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NSR database version of May 20, 2024.

Search: Author = R.Kossakowski

Found 17 matches.

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1998AB47      Phys.Lett. 444B, 516 (1998)

M.C.Abreu, C.Baglin, A.Baldit, M.Bedjidian, P.Bordalo, A.Bussiere, P.Busson, J.Castor, T.Chambon, C.Charlot, B.Chaurand, D.Contardo, E.Descroix, A.Devaux, O.Drapier, B.Espagnon, J.Fargeix, R.Ferreira, F.Fleuret, P.Force, L.Fredj, J.Gago, C.Gerschel, P.Gorodetzky, J.Y.Grossiord, A.Guichard, J.P.Guillaud, R.Haroutunian, D.Jouan, L.Kluberg, R.Kossakowski, G.Landaud, C.Lourenco, R.Mandry, F.Ohlsson-Malek, J.R.Pizzi, C.Racca, S.Ramos, A.Romana, P.Saturnini, S.Silva, P.Sonderegger, X.Tarrago, J.Varela, F.Vazeille, and the NA38 Collaboration

Charmonia Production in 450 GeV/c Proton Induced Reactions

NUCLEAR REACTIONS C, 27Al, Cu, W(p, X), E at 450 GeV/c; measured dimuon mass, transverse momentum, rapidity spectra; deduced J/ψ, ψ' production σ.

doi: 10.1016/S0370-2693(98)01398-7
Citations: PlumX Metrics

1997LI01      Nucl.Phys. A612, 53 (1997)

P.Liaud, K.Schreckenbach, R.Kossakowski, H.Nastoll, A.Bussiere, J.P.Guillaud, L.Beck

The Measurement of the Beta Asymmetry in the Decay of Polarized Neutrons

RADIOACTIVITY 1n(β-); measured β asymmetry; deduced g(A)/g(V). Cold polarized neutrons. Standard model.

doi: 10.1016/S0375-9474(96)00325-9
Citations: PlumX Metrics

1995SC20      Phys.Lett. 349B, 427 (1995)

K.Schreckenbach, P.Liaud, R.Kossakowski, H.Nastoll, A.Bussiere, J.P.Guillaud

A New Measurement of the Beta Emission Asymmetry in the Free Decay of Polarized Neutrons

RADIOACTIVITY 1n(β-); measured β-asymmetry coefficient; deduced g(A)/g(V), g(V), g(A). Cold polarized neutrons, helium filled TPC.

doi: 10.1016/0370-2693(95)00228-D
Citations: PlumX Metrics

1989KO39      Nucl.Phys. A503, 473 (1989)

R.Kossakowski, P.Grivot, P.Liaud, K.Schreckenbach, G.Azuelos

Neutron Lifetime Measurement with a Helium-Filled Time Projection Chamber

RADIOACTIVITY 1n(β-); measured T1/2. Pulsed neutron beam, neutron decay and flux measurement in helium-filled time projection chamber.

doi: 10.1016/0375-9474(89)90246-7
Citations: PlumX Metrics

1989SC37      Nucl.Instrum.Methods Phys.Res. A284, 120 (1989)

K.Schreckenbach, G.Azuelos, P.Grivot, R.Kossakowski, P.Liaud

Neutron Decay Measurements with a Helium-Filled Time Projection Chamber

RADIOACTIVITY 1n(β-); measured T1/2. In-beam electron detection, free neutrons, helium-filled time projection chamber.

doi: 10.1016/0168-9002(89)90262-3
Citations: PlumX Metrics

1986BA63      Z.Phys. A325, 399 (1986)

V.Barci, H.El-Samman, A.Gizon, J.Gizon, R.Kossakowski, B.M.Nyako, T.Vertse, S.Elfstrom, D.Jerrestam, W.Klamra, Th.Lindblad, T.Bengtsson

Effective Moment of Inertia in 132Ce, 134Nd and 136Nd

NUCLEAR STRUCTURE 132Ce, 134,136Nd; calculated effective moments of inertia. Cranking Nilsson-Strutinsky model.

NUCLEAR REACTIONS 96Zr, 98,100Mo(40Ar, X), E=160-189 MeV; measured continuum Eγ, Iγ, σ(Eγ, E), γ(θ). 132Ce, 134,136Nd deduced moments of inertia. NaI(Tl) detectors. Cranking Nilsson-Strutinsky model.

1986KO05      Phys.Rev. C33, 1514 (1986)

R.Kossakowski, S.Andre, J.Genevey, A.Gizon, V.Barci, D.Barneoud, A.Charvet, C.Foin, J.Salicio

Incomplete Mass Transfer in 12C and 14N Reactions on Medium-Heavy Targets at 15 and 30 MeV/nucleon

NUCLEAR REACTIONS 141Pr, 144,150,152,154Sm, 174Yb(14N, X), E=15, 30 MeV/nucleon; 144,150Sm(12C, X), E=30 MeV/nucleon; measured evaporation residue mass, charge distributions; deduced average mass, charge. Delayed γ-emisssion technique.

doi: 10.1103/PhysRevC.33.1514
Citations: PlumX Metrics

1985CH12      Z.Phys. A320, 605 (1985)

A.Charvet, R.Beraud, R.Duffait, T.Ollivier, M.Meyer, R.Kossakowski, S.Andre, D.Barneoud, C.Foin, J.Genevey, A.Gizon, J.Treherne

On-Line γ-Ray Investigation of the 14N + 27Al Reaction at 30 MeV/u

NUCLEAR REACTIONS 27Al(14N, X)30P/29Si/28Si/29Al/28Al/27Al/26Al/25Al/27Mg/26Mg/25Mg/24Mg/23Mg/22Mg/25Na/24Na/23Na/22Na/21Na/23Ne/22Ne/21Ne/20Ne/19Ne/21F/20F/19F/18F/17F/19O/18O/17O/16O/15O/16N/15N/14N/13C/12C/10B, E=30 MeV/nucleon; measured spectra; deduced production σ for residues.

doi: 10.1007/BF01411859
Citations: PlumX Metrics

1985EL08      Phys.Lett. 158B, 459 (1985)

H.El-Samman, V.Barci, A.Gizon, J.Gizon, R.Kossakowski, Th.Lindblad, T.Bengtsson

Effective Dynamic Moment of Inertia of 118Xe and 130Ba

NUCLEAR REACTIONS 112Sn(12C, xnyp), E=112 MeV; 122Sn(12C, 4n), E=80 MeV; measured γ-multiplicity, sum spectra. 118Xe, 130Ba deduced effective moment of inertia.

doi: 10.1016/0370-2693(85)90794-4
Citations: PlumX Metrics

1985KO30      Phys.Rev. C32, 1612 (1985)

R.Kossakowski, J.Jastrzebski, P.Rymuza, W.Skulski, A.Gizon, S.Andre, J.Genevey, J.Gizon, V.Barci

Heavy Residues following 5-10 MeV/Nucleon 12C- and 14N- Induced Reactions on Sm and Pr Targets

NUCLEAR REACTIONS, ICPND 147Sm, 141Pr(12C, X), E=82-110 MeV; 147Sm(12C, X), E=90-110 MeV; 154,150Sm(12C, X), E=90, 110 MeV; 152Sm(12C, X), E=71-110 MeV; 144Sm(14N, X), E=80-107 MeV; 147,150,152Sm(14N, X), E=80-120 MeV; 141Pr(14N, X), E=68-120 MeV; measured Eγ, Iγ; deduced fusion σ(E). 144,147Sm(14N, xn), E=80-120 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 153,154,155,156,157Tm deduced levels. 141Pr(14N, 3n), (14N, 4n), (14N, 5n), (14N, 6n), (14N, 7n), (14N, 2np), (14N, 3np), (14N, 4np), (14N, 5np), (14N, 6np), E=threshold-120 MeV; measured residuals production σ(E).

doi: 10.1103/PhysRevC.32.1612
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0366.

1984BA36      ATOMKI Kozlem. 26, 32 (1984)

V.Barci, H.El-Samman, A.Gizon, J.Gizon, R.Kossakowski, Th.Lindblad

The Effective Moment of Inertia of 118Xe and 130Ba

NUCLEAR REACTIONS 112,122Sn(12C, xnyp), E=80, 112 MeV; measured Eγ, Iγ, sum spectra. 118Xe, 130Ba deduced effective moment of inertia.

1984EL07      ATOMKI Kozlem. 26, 30 (1984)

H.El-Samman, V.Barci, T.Bengtsson, A.Gizon, J.Gizon, L.Hildingsson, D.Jerrestam, W.Klamra, R.Kossakowski, G.A.Leander, Th.Lindblad

Collective Moment of Inertia of 118,122Xe and 128,130Ba

NUCLEAR REACTIONS 112,117,122Sn, 123Sb(12C, xnyp), E not given; measured γγ-coin, energy correlations. 122,118Xe, 128,130Ba deduced dynamic moment of inertia.

1984EL08      Nucl.Phys. A427, 397 (1984)

H.El-Samman, V.Barci, A.Gizon, J.Gizon, L.Hildingsson, D.Jerrestam, W.Klamra, R.Kossakowski, Th.Lindblad, T.Bengtsson, G.A.Leander

On the Difference of the Dynamic Moment of Inertia I(2) Band for Xe and Ba Nuclei

NUCLEAR REACTIONS 112,117,112Sn(12C, X), E=80-118 MeV; 123Sb(12C, X), E=118 MeV; measured γγ-coin, γ-ray multiplicity; deduced γγ-energy correlation matrices. 118,122Xe, 128,130Ba deduced dynamic I(2) band moment of inertia.

doi: 10.1016/0375-9474(84)90091-5
Citations: PlumX Metrics

1982AN13      Z.Phys. A308, 181 (1982)

S.Andre, V.Barci, D.Barneoud, R.Beraud, A.Charvet, H.El Samman, J.Genevey, A.Gizon, J.Gizon, R.Kossakowski, J.Treherne, B.Weiss

On Line γ-Ray Emission following 30 MeV/A 12C Induced Reactions on some Medium-Heavy Targets

NUCLEAR REACTIONS 92Mo, 122Te, 150Sm, 174Yb(12C, X)84Y/86Y/88Zr/88Nb/90Mo/91Mo/112Sn/112Sb/113Sb/114Te/115Te/116Te/117Te/119I/118Xe/120Xe/140Nd/140Pm/140Sm/148Sm/142Eu/145Eu/146Eu/147Eu/148Eu/145Gd/147Gd/148Gd/148Tb/161Yb/162Yb/164Yb, E=30 MeV/nucleon; measured γ(t); deduced residuals production σ. 148,147Gd, 140Nd, 112Sn deduced isomer T1/2, J, π. 116Te, 118Xe, 162Yb deduced levels, rotational bands. Enriched targets, in-beam spectroscopy.

doi: 10.1007/BF01413009
Citations: PlumX Metrics

1981DR07      Z.Phys. A302, 361 (1981)

S.Drissi, S.Andre, J.Genevey, V.Barci, A.Gizon, J.Gizon, J.A.Pinston, J.Jastrzebski, R.Kossakowski, Z.Preibisz

Identification and Structure of Yrast Levels in the N = 89 Odd-Odd 158Tm Nucleus

NUCLEAR REACTIONS 150Sm(14N, xnp), E=80-120 MeV; measured production σ(E) for 157,158,159Er, 158Tm. Activation technique.

RADIOACTIVITY 158Tm [from 150Sm(14N, 6n), E=107 MeV]; measured Eγ, Iγ, γγ-coin, γγ(t); deduced isomer, T1/2, yrast levels, rotational bands, J, π.

doi: 10.1007/BF01414270
Citations: PlumX Metrics

1981GI12      Z.Phys. A301, 67 (1981)

J.Gizon, A.Gizon, S.Andre, J.Genevey, J.Jastrzebski, R.Kossakowski, M.Moszynski, Z.Preibisz

High Spin Levels in 151Ho

NUCLEAR REACTIONS 141Pr(16O, 6n), E=101-131 MeV; 144Sm(12C, 4np), E=82-110 MeV; measured Eγ, Iγ, linear polarization, σ(Eγ, E), γ(θ), γγ-coin, γγ(t). 151Ho deduced levels, J, π, T1/2, δ, configuration, γ-multiplicity. Enriched target, Ge(Li) detectors.

doi: 10.1007/BF01412465
Citations: PlumX Metrics

1980JA16      Phys.Lett. B97, 50 (1980)

J.Jastrzebski, R.Kossakowski, J.Lukasiak, M.Moszynski, Z.Preibisz, S.Andre, J.Genevey, A.Gizon, J.Gizon

Unambiguous Identification and Properties of High Isomers in Nuclei Close to N=82

NUCLEAR REACTIONS 141Pr, 144,147Sm(12C, X), (14N, X), (16O, X), E=70-130 MeV; measured Eγ, Iγ, γγ-coin, delayed γ-multiplicity, γ(t). 151,152,153Er, 150,151,152,153Ho, 149Dy, 148Tb deduced levels, T1/2.

doi: 10.1016/0370-2693(80)90544-4
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