NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.M.Poskanzer Found 60 matches. 2015SU05 Phys.Rev. C 91, 024903 (2015) X.Sun, H.Masui, A.M.Poskanzer, A.Schmah Blast wave fits to elliptic flow data at √ sNN = 7.7-2760 GeV
doi: 10.1103/PhysRevC.91.024903
2014YA18 Phys.Rev. C 90, 024903 (2014) L.Yan, J.-Y.Ollitrault, A.M.Poskanzer Eccentricity distributions in nucleus-nucleus collisions
doi: 10.1103/PhysRevC.90.024903
2009OL05 Phys.Rev. C 80, 014904 (2009) J.-Y.Ollitrault, A.M.Poskanzer, S.A.Voloshin Effect of flow fluctuations and nonflow on elliptic flow methods
doi: 10.1103/PhysRevC.80.014904
2009OL08 Nucl.Phys. A830, 279c (2009) J.-Y.Ollitrault, A.M.Poskanzer, S.A.Voloshin Effect of flow fluctuations and nonflow on elliptic flow methods
doi: 10.1016/j.nuclphysa.2009.09.026
2004PO15 J.Phys.(London) G30, S1225 (2004) A.M.Poskanzer, for the STAR Collaboration Azimuthal anisotropy: the higher harmonics NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed particles azimuthal distributions, anisotropy, related features.
doi: 10.1088/0954-3899/30/8/095
2003WE06 Nucl.Phys. A715, 583c (2003) A.Wetzler, N.Borghini, P.M.Dinh, J.-Y.Ollitrault, A.M.Poskanzer, S.A.Voloshin, and the NA49 Collaboration Directed and Elliptic Flow in Pb+Pb collisions at 40 and 158 AGeV NUCLEAR REACTIONS Pb(Pb, X), E=40, 158 GeV/nucleon; measured proton and charged pion directed and elliptic flow vs transverse momentum, rapidity.
doi: 10.1016/S0375-9474(02)00634-1
2002BO34 Phys.Rev. C66, 014901 (2002) N.Borghini, P.M.Dinh, J.-Y.Ollitrault, A.M.Poskanzer, S.A.Voloshin Effects of Momentum Conservation on the Analysis of Anisotropic Flow NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed directed flow vs rapidity; deduced correction for correlations due to momentum conservation.
doi: 10.1103/PhysRevC.66.014901
2000VO02 Phys.Lett. 474B, 27 (2000) The Physics of the Centrality Dependence of Elliptic Flow NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; calculated pions elliptic flow centrality dependence, related features. Hadronic, partonic characteristics discussed. Comparisons with data.
doi: 10.1016/S0370-2693(00)00017-4
1999PO28 Nucl.Phys. A661, 341c (1999) A.M.Poskanzer, S.A.Voloshin, for the NA49 Collaboration Centrality Dependence of Directed and Elliptic Flow at the SPS NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed data; deduced elliptic flow vs rapidity, centrality.
doi: 10.1016/S0375-9474(99)85036-2
1998PO14 Nucl.Phys. A638, 463c (1998) A.M.Poskanzer, for the NA49 Collaboration Directed and Elliptic Flow in 158 GeV/Nucleon Pb + Pb Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; measured protons, pions transverse momentum, rapidity; deduced collective flow rapidity dependence.
doi: 10.1016/S0375-9474(98)00379-0
1998PO17 Phys.Rev. C58, 1671 (1998) Methods for Analyzing Anisotropic Flow in Relativistic Nuclear Collisions
doi: 10.1103/PhysRevC.58.1671
1997BI14 Nucl.Instrum.Methods Phys.Res. A385, 535 (1997) F.Bieser, G.Cooper, W.Cwienk, V.Eckardt, H.Fessler, H.G.Fischer, F.Gabler, E.Gornicki, W.E.Hearn, W.Heupke, D.Irmscher, P.Jacobs, S.Kleinfelder, V.Lindenstruth, B.Machowski, K.Marks, O.Milgrome, A.Mock, T.Noggle, W.Pimpl, A.M.Poskanzer, W.Rauch, R.Renfordt, H.G.Ritter, D.Rohrich, H.Rudolph, G.W.Ruschmann, E.Schafer, P.Seyboth, J.Seyerlein, R.Stock, K.Sulimma, M.Toy, C.Vu, S.Wenig, H.Wieman, M.E.Wright Design and Performance of TPC Readout Electronics for the NA49 Experiment
doi: 10.1016/S0168-9002(96)01029-7
1995AL20 Phys.Rev.Lett. 75, 3814 (1995) T.Alber, H.Appelshauser, J.Bachler, J.Bartke, H.Bialkowska, F.Bieser, M.A.Bloomer, C.O.Blyth, R.Bock, C.Bormann, F.P.Brady, R.Brockmann, P.Buncic, H.L.Caines, D.Cebra, P.Chan, G.E.Cooper, J.G.Cramer, P.B.Cramer, P.Csato, I.Derado, J.Dunn, V.Eckardt, F.Eckhardt, S.Euler, M.I.Ferguson, H.G.Fischer, Z.Fodor, P.Foka, P.Freund, M.Fuchs, J.Gal, M.Gazdzicki, E.Gladysz, J.Grebieszkow, J.Gunther, J.W.Harris, W.Heck, S.Hegyi, L.A.Hill, I.Huang, M.A.Howe, G.Igo, D.Irmscher, J.Jacobs, P.G.Jones, K.Kadija, J.Kecskemeti, M.Kowalski, A.Kuhmichel, B.Lasiuk, S.Margetis, J.W.Mitchell, A.Mock, J.M.Nelson, G.Odyniec, J.Palinkas, G.Palla, A.D.Panagiotou, A.Petridis, A.Piper, A.M.Poskanzer, D.J.Prindle, F.Puhlhofer, W.Rauch, R.Renfordt, W.Retyk, H.G.Ritter, D.Rohrich, H.Rudolph, K.Runge, A.Sandoval, H.Sann, E.Schafer, N.Schmitz, S.Schonfelder, P.Seyboth, J.Seyerlein, F.Sikler, E.Skrzypczak, R.Stock, H.Strobele, I.Szentpetery, J.Sziklai, M.Toy, T.A.Trainor, S.Trentalange, M.Vassiliou, G.Vesztergombi, D.Vranic, S.Wenig, C.Whitten, T.Wienold, L.Wood, J.Zimanyi, X.-Z.Zhu, R.Zybert Transverse Energy Production in 208Pb + Pb Collisions at 158 GeV per Nucleon NUCLEAR REACTIONS Pb(208Pb, X), E=158 GeV/nucleon; measured forward, transverse energy related features.
doi: 10.1103/PhysRevLett.75.3814
1988DO01 Phys.Rev. C37, 163 (1988) K.G.R.Doss, H.-A.Gustafsson, H.H.Gutbrod, D.Hahn, K.-H.Kampert, B.Kolb, H.Lohner, A.M.Poskanzer, H.G.Ritter, H.R.Schmidt, H.Stocker Multiplicity and Bombarding Energy Dependence of the Entropy in Relativistic Heavy-Ion Reactions NUCLEAR REACTIONS 93Nb(93Nb, X), 197Au(197Au, X), E=150, 250, 400, 650 MeV/nucleon; measured light cluster to proton yield ratio.
doi: 10.1103/PhysRevC.37.163
1987DO13 Phys.Rev.Lett. 59, 2720 (1987) K.G.R.Doss, H.-A.Gustafsson, H.Gutbrod, J.W.Harris, B.V.Jacak, K.-H.Kampert, B.Kolb, A.M.Poskanzer, H.-G.Ritter, H.R.Schmidt, L.Teitelbaum, M.Tincknell, S.Weiss, H.Wieman Fragment Flow in Nuclear Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=200 MeV/nucleon; measured fragment (Z ≥ 3) multiplicity distributions, transverse momentum alignment mean values, azimuthal angular correlations.
doi: 10.1103/PhysRevLett.59.2720
1984GU15 Phys.Lett. 142B, 141 (1984) H.-A.Gustafsson, H.H.Gutbrod, B.Kolb, H.Lohner, B.Ludewigt, A.M.Poskanzer, T.Renner, H.Riedesel, H.G.Ritter, A.Warwick, H.Wieman Thermalization in High Energy Nuclear Collisions NUCLEAR REACTIONS Ca(40Ca, X), (40Ca, pX), E=400, 1050 MeV/nucleon; 93Nb(93Nb, X), (93Nb, pX), E=400, 650 MeV/nucleon; measured σ(θp, Ep), fragment yield isotropy vs charge multiplicity.
doi: 10.1016/0370-2693(84)91249-8
1982CA04 Phys.Lett. 109B, 419 (1982) L.C.Carraz, P.G.Hansen, A.Huck, B.Jonson, G.Klotz, A.Knipper, K.L.Kratz, C.Miehe, S.Mattsson, G.Nyman, H.Ohm, A.M.Poskanzer, A.Poves, H.L.Ravn, C.Richard-Serre, A.Schroder, G.Walter, W.Ziegert The 49K Beta Decay RADIOACTIVITY 49K [from U(p, X), E=600 MeV]; measured β-delayed En, In, nγ-coin, Eγ, Iγ, T1/2, β-activity; deduced β-strength function, Iβ, log ft, neutron branching ratio, (Qβ-B(n)) difference. 48,50,51K; measured neutron branching ratio, (Qβ-B(n)) difference. 48Ca deduced transitions.49Ca deduced levels, possible J, π, configurations.
doi: 10.1016/0370-2693(82)91104-2
1981BJ01 Nucl.Phys. A359, 1 (1981) T.Bjornstad, H.A.Gustafsson, P.G.Hansen, B.Jonson, V.Lindfors, S.Mattsson, A.M.Poskanzer, H.L.Ravn, the ISOLDE Collaboration Delayed Neutron Emission Probabilities of 9Li and 11Li RADIOACTIVITY 9,11Li [from U, Ta(3He, X), on-line mass separation]; measured βn-coin; 11Li measured T1/2, βγ-coin; deduced log ft, β-delayed neutron emission probability.
doi: 10.1016/0375-9474(81)90208-6
1981BJ03 Nucl.Phys. A366, 461 (1981) T.Bjornstad, H.A.Gustafsson, B.Jonson, P.O.Larsson, V.Lindfors, S.Mattsson, G.Nyman, A.M.Poskanzer, H.L.Ravn, D.Schardt The Decay of 8He RADIOACTIVITY 8He [from U(p, X), U(3He, X), chemical mass separation]; measured β-delayed En, In, βγ-coin, T1/2; deduced delayed neutron branching, log ft. Natural targets.
doi: 10.1016/0375-9474(81)90522-4
1981BJ04 Z.Phys. A303, 227 (1981) T.Bjornstad, H.-A.Gustafsson, B.Jonson, O.C.Jonsson, V.Lindfors, S.Mattsson, A.M.Poskanzer, H.L.Ravn, D.Schardt, the ISOLDE Collaboration Comparative Yields of Alkali Elements and Thallium form Uranium Irradiated with GeV Protons, 3He and 12C NUCLEAR REACTIONS U(p, X), E=600 MeV; U(3He, X), E=890 MeV; U(12C, X)E=936 MeV; measured absolute, comparative yields for 24,25,26,27,28,29,30,31,32,33,34Na, 37,38,42,43,44,45,46,47,48,49,50,51,52,53K, 184,185,186,187,188,190,191,193,195,197Tl, 202,203,204,205,206,207,208,209,210,211,212,213,219,220,221,222,224,225,226,228,229,230Fr. Activation technique, 4π plastic scintillator, β-counting. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0515. 1980AZ01 Phys.Lett. B96, 31 (1980) R.E.Azuma, T.Bjornstad, H.A.Gustafsson, P.G.Hansen, B.Jonson, S.Mattsson, G.Nyman, A.M.Poskanzer, H.L.Ravn, and the ISOLDE Collaboration Beta-Delayed Three-Neutron Radioactivity of 11Li RADIOACTIVITY 11Li [from U(p, X), E=600 MeV]; measured β-delayed, one-, two-, three-neutron emission intensity In, relative two-, three-neutron branching ratios.
doi: 10.1016/0370-2693(80)90205-1
1980DE26 Phys.Lett. B94, 307 (1980) C.Detraz, M.Epherre, D.Guillemaud, P.G.Hansen, B.Jonson, R.Klapisch, M.Langevin, S.Mattsson, F.Naulin, G.Nyman, A.M.Poskanzer, H.L.Ravn, M. de Saint-Simon, K.Takahashi, C.Thibault, F.Touchard Beta-Delayed Two-Neutron Emission from 30,31,32Na RADIOACTIVITY 30,31,32Na [from U(p, X), E=660 MeV]; measured β-delayed nn(t), Eγ, Iγ; deduced two-neutron emission branching ratios.
doi: 10.1016/0370-2693(80)90884-9
1980SA09 Phys.Rev. C21, 1321 (1980) A.Sandoval, H.H.Gutbrod, W.G.Meyer, R.Stock, C.Lukner, A.M.Poskanzer, J.Gosset, J.-C.Jourdain, C.H.King, G.King, Nguyen Van Sen, G.D.Westfall, K.L.Wolf Spectra of p, d, and t from Relativistic Nuclear Collisions NUCLEAR REACTIONS U(20Ne, p), (20Ne, d), (20Ne, t), E=0.24, 0.39, 1.04, 2.1 GeV/nucleon; U, Ca(40Ar, p), (40Ar, d), (40Ar, t), Au, Ag, Al(20Ne, p), (20Ne, d), (20Ne, t), U, Al(α, p), (α, d), (α, t), E=390 MeV/nucleon; U, Ca(40Ar, p), (40Ar, d), (40Ar, t), U(α, p), (α, d), (α, t), U(p, p), (p, d), (p, t), E=1.04 GeV/nucleon; measured σ(E, θ).
doi: 10.1103/PhysRevC.21.1321
1979WO03 Phys.Rev.Lett. 42, 1448 (1979) K.L.Wolf, H.H.Gutbrod, W.G.Meyer, A.M.Poskanzer, A.Sandoval, R.Stock, J.Gosset, C.H.King, G.King, Nguyen Van Sen, G.D.Westfall Pion Production in the 40Ar + 40Ca Reaction at 1.05 GeV/Nucleon NUCLEAR REACTIONS 40Ca(40Ar, π+), E=1.05 GeV/nucleon; measured production σ. Cascade, thermal model inadequate.
doi: 10.1103/PhysRevLett.42.1448
1978WE04 Phys.Rev. C17, 1368 (1978) G.D.Westfall, R.G.Sextro, A.M.Poskanzer, A.M.Zebelman, G.W.Butler, E.K.Hyde Energy Spectra of Nuclear Fragments Produced by High Energy Protons NUCLEAR REACTIONS C, Al(p, X), E=2.1, 4.9 GeV; Ag, U(p, X), E=4.9 GeV; measured σ(Z, θ).
doi: 10.1103/PhysRevC.17.1368
1977BU11 Phys.Rev.Lett. 38, 1380 (1977) G.W.Butler, D.G.Perry, L.P.Remsberg, A.M.Poskanzer, J.B.Natowitz, F.Plasil Observation of the New Nuclides 27Ne, 31Mg, 32Mg, 34Al, and 39P NUCLEAR REACTIONS U(p, X), E=800 MeV; measured yields for 27Ne, 31,32Mg, 34Al, 39P.
doi: 10.1103/PhysRevLett.38.1380
1977GO07 Phys.Rev. C16, 629 (1977) J.Gosset, H.H.Gutbrod, W.G.Meyer, A.M.Poskanzer, A.Sandoval, R.Stock, G.D.Westfall Central Collisions of Relativistic Heavy Ions NUCLEAR REACTIONS U(20Ne, X), E=0.25, 0.4, 2.1 GeV/nucleon; U(α, X), E=400 MeV/nucleon; 27Al(20Ne, X), E=2.1 GeV/nucleon; U(12C, X), E=2.1 GeV/nucleon; measured σ(θ) for proton, light nuclei production.
doi: 10.1103/PhysRevC.16.629
1976GU13 Phys.Rev.Lett. 37, 667 (1976) H.H.Gutbrod, A.Sandoval, P.J.Johansen, A.M.Poskanzer, J.Gosset, W.G.Meyer, G.D.Westfall, R.Stock Final-State Interactions in the Production of Hydrogen and Helium Isotopes by Relativistic Heavy Ions of Uranium NUCLEAR REACTIONS U(20Ne, X), E=250, 400, 2100 MeV/nucleon; U(α, X), E=400 MeV/nucleon; measured σ(Ep, θ), σ(Ed, θ), σ(Et, θ), σ(E(3He), θ), σ(Eα, θ).
doi: 10.1103/PhysRevLett.37.667
1976WE30 Phys.Rev.Lett. 37, 1202 (1976) G.D.Westfall, J.Gosset, P.J.Johansen, A.M.Poskanzer, W.G.Meyer, H.H.Gutbrod, A.Sandoval, R.Stock Nuclear Fireball Model for Proton Inclusive Spectra from Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS U(α, X), (20Ne, X), E=0.25, 0.4, 2.1 GeV/nucleon; analyzed available data; deduced a simple model for the emission of nucleons with velocities intermediate between those of the target and projectile, σ(θ, E).
doi: 10.1103/PhysRevLett.37.1202
1975PO14 Phys.Rev.Lett. 35, 1701 (1975) A.M.Poskanzer, R.G.Sextro, A.M.Zebelman, H.H.Gutbrod, A.Sandoval, R.Stock Search for Fragment Emission from Nuclear Shock Waves NUCLEAR REACTIONS Ag, U(p, X), E=2.7 GeV; Ag, U(α, X), E=0.7-1.05 GeV/nucleon; Ag, U(16O, X), E=1.05 GeV/nucleon; measured σ(E(3He), θ), σ(Eα, θ).
doi: 10.1103/PhysRevLett.35.1701
1975TH08 Phys.Rev. C12, 644 (1975) C.Thibault, R.Klapisch, C.Rigaud, A.M.Poskanzer, R.Prieels, L.Lessard, W.Reisdorf Direct Measurement of the Masses of 11Li and 26-32Na with an on-Line Mass Spectrometer RADIOACTIVITY 11Li; measured neutron binding energy, delayed neutron branching ratio, T1/2; deduced log ft. ATOMIC MASSES 11Li, 26,27,28,29,30,31,32Na; measured mass excesses.
doi: 10.1103/PhysRevC.12.644
1975ZE01 Phys.Rev. C11, 1280 (1975) A.M.Zebelman, A.M.Poskanzer, J.D.Bowman, R.G.Sextro, V.E.Viola, Jr. Fragments from Uranium Irradiated by 2.1 GeV/Nucleon Deuterons and Alpha Particles NUCLEAR REACTIONS U(p, X), E=4.9 GeV; U(α, X), E=2.1 GeV/nucleon; measured σ(fragment mass, θ) for A=6-12.
doi: 10.1103/PhysRevC.11.1280
1974BO05 Phys.Rev. C9, 836 (1974) J.D.Bowman, A.M.Poskanzer, R.G.Korteling, G.W.Butler Detection of Neutron-Excess Isotopes of Low-Z Elements Produced in High-Energy Nuclear Reactions NUCLEAR REACTIONS U(p, X), E=4.8 GeV; measured σ(fragment mass). 13Li, 14Be, 17,19B, 18,19,20C, 22N deduced yields.
doi: 10.1103/PhysRevC.9.836
1973BO30 Phys.Rev.Lett. 31, 614 (1973) J.D.Bowman, A.M.Poskanzer, R.G.Korteling, G.W.Butler Discovery of Two Isotopes, 14Be and 17B, at the Limits of Particle Stability NUCLEAR REACTIONS, Fission U(p, F), E=4.8 GeV; measured yields. 6,7,8,9,11,13Li, 7,9,10,11,12Be, 8,10,11,12,13,14,15B deduced nothing. 14Be, 17B deduced J, π, t.
doi: 10.1103/PhysRevLett.31.614
1973KL10 Phys.Rev.Lett. 31, 118 (1973) R.Klapisch, R.Prieels, C.Thibault, A.M.Poskanzer, C.Rigaud, E.Roeckl On-Line Mass-Spectrometric Measurement of the Masses of Neutron-Rich Sodium Isotopes ATOMIC MASSES 27,28,29,30Na; measured mass.
doi: 10.1103/PhysRevLett.31.118
1972KL04 Phys.Rev.Lett. 29, 1254 (1972) R.Klapisch, C.Thibault, A.M.Poskanzer, R.Prieels, C.Rigaud, E.Roeckl Half-Life of the New Isotope 32Na; Observation of 33Na and Other New Isotopes Produced in the Reaction of High-Energy Protons on U RADIOACTIVITY 26,27,28,29,30,31,32,33Na; measured T1/2. NUCLEAR REACTIONS U(p, X), E=24 GeV; measured σ. 48,49,50K, 227,228Fr deduced existence.
doi: 10.1103/PhysRevLett.29.1254
1972TR01 Phys.Rev. C5, 222 (1972) B.L.Tracy, J.Chaumont, R.Klapisch, J.M.Nitschke, A.M.Poskanzer, E.Roeckl, C.Thibault Rb and Cs Isotopic Cross Sections from 40-60-Mev-Proton Fission of 238U, 232Th, and 235U NUCLEAR REACTIONS, Fission 232Th, 235,238U(p, F), E=40-60 MeV; measured σ(E), Rb, Cs isotopic mass distributions; deduced average neutron number.
doi: 10.1103/PhysRevC.5.222
1972WE12 Nucl.Phys. A192, 517 (1972) L.Westgaard, B.R.Erdal, P.G.Hansen, E.Kugler, G.Sletten, S.Sundell, T.Fritsch, E.Henrich, W.Theis, G.K.Wolf, J.Camplan, R.Klapisch, R.Meunier, A.M.Poskanzer, C.Stephan, J.Tys Search for Super-Heavy Elements Produced by Secondary Reactions in Uranium NUCLEAR REACTIONS U(p, X), E=24 GeV; measured production σ for 236,238,239Pu, 241Am, 242Cm, 248Cf; deduced upper limits for super-heavy element production.
doi: 10.1016/0375-9474(72)90088-7
1971HY01 Phys.Rev. C4, 1759 (1971) E.K.Hyde, G.W.Butler, A.M.Poskanzer Characteristics of Fragments Produced in the Interaction of 5.5-GeV Protons with Silver NUCLEAR REACTIONS Ag(p, X), E=5.5 GeV; measured fragment energy spectra.
doi: 10.1103/PhysRevC.4.1759
1971PO01 Phys.Rev. C3, 882 (1971) A.M.Poskanzer, G.W.Butler, E.K.Hyde Fragment Production in the Interaction of 5.5-GeV Protons with Uranium NUCLEAR REACTIONS, Fission U(p, F), E=5.5 GeV; measured σ(E(fragment), θ(fragment)).
doi: 10.1103/PhysRevC.3.882
1971TR02 Phys.Lett. 34B, 277 (1971) B.L.Tracy, J.Chaumont, R.Klapisch, J.M.Nitschke, A.M.Poskanzer, E.Roeckl, C.Thibault Half-Lives of the New Isotopes 99Rb, 98Sr and 145-146Cs RADIOACTIVITY 96,97,98,99Rb, 98,97Sr, 97,98Y, 145,146Cs; measured T1/2.
doi: 10.1016/0370-2693(71)90603-4
1970BU22 Nucl.Instrum.Methods 89, 189 (1970) G.W.Butler, A.M.Poskanzer, D.A.Landis Identification of Nuclear Fragments by a Combined Time-of-Flight, Δ E-E Technique NUCLEAR REACTIONS U(p, X), E=5.5 GeV; measured fragment mass spectra. 18C, 20N deduced particle stability.
doi: 10.1016/0029-554X(70)90822-0
1968PO04 Phys.Letters 27B, 414 (1968) A.M.Poskanzer, G.W.Butler, E.K.Hyde, J.Cerny, D.A.Landis, F.S.Goulding Observation of the New Isotope 17C Using a Combined Time-of-Flight Particle-Identification Technique NUCLEAR STRUCTURE 17C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90222-0
1968PO11 Phys.Rev. 168, 1331 (1968) A.M.Poskanzer, J.B.Cumming, L.P.Remsberg Al27(p, pπ+)Mg27 Reaction from 0.6 to 28 GeV NUCLEAR REACTIONS 27Al(p, X)27Mg, E=0.6-28 GeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties.
doi: 10.1103/PhysRev.168.1331
1967ES02 Phys.Rev. 156, 1094 (1967) R.A.Esterlund, R.McPherson, A.M.Poskanzer, P.L.Reeder Beta-Delayed Protons from Ne17 NUCLEAR STRUCTURE 17Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.156.1094
1966ES04 BNL-10520 (1966) R.A.Esterlund, R.McPherson, A.M.Poskanzer, P.L.Reeder Beta-Delayed Protons from Ne17 NUCLEAR STRUCTURE 17Ne; measured not abstracted; deduced nuclear properties.
1966PO09 Phys.Rev.Letters 17, 1271 (1966) A.M.Poskanzer, S.W.Cosper, E.K.Hyde, J.Cerny New Isotopes: 11Li, 14B, and 15B NUCLEAR STRUCTURE 11Li, 15B, 14B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.1271
1966PO12 Phys.Rev. 152, 995 (1966) A.M.Poskanzer, R.McPherson, R.A.Esterlund, P.L.Reeder Beta-Delayed Protons from Ar33, Ca37, and Ti41 NUCLEAR STRUCTURE 41Ti, 37Ca, 33Ar; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.152.995
1966RE07 Phys.Rev. 147, 781 (1966) P.L.Reeder, A.M.Poskanzer, R.A.Esterlund, R.McPherson Beta-Delayed Protons from Si25 NUCLEAR STRUCTURE 25Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.147.781
1966RE15 Phys.Rev. 147, 781 (1966) P.L.Reeder, A.M.Poskanzer, R.A.Esterlund, R.McPherson Beta-Delayed Protons from Si25 RADIOACTIVITY 25Si(β+) [from 24Mg(3He, 2n), E=32 MeV]; measured β-delayed Ep, Ip, logft. 25Al; deduced levels, J, π.
doi: 10.1103/PhysRev.147.781
1965DO13 Phys.Rev. 139, B1513 (1965) I.Dostrovsky, R.Davis, Jr., A.M.Poskanzer, P.L.Reeder Cross Sections for the Production of Li9, C16, and N17 in Irradiations With GeV-Energy Protons RADIOACTIVITY 9Li, 17N; measured T1/2.
doi: 10.1103/PhysRev.139.B1513
1965MC09 Phys.Rev. 140, B1513 (1965) R.McPherson, R.A.Esterlund, A.M.Poskanzer, P.L.Reeder Oxygen-13 NUCLEAR STRUCTURE 13O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B1513
1965PO03 Phys.Rev. 138, B18 (1965) A.M.Poskanzer, P.L.Reeder, I.Dostrovsky New Delayed-Neutron-Emitting Isotope: Be12 NUCLEAR STRUCTURE 13B, 12Be, 8Be, 8He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B18
1965PO06 Phys.Rev.Letters 15, 1030 (1965) A.M.Poskanzer, R.A.Esterlund, R.McPherson Decay of He8 NUCLEAR STRUCTURE 8He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.15.1030
1964PO06 Phys.Rev. 133, B1507 (1964) A.M.Poskanzer, L.P.Remsberg, S.Katcoff, J.B.Cumming C12(p, pn)C11 cross section at 1.0 GeV NUCLEAR REACTIONS 12C(p, x), E=1 GeV; measured products, 11C; deduced σ, σ(E). Data were imported from EXFOR entry O0429.
doi: 10.1103/PhysRev.133.B1507
1964RE08 Phys.Rev.Letters 13, 767 (1964) P.L.Reeder, A.M.Poskanzer, R.A.Esterlund New Delayed-Proton Emitters: Ti41, Ca37, and Ar33 NUCLEAR STRUCTURE 33Ar, 37Ca, 41Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.767
1964SC02 Phys.Rev. 133, B1 (1964) A.Schwarzschild, A.M.Poskanzer, G.T.Emery, M.Goldhaber Another Search for H5 NUCLEAR STRUCTURE 7Li, 5H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B1
1962CU10 Phys.Rev. 127, 950 (1962) J.B.Cumming, G.Friedlander, J.Hudis, A.M.Poskanzer Spallation of aluminum by 28-GeV protons NUCLEAR REACTIONS C(p, x), 27Al(p, x), E=28 GeV; measured products, 7Be, 11C, 13N, 15O, 18F, 22Na, 24Na, 24Ne, 27Mg; deduced σ, σ(E). Data were imported from EXFOR entry C0261.
doi: 10.1103/PhysRev.127.950
1962CU11 Phys.Rev. 128, 2392 (1962) J.B.Cumming, J.Hudis, A.M.Poskanzer, S.Kaufman Al27(p, 3pn)Na24/C12(p, pn)C11 cross section ratio in the GeV region NUCLEAR REACTIONS 12C(p, np), 12C(p, x), 27Al(p, n3p), 27Al(p, x), E=420 MeV-16.9 GeV; measured products, 24Na, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry C0224.
doi: 10.1103/PhysRev.128.2392
1961PA22 Phys.Rev. 123, 647 (1961) Spallation of Uranium and Thorium Nuclei with Bev-Energy Protons RADIOACTIVITY 237Pa; measured nothing;analyzed activation data; deduced T1/2.
doi: 10.1103/PhysRev.123.647
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