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NSR database version of April 11, 2024.

Search: Author = A.M.Poskanzer

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2000VO02      Phys.Lett. 474B, 27 (2000)

S.A.Voloshin, A.M.Poskanzer

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1998PO17      Phys.Rev. C58, 1671 (1998)

A.M.Poskanzer, S.A.Voloshin

Methods for Analyzing Anisotropic Flow in Relativistic Nuclear Collisions

doi: 10.1103/PhysRevC.58.1671
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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

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

Thermalization in High Energy Nuclear Collisions

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

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


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23273.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2151.


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0005.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0393.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0376.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2357.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0236.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0429.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0261.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0224.


1961PA22      Phys.Rev. 123, 647 (1961)

B.D.Pate, A.M.Poskanzer

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0369.


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