 938 (1970) K.Haravu, C.L.Hollas, P.J.Riley, W.R.Coker 86Kr(d, p)87Kr Reaction NUCLEAR REACTIONS 86Kr(d, p), E=11 MeV; measured σ(Ep, θ). 87Kr deduced levels, J, π, S, L(n).
doi: 10.1103/PhysRevC.1.938
1970MI08 Phys.Rev. C1, 1595 (1970) V.D.Mistry, C.L.Hollas, H.R.Hiddleston, P.J.Riley Isobaric Analog Resonances in Proton Elastic Scattering from 110Cd, 112Cd, and 114Cd NUCLEAR REACTIONS 110,112,114Cd(p, p), (p, p'), E=6-11 MeV; measured σ(E). 111,113,115In deduced isobaric analog, level-width, L(p), J, π, S. Cd-In isotopes deduced Coulomb displacement energies.
doi: 10.1103/PhysRevC.1.1595
1970ZA09 Phys.Rev.Lett. 25, 1503 (1970) S.A.A.Zaidi, C.L.Hollas, J.L.Horton, P.J.Riley, J.L.C.Ford, Jr., C.M.Jones Anomalies in the Cross Sections of (d, n) Reactions Leading to Isobaric Analog States NUCLEAR REACTIONS 92,94,96Mo, 96Zr(d, n), E=12 MeV; measured σ(En, θ). 93,95,97Tc, 97Nb deduced isobaric analog states, S.
doi: 10.1103/PhysRevLett.25.1503
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