NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = W.Haeberli Found 135 matches. Showing 1 to 100. [Next]2007CR01 Phys.Rev.Lett. 98, 052301 (2007) C.B.Crawford, A.Sindile, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, D.Dutta, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, W.Haeberli, D.Hasell, W.Hersman, M.Holtrop, P.Karpius, M.Kohl, H.Kolster, T.Lee, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.G.Milner, R.P.Redwine, J.Seely, A.Shinozaki, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, J.F.J.van den Brand, J.van der Laan, F.Wang, T.Wise, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart Measurement of the Proton's Electric to Magnetic Form Factor Ratio from 1H(pol)(e(pol), e'p) NUCLEAR REACTIONS 1H(polarized e, e'p), E=high; measured asymmetries. 1H deduced electric to magnetic form factor ratios. Polarized target.
doi: 10.1103/PhysRevLett.98.052301
2006BA24 Phys.Rev.Lett. 96, 174801 (2006) M.Bai, T.Roser, L.Ahrens, I.G.Alekseev, J.Alessi, J.Beebe-Wang, M.Blaskiewicz, A.Bravar, J.M.Brennan, D.Bruno, G.Bunce, E.Courant, A.Drees, W.Fischer, C.Gardner, R.Gill, J.Glenn, W.Haeberli, H.Huang, O.Jinnouchi, J.Kewisch, A.Luccio, Y.Luo, I.Nakagawa, H.Okada, F.Pilat, W.W.MacKay, Y.Makdisi, C.Montag, V.Ptitsyn, T.Satogata, E.Stephenson, D.Svirida, S.Tepikian, D.Trbojevic, N.Tsoupas, T.Wise, A.Zelenski, K.Zeno, S.Y.Zhang Polarized Proton Collisions at 205 GeV at RHIC NUCLEAR REACTIONS 1H(polarized p, X), E ≈ 40-200 GeV; measured beam polarization, energy dependence.
doi: 10.1103/PhysRevLett.96.174801
2006OK03 Phys.Lett. B 638, 450 (2006) H.Okada, I.G.Alekseev, A.Bravar, G.Bunce, S.Dhawan, R.Gill, W.Haeberli, O.Jinnouchi, A.Khodinov, Y.Makdisi, A.Nass, N.Saito, E.J.Stephenson, D.N.Svirida, T.Wise, A.Zelenski Measurement of the analyzing power AN in pp elastic in the CNI region with a polarized atomic hydrogen gass jet target NUCLEAR REACTIONS 1H(polarized p, X), E(cm)=13.7 GeV; measured analysing powers, momentum-transfer dependence. Comparison with Coulomb nuclear interference calculations.
doi: 10.1016/j.physletb.2006.06.008
2006PR22 Phys.Rev.C 74, 064003 (2006) B.v.Przewoski, H.O.Meyer, J.T.Balewski, W.W.Daehnick, J.Doskow, W.Haeberli, R.Ibald, B.Lorentz, R.E.Pollock, P.V.Pancella, F.Rathmann, T.Rinckel, S.K.Saha, B.Schwartz, P.Thorngren-Engblom, A.Wellinghausen, T.J.Whitaker, T.Wise Analyzing powers and spin correlation coefficients for p + d elastic scattering at 135 and 200 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=135, 200 MeV; measured σ(θ), analyzing powers, spin correlation coefficients; deduced no three-nucleon force effect. Polarized target, comparison with Faddeev calculations.
doi: 10.1103/PhysRevC.74.064003
2005BR16 Nucl.Phys. B(Proc.Supp.) S146, 77 (2005) A.Bravar, I.Alekseev, G.Bunce, S.Dhawan, R.Gill, H.Huang, W.Haeberli, G.Igo, O.Jinnouchi, A.Khodinov, A.Kponou, K.Kurita, Y.Makdisi, W.Meng, A.Nass, H.Okada, N.Saito, H.Spinka, E.Stephenson, D.Svirida, D.Underwood, C.Whitten, T.Wise, J.Wood, A.Zelenski Spin Dependence in Polarized pp → pp and p C → p C Elastic Scattering at Very Low Momentum Transfer t at RHIC NUCLEAR REACTIONS 1H, C(polarized p, p), E=4-100 GeV; measured analyzing powers; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysbps.2005.02.066
2003HU06 Phys.Rev.Lett. 90, 202301 (2003) R.Huber, J.Lang, S.Navert, J.Sromicki, K.Bodek, St.Kistryn, J.Zejma, O.Naviliat-Cuncic, E.Stephan, W.Haeberli Search for Time-Reversal Violation in the β Decay of Polarized 8Li Nuclei RADIOACTIVITY 8Li(β-) [from 7Li(polarized d, p)]; measured β-decay asymmetry from polarized source, electrons transverse polarization; deduced time reversal violating triple correlation parameter, scalar leptoquark mass limit. Comparison with model.
doi: 10.1103/PhysRevLett.90.202301
2001ME12 Phys.Rev. C63, 064002 (2001) H.O.Meyer, A.Wellinghausen, J.T.Balewski, J.Doskow, R.E.Pollock, B.von Przewoski, T.Rinckel, P.Thorngren-Engblom, L.D.Knutson, W.Haeberli, B.Lorentz, F.Rathmann, B.Schwartz, T.Wise, W.W.Daehnick, S.K.Saha, P.V.Pancella Complete Set of Polarization Observables in p(pol)p(pol) → ppπ0 Close to Threshold NUCLEAR REACTIONS 1H(polarized p, pπ0), E=325-400 MeV; measured σ(E, θ), polarization observables; deduced partial wave amplitudes. Polarized target.
doi: 10.1103/PhysRevC.63.064002
2001WI16 Phys.Rev.Lett. 87, 042701 (2001) T.Wise, W.Haeberli, B.Lorentz, P.A.Quin, F.Rathmann, B.Schwartz, T.G.Walker, A.Wellinghausen, J.T.Balewski, J.Doskow, H.O.Meyer, R.E.Pollock, B.von Przewoski, T.Rinckel, S.K.Saha, P.V.Pancella Nuclear Polarization of Hydrogen Molecules from Recombination of Polarized Atoms NUCLEAR REACTIONS 1H(polarized p, p'), E=203 MeV; measured polarization transfer; deduced target polarization features. Molecular hydrogen on Cu surface.
doi: 10.1103/PhysRevLett.87.042701
2000LO03 Phys.Rev. C61, 054002 (2000) B.Lorentz, W.Haeberli, F.Rathmann, T.Wise, J.Doskow, M.Dzemidzic, H.O.Meyer, R.E.Pollock, B.von Przewoski, T.Rinckel, F.Sperisen, P.V.Pancella Angular Distribution of the Longitudinal p(pol)p(pol) Spin Correlation Parameter Azz at 197.4 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=197.4 MeV; measured spin correlation parameter A(zz) vs θ. Polarized target. Comparison with model predictions.
doi: 10.1103/PhysRevC.61.054002
2000ME10 Phys.Lett. 480B, 7 (2000) H.O.Meyer, L.D.Knutson, J.T.Balewski, W.W.Daehnick, J.Doskow, W.Haeberli, B.Lorentz, R.E.Pollock, P.V.Pancella, B.von Przewoski, F.Rathmann, T.Rinckel, S.W.Saha, B.Schwartz, P.Thorngren-Engblom, A.Wellinghausen, T.Wise Observation of a Large Longitudinal Analyzing Power in a Nuclear Reaction NUCLEAR REACTIONS 1H(polarized p, pπ0), E=375 MeV; measured longitudinal analyzing power vs azimuthal angle; deduced implications for parity violation experiments. Polarized target.
doi: 10.1016/S0370-2693(00)00360-9
2000TH05 Nucl.Phys. A663-664, 447c (2000) P.Thorngren-Engblom, H.O.Meyer, J.T.Balewski, W.W.Daehnick, J.Doskow, W.Haeberli, B.Lorentz, P.V.Pancella, R.E.Pollock, B.von Przewoski, F.Rathmann, T.Rinckel, S.K.Saha, B.Schwartz, A.Wellinghausen, T.Wise Initial Singlet and Triplet Spin State Contributions to p(pol)p(pol) → ppπ0 NUCLEAR REACTIONS 1H(polarized p, pπ0), E=325, 350, 375, 400 MeV; measured spin-dependent σ(θ). Polarized target.
doi: 10.1016/S0375-9474(99)00604-1
2000VO11 Phys.Rev. C61, 064604 (2000) B.von Przewoski, J.T.Balewski, J.Doskow, H.O.Meyer, R.E.Pollock, T.Rinckel, P.Thorngren-Engblom, A.Wellinghausen, W.Haeberli, B.Lorentz, F.Rathmann, B.Schwartz, T.Wise, W.W.Daehnick, S.K.Saha, P.V.Pancella Measurement of Spin Correlation Coefficients in p(pol)p(pol) → dπ+ NUCLEAR REACTIONS 1H(polarized p, π+), E=350.5, 375.0, 400.0 MeV; measured analyzing power, spin correlation coefficients; deduced partial wave contributions. Polarized target. Comparisons with model predictions.
doi: 10.1103/PhysRevC.61.064604
1999ME26 Phys.Rev.Lett. 83, 5439 (1999) H.O.Meyer, J.T.Balewski, J.Doskow, R.E.Pollock, B.von Przewoski, T.Rinckel, P.Thorngren-Engblom, A.Wellinghausen, W.Haeberli, B.Lorentz, F.Rathmann, B.Schwartz, T.Wise, W.W.Daehnick, S.K.Saha, P.V.Pancella Measurement of Partial-Wave Contributions in pp → ppπ0 NUCLEAR REACTIONS 1H(polarized p, pπ0), E=325-400 MeV; measured spin-dependent total σ ratios; deduced partial wave contributions. Polarized target.
doi: 10.1103/PhysRevLett.83.5439
1999SR01 Phys.Rev.Lett. 82, 57 (1999) J.Sromicki, K.Bodek, D.Conti, St.Kistryn, J.Lang, S.Navert, O.Naviliat-Cuncic, E.Stephan, C.Sys, J.Zejma, W.Haeberli, E.Reichert, M.Steigerwald Polarization in Mott Scattering of Multi-MeV Electrons from Heavy Nuclei NUCLEAR REACTIONS Pb(polarized e, e'), E=14 MeV; measured σ(θ), scattering asymmetry, analyzing power A; deduced target thickness effects.
doi: 10.1103/PhysRevLett.82.57
1998ME21 Phys.Rev.Lett. 81, 3096 (1998) H.O.Meyer, J.T.Balewski, M.Dzemidzic, J.Doskow, R.E.Pollock, B.von Przewoski, T.Rinckel, F.Sperisen, P.Thorngren-Engblom, M.Wolanski, W.Haeberli, B.Lorentz, F.Rathmann, B.Schwartz, T.Wise, W.W.Daehnick, R.W.Flammang, S.K.Saha, D.J.Tedeschi, P.V.Pancella Dependence of p(pol)p(pol) → ppπ0 Near Threshold on the Spin of the Colliding Nucleons NUCLEAR REACTIONS 1H(polarized p, pπ0), E=325.6, 350.5, 375, 400 MeV; measured spin-dependent σ, Ay, (A(xx)-A(yy)), asymmetries; deduced partial wave contributions. Polarized target.
doi: 10.1103/PhysRevLett.81.3096
1998RA14 Phys.Rev. C58, 658 (1998) F.Rathmann, B.von Przewoski, W.A.Dezarn, J.Doskow, M.Dzemidzic, W.Haeberli, J.G.Hardie, B.Lorentz, H.O.Meyer, P.V.Pancella, R.E.Pollock, T.Rinckel, F.Sperisen, T.Wise Complete Angular Distribution Measurements of pp Spin Correlation Parameters Axx, Ayy, and Axz and Analyzing Power Ay at 197.4 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=197.4 MeV; measured σ(θ), A(y)(θ), spin correlation coefficients; deduced large spin-spin effects. Comparison to partial wave analyses, NN potential models. Polarized target.
doi: 10.1103/PhysRevC.58.658
1998VO10 Phys.Rev. C58, 1897 (1998) B.von Przewoski, F.Rathmann, W.A.Dezarn, J.Doskow, M.Dzemidzic, W.Haeberli, J.G.Hardie, B.Lorentz, H.O.Meyer, P.V.Pancella, R.E.Pollock, T.Rinckel, F.Sperisen, T.Wise Proton-Proton Analyzing Power and Spin Correlation Measurements between 250 and 450 MeV at 7' ≤ θc.m. ≤ 90' with Internal Target in a Storage Ring NUCLEAR REACTIONS 1H(polarized p, p), E=250-450 MeV; measured analyzing power Ay(θ), spin correlation coefficients Axx(θ), Ayy(θ), Axz(θ). Polarized target. Comparison with partial wave analysis, potential models.
doi: 10.1103/PhysRevC.58.1897
1997HA03 Phys.Rev. C55, 597 (1997) W.Haeberli, B.Lorentz, F.Rathmann, M.A.Ross, T.Wise, W.A.Dezarn, J.Doskow, J.G.Hardie, H.O.Meyer, R.E.Pollock, B.von Przewoski, T.Rinckel, F.Sperisen, P.V.Pancella Proton-Proton Spin Correlation Measurements at 200 MeV with an Internal Target in a Storage Ring NUCLEAR REACTIONS 1H(polarized p, p), E=197.8 MeV; measured analyzing power, spin correlation coefficients vs θ. Comparisons with potential models, partial wave analyses. Internal polarized gas target.
doi: 10.1103/PhysRevC.55.597
1997HA53 Nucl.Phys. A626, 103c (1997) Polarization Experiments at Proton Storage Rings NUCLEAR REACTIONS 1H(polarized p, p), E not given; reviewed, analyzed polarization, spin correlation data. Polarized targets.
doi: 10.1016/S0375-9474(97)00527-7
1997KA10 Phys.Rev. C55, 640 (1997) N.I.Kaloskamis, A.Garcia, S.E.Darden, E.Miller, W.Haeberli, P.A.Quin, B.P.Schwartz, E.Yacoub, E.G.Adelberger Isospin Mixing in 37K and Spin Decomposition of Gamow-Teller Strength in 37Ca Decay NUCLEAR REACTIONS 36Ar(polarized p, p), E=3.22-5.98 MeV; measured σ(θ), analyzing power vs θ vs E. 37K deduced resonances, J, π, Γ, Γp, isospin-mixing matrix elements. RADIOACTIVITY 37Ca(β+); analyzed data; deduced Gamow-Teller transition strength related features.
doi: 10.1103/PhysRevC.55.640
1997ME19 Nucl.Phys. A626, 135c (1997) H.O.Meyer, M.Dzemidzic, J.Doskow, W.Haeberli, J.G.Hardie, B.Lorentz, P.V.Pancella, R.E.Pollock, B.von Przewoski, F.Rathmann, T.Rinckel, F.Sperisen, T.Wise Calibration of the Polarization of a Beam of Arbitrary Energy in a Storage Ring NUCLEAR REACTIONS 1H(polarized p, p), E=200, 400 MeV; measured scattering asymmetries; deduced stored beam polarization. Polarized target.
doi: 10.1016/S0375-9474(97)00530-7
1996SR02 Phys.Rev. C53, 932 (1996) J.Sromicki, M.Allet, K.Bodek, W.Hajdas, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, J.Zejma, W.Haeberli Study of Time Reversal Violation in β Decay of Polarized 8Li RADIOACTIVITY 8Li(β-) [from 7Li(polarized d, p), E=10 MeV]; measured electron transverse polarizations, time reversal violating triple correlation R. Polarization transfer, Mott scattering, vector polarized source.
doi: 10.1103/PhysRevC.53.932
1995DE67 Nucl.Instrum.Methods Phys.Res. A362, 36 (1995) W.A.Dezarn, J.Doskow, J.G.Hardie, H.O.Meyer, R.E.Pollock, B.von Przewoski, T.Rinckel, F.Sperisen, W.Haeberli, B.Lorentz, F.Rathmann, M.A.Ross, T.Wise, P.V.Pancella Polarized Internal Gas Target for Hydrogen and Deuterium at the IUCF Cooler Ring NUCLEAR REACTIONS 1H(polarized p, p), E=200 MeV; measured analyzing power vs θ; deduced target polarization. Polarized internal target for 1,2H at IUCF cooler ring.
doi: 10.1016/0168-9002(95)00230-8
1995ZE01 Phys.Rev. C51, 1494 (1995) V.J.Zeps, E.G.Adelberger, A.Garcia, C.A.Gossett, H.E.Swanson, W.Haeberli, P.A.Quin, J.Sromicki Parity Mixing of the 0+-0- I = 1 Doublet in 14N NUCLEAR REACTIONS, ICPND 13C(polarized p, p), E=1.1-2.2 MeV; 13C(p, γ), E=0.45-3 MeV; measured σ(E). 14N levels deduced ΔI=0 parity-mixing matrix element, levels parameters. Enriched targets. S-matrix analysis.
doi: 10.1103/PhysRevC.51.1494
1994MC05 Phys.Rev. C50, 589 (1994) J.E.McAninch, L.O.Lamm, W.Haeberli Analyzing Power in Neutron-Deuteron Elastic Scattering at E(lab)(n) = 3 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=3 MeV; measured analyzing power vs θ; deduced polarization transfer coefficient for 3H(polarized p, n) reaction.
doi: 10.1103/PhysRevC.50.589
1994PR11 Nucl.Instrum.Methods Phys.Res. A349, 321 (1994) Measurement of Cell Wall Depolarization of Polarized Hydrogen Gas Targets in a Weak Magnetic Field NUCLEAR REACTIONS 3H(polarized d, n), E=low; measured neutron anisotropy; deduced H0 target polarization. Tritiated target.
doi: 10.1016/0168-9002(94)91196-7
1994RO30 Nucl.Instrum.Methods Phys.Res. A344, 307 (1994) M.A.Ross, A.D.Roberts, T.Wise, W.Haeberli, W.A.Dezarn, J.Doskow, H.O.Meyer, R.E.Pollock, B.von Przewoski, T.Rinckel, F.Sperisen, P.V.Pancella Performance of a Polarized-Hydrogen Storage Cell Target
doi: 10.1016/0168-9002(94)90079-5
1993CO07 Phys.Lett. 304B, 60 (1993) A.Converse, M.Allet, W.Haeberli, W.Hajdas, J.Lang, J.Liechti, H.Luscher, M.A.Miller, R.Muller, O.Naviliat-Cuncic, P.A.Quin, J.Sromicki Measurement of the Asymmetry Parameter for 35Ar β-Decay as a Test of the CVC Hypothesis RADIOACTIVITY 35Ar(β+) [from 35Cl(polarized p, n)35Ar, E=9.2 MeV]; measured β-decay, βγ-coin, asymmetry parameter, Eβ, Iβ; deduced conserved vector current hypothesis implications. Polarized source.
doi: 10.1016/0370-2693(93)91400-H
1993MC08 Phys.Lett. 307B, 13 (1993) J.E.McAninch, W.Haeberli, H.Witala, W.Glockle, J.Golak Analyzing Power in nd Elastic Scattering at E(n)(lab) = 3 MeV. Measurement and Calculation NUCLEAR REACTIONS 2H(polarized n, n), E < breakup threshold; measured analyzing power vs θ; deduced charge independence breaking component in NN-interaction role. Rigorous 3-body calculations.
doi: 10.1016/0370-2693(93)90185-K
1993PR06 Nucl.Instrum.Methods Phys.Res. A326, 416 (1993) Polarization Measurement for Polarized Gas Targets NUCLEAR REACTIONS 2H(t, n), E not given; measured neutron intensity; deduced target tensor polarization.
doi: 10.1016/0168-9002(93)90844-8
1993RO24 Nucl.Instrum.Methods Phys.Res. A326, 424 (1993) M.A.Ross, W.K.Pitts, W.Haeberli, H.O.Meyer, S.F.Pate, R.E.Pollock, B.von Przewoski, T.Rinckel, J.Sowinski, F.Sperisen, P.V.Pancella Test of a Windowless Storage Cell Target in a Proton Storage Ring NUCLEAR REACTIONS 1H(p, p), E=185 MeV; analyzed σ(θ); deduced target density luminosity.
doi: 10.1016/0168-9002(93)90845-9
1992AL01 Phys.Rev.Lett. 68, 572 (1992) M.Allet, W.Hajdas, J.Lang, H.Luscher, R.Muller, O.Naviliat-Cuncic, J.Sromicki, A.Converse, W.Haeberli, M.A.Miller, P.A.Quin Search for Time-Reversal Violation in the Beta Decay of 8Li RADIOACTIVITY 8Li [from 7Li(polarized d, p), E=10 MeV]; measured electron transverse polarization; deduced time reversal violating triple correlation parameter.
doi: 10.1103/PhysRevLett.68.572
1992CO06 Phys.Rev. C45, 2320 (1992) A.Converse, W.Haeberli, W.Hajdas, St.Kistryn, J.Lang, J.Liechti, H.Luscher, R.Muller, J.Smyrski, J.Sromicki Absolute Calibration of the Transverse Analyzing Power in Proton-Carbon Elastic Scattering at 50.24 MeV NUCLEAR REACTIONS C(polarized p, p), E=50.24 MeV; measured analyzing power vs θ; deduced transverse analyzing power calibration.
doi: 10.1103/PhysRevC.45.2320
1992DU05 Nucl.Instrum.Methods Phys.Res. A322, 13 (1992) M.Duren, Z.Moroz, M.Veltri, K.Zapfe, H.Mairon, M.Metzger, B.Povh, K.Rith, E.Steffens, F.Stock, D.Toporkov, F.Zetsche, T.-A.Shibata, D.Fick, W.Korsch, G.Graw, W.Haeberli, G.T.Garvey Test of a Polarized Hydrogen Gas Target Based on the Storage Cell Technique NUCLEAR REACTIONS 1H(α, α), E=34.5 MeV; measured integrated yield; deduced target areal density. Polarized target, storage rings usage.
doi: 10.1016/0168-9002(92)90352-5
1992PI01 Phys.Rev. C45, R1 (1992) W.K.Pitts, W.Haeberli, J.S.Price, H.O.Meyer, S.F.Pate, R.E.Pollock, B.von Przewoski, T.Rinckel, J.Sowinski, F.Sperisen, P.V.Pancella Spin Dependence in pp Scattering in the Coulomb-Nuclear Interference Region NUCLEAR REACTIONS 1H(polarized p, p), E=185.4 MeV; measured analyzing power vs θ; deduced electromagnetic spin-orbit effects role.
doi: 10.1103/PhysRevC.45.R1
1991MI18 Phys.Rev. C44, 1995 (1991) M.A.Miller, P.A.Voytas, A.D.Roberts, P.A.Quin, W.Haeberli Polarization Transfer in the 23Na(p(pol), 23Mg(pol))n, 31P(p(pol), 31S(pol))n, and 35Cl(p(pol), 35Ar(pol))n Reactions NUCLEAR REACTIONS 31P(polarized p, n), E=6.38-9.1 MeV; 35Cl(polarized p, n), E=7.27-10.29 MeV; 23Na(polarized p, n), E ≈ 7 MeV; measured residual nucleus β+-decay parity violating asymmetry; deduced polarization transfer coefficient energy dependence. NaI, red phosphorous, Cl2, CCL4-(He) mixture targets. RADIOACTIVITY 31S [from 31P(polarized p, n), E=6.38-9.1 MeV]; 35Ar [from 35Cl(polarized p, n), E=7.27-10.29 MeV]; 23Mg [from 23Na(polarized p, n), E ≈ 7 MeV]; measured β+-decay parity violating asymmetry.
doi: 10.1103/PhysRevC.44.1995
1991VO04 Phys.Rev. C44, 44 (1991) B.von Przewoski, H.O.Meyer, P.V.Pancella, S.F.Pate, R.E.Pollock, T.Rinckel, F.Sperisen, J.Sowinski, W.Haeberli, W.K.Pitts, J.S.Price Absolute Measurement of the p + p Analyzing Power at 183 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=183.1 MeV; measured analyzing power, θ(cm)=18.1°.
doi: 10.1103/PhysRevC.44.44
1990SR03 J.Phys.(Paris), Colloq.C-6, 527 (1990) J.Sromicki, M.Allet, A.Converse, W.Hajdas, J.Lang, H.Luscher, R.Muller, O.Naviliat-Cuncic, W.Haeberli, M.A.Miller, P.A.Quin An Experiment to Investigate Time Reversal Invariance in the Decay of 8Li RADIOACTIVITY 8Li [from 7Li(polarized d, p), E=10 MeV]; measured time reversal violating parameter.
1989HO05 Nucl.Instrum.Methods Phys.Res. A274, 207 (1989) D.Holslin, J.McAnich, J.Sromicki, P.A.Quin, W.Haeberli New Instrumental Effects in Fast Neutron Polarization Measurements NUCLEAR REACTIONS 1H(polarized n, n), E=10 MeV; measured analyzing power vs θ; deduced instrumental effects role.
doi: 10.1016/0168-9002(89)90381-1
1989KI03 Phys.Lett. 219B, 58 (1989) S.Kistryn, J.Lang, J.Liechti, H.Luscher, Th.Maier, R.Muller, M.Simonius, J.Smyrski, J.Sromicki, W.Haeberli Measurement of Parity Nonconservation in Proton-Deuteron Scattering at 43 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=43 MeV; measured σ asymmetry; deduced longitudinal analyzing power.
doi: 10.1016/0370-2693(89)90837-X
1989SM05 Nucl.Phys. A501, 319 (1989) J.Smyrski, St.Kistryn, J.Lang, J.Liechti, H.Luscher, Th.Maier, R.Muller, M.Simonius, J.Sromicki, F.Foroughi, W.Haeberli A Precision Measurement of the Analyzing Power A(y) in pp Elastic Scattering at 50.04 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=50.04 MeV; measured analyzing power vs θ. Phase shift, potential model predictions comparisons.
doi: 10.1016/0375-9474(89)90296-0
1988HA30 Can.J.Phys. 66, 485 (1988) Parity Violation in Proton Scattering: Low energy region NUCLEAR REACTIONS 1H(polarized p, p), E < 50 MeV; compiled, analyzed data; deduced parity-violating analyzing power.
doi: 10.1139/p88-080
1988HO13 Phys.Rev.Lett. 61, 1561 (1988) D.Holslin, J.McAninch, P.A.Quin, W.Haeberli New Test of Nucleon-Nucleon Potential Models NUCLEAR REACTIONS 1H(polarized n, n), E=10.03 MeV; measured analyzing power vs θ; deduced neutron magnetic moment role.
doi: 10.1103/PhysRevLett.61.1561
1988WA13 Phys.Rev. C37, 2301 (1988) T.R.Wang, W.Haeberli, S.W.Wissink, S.S.Hanna Electric Quadrupole Strength in 20Ne from the 19F(p(pol), γ0)20Ne Reaction NUCLEAR REACTIONS, ICPND 19F(polarized p, γ), E=3.5-13.3 MeV; measured σ(θ), analyzing power vs θ, σ(E). 20Ne deduced GQR features.
doi: 10.1103/PhysRevC.37.2301
1987HA31 Helv.Phys.Acta 60, 776 (1987) W.Haeberli, S. Jaccard, S.Kistryn, J.Lang, J.Liechti, Th. Maier, R.Muller, F.Nessi-Tedaldi, M.Simonius, J.Smyrski, J.Sromicki Precision Measurement of Parity Violation in 45 MeV pp Scattering NUCLEAR REACTIONS 1H(polarized p, p), E=45 MeV; measured σ helicity dependence; deduced nucleon-nucleon interaction parity violation.
1987KI09 Phys.Rev.Lett. 58, 1616 (1987) S.Kistryn, J.Lang, J.Liechti, Th.Maier, R.Muller, F.Nessi-Tedaldi, M.Simonius, J.Smyrski, S.Jaccard, W.Haeberli, J.Sromicki Precision Measurement of Parity Nonconservation in Proton-Proton Scattering at 45 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=45 MeV; measured longitudinal analyzing power; deduced parity nonconservation. Gas target, ionization chamber.
doi: 10.1103/PhysRevLett.58.1616
1986LA29 Phys.Rev. C34, 1545 (1986) J.Lang, Th.Maier, R.Muller, F.Nessi-Tedaldi, Th.Roser, M.Simonius, J.Sromicki, W.Haeberli Parity Nonconservation in Elastic pα Scattering NUCLEAR REACTIONS 4He(polarized p, p), E=46 MeV; measured positive, negative helicity σ; deduced parity nonconserving longitudinal analyzing power. Pressurized target, ionization chamber.
doi: 10.1103/PhysRevC.34.1545
1986ME02 Phys.Lett. 166B, 282 (1986) S.Mellema, T.R.Wang, W.Haeberli Evidence for Multipolarities other than E2 in the 2H(d, γ)4He Reactions NUCLEAR REACTIONS 2H(polarized d, γ), E=10 MeV; measured σ(θ), vector, tensor analyzing power vs θ.
doi: 10.1016/0370-2693(86)90799-9
1986ME16 Phys.Rev. C34, 2043 (1986) S.Mellema, T.R.Wang, W.Haeberli Tensor-Force Effects in the 2H(d(pol), γ)4He Reaction and the D State of 4He NUCLEAR REACTIONS 2H(polarized d, γ), E=10 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced partial-wave amplitudes, phases. 4He transitions deduced γ-multipolarity, multipole strengths.
doi: 10.1103/PhysRevC.34.2043
1985LA01 Phys.Rev.Lett. 54, 170 (1985); Erratum Phys.Rev.Lett. 54, 2729 (1985) J.Lang, Th.Maier, R.Muller, F.Nessi-Tedaldi, Th.Roser, M.Simonius, J.Sromicki, W.Haeberli Parity Nonconservation in Elastic pα Scattering and the Determination of the Weak Meson-Nucleon Coupling Constants NUCLEAR REACTIONS 4He(polarized p, p), E=46 MeV; measured analyzing power vs θ; deduced parity nonconservation, weak meson-nucleon coupling constants.
doi: 10.1103/PhysRevLett.54.170
1984BA54 Phys.Rev. C30, 1409 (1984) R.Balzer, R.Henneck, Ch.Jacquemart, J.Lang, F.Nessi-Tedaldi, T.Roser, M.Simonius, W.Haeberli, S.Jaccard, W.Reichart, Ch.Weddigen Parity Violation in Proton-Proton Scattering at 45 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=44.8 MeV; measured parity nonconserving longitudinal analyzing power. Longitudinally polarized beam, pressurized H2 target, cylindrical ionization chamber scattered proton detector.
doi: 10.1103/PhysRevC.30.1409
1984KR12 Nucl.Instrum.Methods 220, 123 (1984) D.Kramer, K.Becker, K.Blatt, R.Caplar, D.Fick, H.Gemmeke, W.Haeberli, H.Jansch, O.Karban, I.Koenig, L.Luh, K.-H.Mobius, V.Necas, W.Ott, M.Tanaka, G.Tungate, I.M.Turkiewicz, A.Weller, E.Steffens The Source of Polarized Heavy Ions (PSI) at the Heidelberg MP Tandem NUCLEAR REACTIONS 1H(polarized 7Li, α), E=44 MeV; measured polarization effect vs filter magnet current.
1983CA20 Phys.Rev. C28, 1837 (1983) j Dependence of the Vector Analyzing Power in the 40Ca(d(pol), p)41Ca Reaction at 4 MeV NUCLEAR REACTIONS 40Ca(polarized d, p), E=4 MeV; measured σ(Ep), vector analyzing power iT11(θ). 41Ca level deduced J, π.
doi: 10.1103/PhysRevC.28.1837
1982BA09 Phys.Rev.Lett. 48, 918 (1982) M.D.Barker, P.C.Colby, W.Haeberli, P.Signell Proton-Proton Scattering at Low Energies NUCLEAR REACTIONS 1H(polarized p, p), E=5.05, 9.85 MeV; measured analyzing power vs θ; deduced model independent s-, p-wave phase shifts.
doi: 10.1103/PhysRevLett.48.918
1980CA18 Nucl.Phys. A349, 103 (1980) Effect of the Deuteron D-state on the Polarization and Analyzing Power in ln=0 (d, p) Reactions NUCLEAR REACTIONS 116Sn(d, p), (polarized d, p), E=8.22, 18 MeV; 90Zr(d, p), (polarized d, p), E=12 MeV; calculated σ(θ), proton polarization P(θ), vector analyzing power vs θ; deduced D- state effects, separation of proton, deuteron spin-dependent effects. DWBA analyses.
doi: 10.1016/0375-9474(80)90446-7
1980ST18 Phys.Rev.Lett. 45, 520 (1980) Determination of the Asymptotic Ratio of the Deuteron D- and S-State Amplitudes NUCLEAR REACTIONS 208Pb(polarized d, p), E=7, 8, 9 MeV; measured tensor analyzing power vs θ. 2H deduced asymptotic d- to s-state amplitude ratio. DWBA, different deuteron wave functions.
doi: 10.1103/PhysRevLett.45.520
1979BA65 Helv.Phys.Acta 52, 420 (1979) R.Balzer, R.Henneck, C.Jacquemart, J.Lang, M.Simonius, W.Haeberli, S.Jaccard, L.Rezzonico, C.Weddigen Messung der Paritatsverletzung in Proton-Proton-Streuung bei 50 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=50 MeV; measured asymmetry.
1979CA12 Nucl.Phys. A327, 419 (1979) The Separation of Proton and Deuteron Spin-Dependent Effects in the 116Sn(d, p)117Sn Reaction NUCLEAR REACTIONS 116Sn(polarized d, d), E=8.22 MeV; measured iT11(θ), σ(θ). 117Sn(polarized p, p), E=12.91 MeV; measured Ay(θ), σ(θ); deduced optical-model parameters. 116Sn(polarized d, p), E=8.22 MeV; measured iT11(Ep, θ), σ(Ep, θ). 117Sn(polarized p, d), E=12.91 MeV; measured Ay(Ed, θ), σ(Ed, θ). Enriched targets.
doi: 10.1016/0375-9474(79)90267-7
1979GO06 Nucl.Phys. A316, 116 (1979) The Optical Model for Elastic Scattering of 10 to 15 MeV Polarized Deuterons from Medium-Weight Nuclei NUCLEAR REACTIONS 46Ti, 52Cr, 54Fe, 68Zn, 90Zr(polarized d, d), E=10.0 MeV; 68Zn, 90Zr(polarized d, d), E=12.0 MeV; 46Ti, 54Fe(polarized d, d)E=13.0 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced optical-model parameters. Enriched targets.
doi: 10.1016/0375-9474(79)90675-4
1978GO03 Phys.Rev.Lett. 40, 701 (1978) Evidence for a Complex L.S Interaction in the Deuteron-Nucleus Optical Potential NUCLEAR REACTIONS 46Ti, 52Cr, 60,64Ni, 68Zn, 90Zr, 56Fe, 122Sn(polarized d, d), E ≈ 15 MeV; calculated potential, σ(θ), A(θ).
doi: 10.1103/PhysRevLett.40.701
1977BR27 Nucl.Phys. A287, 205 (1977); Erratum Nucl.Phys. A306, 536 (1978) Vector Analyzing Power and Cross Section for (d, t) and (d, 3He) Reactions on 64Zn at E = 13 MeV NUCLEAR REACTIONS 64Zn(polarized d, d), E=13.0 MeV; measured vector analyzing power iT11(θ), cross section σ(θ); deduced optical-model parameters. 64Zn(polarized d, t), (polarized d, 3He), E=13.0 MeV; measured iT11(θ), σ(θ). 63Zn, 63Cu levels deduced J, π, S. Enriched target.
doi: 10.1016/0375-9474(77)90491-2
1977BR28 Nucl.Phys. A287, 213 (1977) Tensor Analyzing Powers in 64Zn(d, t)63Zn and 64Zn(d, 3He)63Cu at E = 13 MeV NUCLEAR REACTIONS 64Zn(polarized d, t), (polarized d, 3He), E=13.0 MeV; measured A(θ). Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(77)90492-4
1977ME06 Nucl.Instrum.Methods 140, 85 (1977) H.O.Meyer, T.P.Cleary, W.Haeberli A Polarization Standard for Protons between 6 and 8 MeV NUCLEAR REACTIONS 4He(polarized p, p), E=5-12 MeV; measured A(E, θ).
doi: 10.1016/0029-554X(77)90068-4
1977ST01 Nucl.Phys. A277, 374 (1977) Observation of Deuteron D-State and Compound Nucleus Effects in (d, p) Reactions on 46Ti and 52Cr with a Polarized Deuteron Beam NUCLEAR REACTIONS 46Ti(polarized d, d), E=5.92, 9.96 MeV; 52Cr(polarized d, d), E=5.97 MeV; 54Fe(polarized d, d), E=6.0 MeV; measured vector analyzing power iT11(θ), σ(θ); deduced optical model parameters. 46Ti(polarized d, p), E=5.92, 9.96 MeV; 52Cr(polarized d, p), E=5.97 MeV; measured analyzing powers iT11, T20, T21, T22(Ep, θ). 46Ti, 52Cr(polarized d, p), E=5-7 MeV; measured vector analyzing power iT11(Ed; Ep, θ), σ(Ed;Ep, θ). 47Ti, 53Cr deduced level properties. Enriched targets.
doi: 10.1016/0375-9474(77)90708-4
1977ST06 Nucl.Phys. A277, 365 (1977) K.Stephenson, L.D.Knutson, W.Haeberli An Absolute Standard for Deuteron Vector Analyzing Powers NUCLEAR REACTIONS 16O(d, α), E=6.84 MeV; measured T21(θ), T20(θ); deduced iT11(θ); θ=29°, 34°. 3He(d, p), E=6.44 MeV; measured iT11(29°). 3He(d, α), E=6.44 MeV; measured iT11(θ); θ=29°, 34°.
doi: 10.1016/0375-9474(77)90707-2
1976BR17 Nucl.Phys. A263, 189 (1976) M.E.Brandan, G.R.Plattner, W.Haeberli A Test of p-4He Phase Shifts between 2 and 9 MeV NUCLEAR REACTIONS 4He(polarized p, p), E=3.47-8.94 MeV; measured A(E, θ). 4He(p, p), E=2.24-5.90 MeV; measured σ(168.8°)/σ(104.4°). Phase-shift analysis.
doi: 10.1016/0375-9474(76)90167-6
1976HA53 Phys.Rev. C14, 2322 (1976) Comment on Elastic Proton Scattering from 56Fe in the Giant Resonance Region of 57Co NUCLEAR REACTIONS 56Fe(polarized p, p), E=8-17 MeV; reanalyzed phase shifts; deduced no evidence of resonance in 57Co.
doi: 10.1103/PhysRevC.14.2322
1975HU08 Phys.Rev.Lett. 35, 429 (1975) J.D.Hutton, W.Haeberli, L.D.Knutson, P.Signell Polarization of Proton-Proton Scattering at 10 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=10 MeV; measured A(θ).
doi: 10.1103/PhysRevLett.35.429
1975KN04 Phys.Rev.Lett. 35, 558 (1975) Probing the Deuteron Wave Function with Sub-Coulomb (d, p) Reactions NUCLEAR REACTIONS 208Pb(polarized d, p), E=9 MeV; calculated measured A(θ).
doi: 10.1103/PhysRevLett.35.558
1975KN08 Phys.Rev. C12, 1469 (1975) Spin-Dependent Potentials for Deuteron-Nucleus Scattering NUCLEAR REACTIONS 90Zr(polarized d, d), E=5.5 MeV; 208Pb(polarized d, d), E=9.0 MeV; measured σ(θ), polarization parameters iT(θ). Optical model analysis, enriched targets.
doi: 10.1103/PhysRevC.12.1469
1975KO19 Nucl.Phys. A252, 381 (1975) Vector Analyzing Power and Cross Section for (d, p) Reactions on 53Cr, 57Fe, 117Sn and 119Sn NUCLEAR REACTIONS 53Cr, 57Fe(polarized d, d), (polarized d, p), E=10 MeV; 117,119Sn(polarized d, d), (polarized d, p), E=12 MeV; measured σ(θ), polarization parameters iT11(θ); deduced deuteron optical-model parameters, angular momentum transfer. 54Cr, 58Fe, 118,120Sn levels deduced J, π, S. Enriched targets.
doi: 10.1016/0375-9474(75)90507-2
1975VI06 Nucl.Phys. A253, 55 (1975) Study of the Reactions 118Sn(d, t) and 98Mo(d, t) (I). Spectroscopy of 117Sn and 97Mo NUCLEAR REACTIONS 118Sn, 98Mo(polarized d, d), E=12.0 MeV; measured vector analyzing power iT11(θ), cross section σ(θ); deduced optical model parameters. 118Sn, 98Mo(polarized d, t), E=12.0 MeV; measured iT11(Et, θ), σ(Et, θ). 117Sn, 97Mo levels deduced J, π, spectroscopic factors. Enriched targets.
doi: 10.1016/0375-9474(75)90121-9
1974AR16 Nucl.Instrum.Methods 116, 605 (1974) J.Arvieux, J.Birchall, H.E.Conzett, W.Dahme, W.Haeberli, R.M.Larimer Is the 12C(d, d0) Reaction a Good Polarization Standard (Question) NUCLEAR REACTIONS 12C(polarized d, d), E=20, 25, 30 MeV; measured Pd.
doi: 10.1016/0029-554X(74)90851-9
1974KN01 Phys.Rev.Lett. 32, 690 (1974) L.D.Knutson, E.J.Stephenson, W.Haeberli Classical Description of the Deuteron D-State Effects in Sub-Coulomb (d, p) Reactions NUCLEAR REACTIONS 208Pb(polarized d, p); measured nothing, calculated effect of deuteron d-state on analyzing power.
doi: 10.1103/PhysRevLett.32.690
1974LO15 Nucl.Phys. A232, 381 (1974) Elastic Scattering of 9-13 MeV Vector Polarized Deuterons NUCLEAR REACTIONS 27Al, Si, 46,48Ti, 53Cr, 68Zn, 90Zr, 120Sn(polarized d, d), E=9-13 MeV; measured iT11(θ), σ(θ); deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(74)90627-7
1973KN03 Phys.Rev.Lett. 30, 986 (1973) Investigation of the Spin Dependence in the Deuteron-Nucleus Interaction NUCLEAR REACTIONS 90Zr(d, d), E=5.5 MeV; measured σ(θ), analyzing power (θ); deduced optical model parameters.
doi: 10.1103/PhysRevLett.30.986
1973KN05 Phys.Rev.Lett. 31, 392 (1973) L.D.Knutson, E.J.Stephenson, N.Rohrig, W.Haeberli Observation of the Deuteron D-State Effects in (d, p) Reactions NUCLEAR REACTIONS 52Cr, 90Zr, 208Pb(polarized d, p), E=6, 9, 10 MeV; measured analyzing power.
doi: 10.1103/PhysRevLett.31.392
1973RA18 Nucl.Phys. A206, 459 (1973) R.D.Rathmell, P.J.Bjorkholm, W.Haeberli Vector Analysing Power and Cross Section for 90Zr(d, p)91Zr at 11 and 12 MeV NUCLEAR REACTIONS 90Zr(polarized d, d), E=11 MeV; measured polarization parameters iT11 (Ed; θ), σ(Ed; θ). 90Zr(polarized d, p), E=11, 12 MeV; measured polarization parameters iT11 (Ed; Ep, θ), σ(Ed; Ep, θ). 91Zr deduced J, π, S. Enriched targets.
doi: 10.1016/0375-9474(73)90078-X
1973RO16 Nucl.Phys. A206, 225 (1973) A Study of (d, p) Reactions on 52Cr, 54Fe and 90Zr with a Tensor Polarized Deuteron Beam NUCLEAR REACTIONS 52Cr, 54Fe, 90Zr(polarized d, p), Ed=10.0 MeV; measured polarization parameters iT11, T20, T21, T22 (Ep, θ), σ(Ep, θ). 90Zr(polarized d, p), Ed=9.9, 10.0, 10.1 MeV; measured polarization parameter iT11 (Ed, Ep, θ). 53Cr, 55Fe, 91Zr deduced levels. Enriched targets.
doi: 10.1016/0375-9474(73)90530-7
1973VI06 Nucl.Phys. A210, 70 (1973) S.E.Vigdor, R.D.Rathmell, H.S.Liers, W.Haeberli Study of the Reactions 208Pb(d, p) and 208Pb(d, t) Near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(polarized d, d), Ed=12.3 MeV; measured vector analyzing power iT11(θ), cross section σ(θ). Deduced optical model parameters. 208Pb(polarized d, p), (polarized d, t), Ed=12.3 MeV; measured iT11(Q, θ), σ(Q, θ). 207Pb, 209Pb deduced J, π, S. Enriched target.
doi: 10.1016/0375-9474(73)90505-8
1973VI07 Nucl.Phys. A210, 93 (1973) S.E.Vigdor, R.D.Rathmell, W.Haeberli Semi-Classical Interpretation of the Vector Analyzing Power in Sub-Coulomb Neutron-Transfer Reactions NUCLEAR REACTIONS 90Zr, 207Pb(polarized d, p), 208Pb(polarized d, t); calculated σ(θ), iT11.
doi: 10.1016/0375-9474(73)90506-X
1972DU18 Nucl.Phys. A196, 107 (1972) J.C.Duder, E.J.Stephenson, W.Haeberli Polarization Transfer in the 2H(d, p)3H Reaction at 0° NUCLEAR REACTIONS 2H(polarized d, p), E=7.1, 9.8 MeV; measured polarization transfer coefficients, θ=0°. Enriched target.
doi: 10.1016/0375-9474(72)90953-0
1972KO41 Nucl.Phys. A196, 225 (1972) Vector Analysing Power and Cross Section for (d, p) Reactions on 40Ca, 46Ti, 48Ti, 50Ti, 52Cr and 54Fe NUCLEAR REACTIONS 40Ca, 46,48,50Ti, 52Cr, 54Fe(polarized d, p)41Ca, 47,49,51Ti, 53Cr, 55Fe, Ed=10, 11 MeV; measured polarization parameters iT11(Ed;Ep, θ), cross sections σ(Ed;Ep, θ). 41Ca, 47,49,51Ti, 53Cr, 55Fe deduced J, π, S. Natural Ca target, enriched 46,48,50Ti, 52Cr, 54Fe targets.
doi: 10.1016/0375-9474(72)90963-3
1972RA01 Nucl.Phys. A178, 458 (1972) Elastic Scattering of Polarized Protons from Nuclei Near A = 200 between 11 and 14 MeV NUCLEAR REACTIONS 181Ta(p, p), E=10.8, 13.8 MeV; 197Au(p, p), E=13.0, 13.8 MeV; 207Pb(p, p), E=13.0 MeV; 208Pb(p, p), E=13.0 MeV; 209Bi(p, p), E=10.8, 13.0 MeV; measured polarization(E;θ), σ(E;θ); deduced optical-model parameters. Natural 181Ta, 197Au, 209Bi targets, enriched 207Pb, 208Pb targets. 181Ta(p, p), E=9-14 MeV; 197Au(p, p), E=8-14 MeV; measured polarization(E). 182Ta, 198Au deduced resonances. Natural targets, polarized beams.
doi: 10.1016/0375-9474(72)90473-3
1971KE16 Nucl.Phys. A172, 625 (1971) The Asymmetry of Protons from the Break-up of Vector-Polarized Deuterons on 4He NUCLEAR REACTIONS 4He(polarized d, pn), E=8.5, 10, 11 MeV; measured analyzing power iT11(Ed, Ep, θ(p)). Natural target.
doi: 10.1016/0375-9474(71)90049-2
1971KO20 Nucl.Phys. A172, 652 (1971) Vector Analyzing Power and Cross Section for 40Ca(d, p)41Ca from 5 to 11 MeV NUCLEAR REACTIONS 40Ca(polarized d, p), Ed=5, 9, 11 MeV; measured polarization parameters iT11(Ed;Ep, θ), cross sections σ(Ed;Ep, θ); deduced J-dependence. 41Ca deduced S. Natural target.
doi: 10.1016/0375-9474(71)90052-2
1971KO21 Nucl.Phys. A172, 663 (1971) D.C.Kocher, P.J.Bjorkholm, W.Haeberli The Reactions 16O(d, p)17O and 28Si(d, p)29Si Initiated by Vector-Polarized Deuterons NUCLEAR REACTIONS 16O(polarized d, d); measured polarization parameter iT11(Ed, θ); 16O(polarized d, p)17O, Ed=8 MeV; 28Si(polarized d, p)29Si, Ed=9 MeV; measured polarization parameters iT11(Ed;Ep, θ), cross sections σ(Ed;Ep, θ); deduced J-dependence. 17O, 29Si deduced S. Natural targets.
doi: 10.1016/0375-9474(71)90053-4
1971LI03 Phys.Rev.Lett. 26, 261 (1971) H.S.Liers, R.D.Rathmell, S.E.Vigdor, W.Haeberli j Dependence in the Vector Analyzing Power for 208Pb(d, t)207Pb NUCLEAR REACTIONS 208Pb(polarized d, t), E=12.3 MeV; measured σ(θ), vector analyzing power iT11(θ). 207Pb levels deduced S.
doi: 10.1103/PhysRevLett.26.261
1971SC04 Nucl.Phys. A163, 432 (1971) P.Schwandt, T.B.Clegg, W.Haeberli Polarization Measurements and Phase Shifts for p-4He Scattering between 3 and 18 MeV NUCLEAR REACTIONS 4He(polarized p, p), E=4.58, 5.95, 7.89, 9.89, 11.94 MeV; measured polarization P(E, θ); deduced scattering phase shifts. Natural target.
doi: 10.1016/0375-9474(71)90500-8
1970KE17 Nucl.Phys. A156, 465 (1970) Vector-Polarization Measurements and Phase-Shift Analysis for D-α Scattering between 3 and 11 MeV NUCLEAR REACTIONS 4He(vector-polarized d, d), E=3-11 MeV; measured vector analyzing power (iT11(θ)); deduced phase shifts. 6Li deduced resonances.
doi: 10.1016/0375-9474(70)90244-7
1970KO11 Phys.Rev.Lett. 25, 36 (1970) Inconsistencies in Angular Momentum Assignments to Nuclear Energy Levels in 41Ca NUCLEAR REACTIONS 40Ca(vector-polarized d, p), E=11 MeV; measured vector analyzing power iT11(θ). 41Ca levels deduced L(n), J.
doi: 10.1103/PhysRevLett.25.36
1970LO03 Nucl.Phys. A148, 236 (1970) Polarization of Protons Elastically Scattered from Beryllium NUCLEAR REACTIONS 9Be(p, p), Ep=3.0 to 12.0 MeV; measured polarization P(E;θ); deduced optical-model parameters. Natural target.
doi: 10.1016/0375-9474(70)90621-4
1969KO11 Phys.Rev.Letters 23, 315 (1969) Stripping Reactions on Odd-A Nuclei Initiated by Vector-Polarized Deuterons NUCLEAR REACTIONS 53Cr(polarized d, p), E=10 MeV; measured σ(θ), vector analyzing power. 54Cr levels deduced resonances, J, π, L(n), S.
doi: 10.1103/PhysRevLett.23.315
1969MO05 Nucl.Phys. A126, 225(1969) Proton Polarization in p-3He Elastic Scattering Between 4 and 11 MeV NUCLEAR REACTIONS 3He(polarized p, p), E=4-11 MeV; measured polarization (E, θ); deduced phase shifts. Enriched target.
doi: 10.1016/0375-9474(69)90409-6
1969SC02 Nucl.Phys. A123, 401(1969) Optical-Model Analysis of d-Ca Polarization and Cross-Section Measurements from 5 to 34 MeV NUCLEAR REACTIONS 40Ca(polarized d, d), E=5, 7, 9, 11 MeV; measured polarization parameters T(qk)(θ); deduced optical-model parameters for E=5-35 MeV. Natural target.
doi: 10.1016/0375-9474(69)90510-7
1968BJ07 Bull. Am. Phys. Soc. 13, No. 4, 723, KH1 (1968) Deuteron Vector Analyzing Power for the Reactions 54Fe(d, p)55Fe and 16O(d, p)17O NUCLEAR STRUCTURE 55Fe, 17O, 16O; measured not abstracted; deduced nuclear properties.
1968CL07 Nucl.Phys. A119, 238(1968) T.B.Clegg, G.R.Plattner, W.Haeberli Polarization of Protons Elastically Scattered from Deuterons at 12.0 MeV NUCLEAR REACTIONS 2H(p, p), E=12 MeV; measured polarization (θ). Enriched target.
doi: 10.1016/0375-9474(68)90818-X
1968SC29 Nucl.Phys. A110, 585 (1968) Elastic scattering of polarized deuterons from 27Al, Si and 60Ni between 7 and 11 MeV NUCLEAR REACTIONS 27Al(d, d), Si(d, d), 60Ni(d, d), E=7-11 MeV; measured products, 60Ni, Si, 27Al; deduced σ(θ), polarization data. Data were imported from EXFOR entry C1068.
doi: 10.1016/0375-9474(68)90375-8
1968VE07 Nucl.Phys. A115, 172 (1968) Polarization Measurements Near Isobaric Analogue Resonances in 139La and 141Pr NUCLEAR REACTIONS 138Ba(p, p), E = 9.6-12.0 MeV; 140Ce(p, p), E = 9.2-11.8 MeV; measured polarization (E; θ). 139Ba, 141Ce levels deduced J. Natural targets.
doi: 10.1016/0375-9474(68)90650-7
1968YU01 Nucl.Phys. A117, 1 (1968) Use of Polarized Deuterons to Determine the Total Angular Momentum Transfer in Stripping Reactions NUCLEAR REACTIONS 9Be, 12C, 24Mg, 40Ca, 52Cr(polarized d, p), E=8 MeV; measured vector analyzing power. Natural targets.
doi: 10.1016/0375-9474(68)90858-0
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