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1993BE13 Acta Phys.Pol. B24, 451 (1993)

P.Bednarczyk, E.Bozek, B.Fornal, M.Lach, A.Maj, W.Meczynski, T.Pawlat, J.Styczen

Cross Section Ratio for pn and d Emission as a Probe of Level Density for Light-Medium Nuclei

NUCLEAR REACTIONS ⁵¹V, ⁵⁹Co, ⁵⁴Fe(α, xp), (α, xd), (α, xα), E=26.5 MeV; measured (particle)γ-coin, particle spectra; deduced σ(pn)/σ(d), dependence on level density. Evaporation code analysis.

1993DU04 Phys.Rev. C47, 2043 (1993)

G.Duchene, P.Romain, F.A.Beck, Ph.Benet, D.Disdier, B.Haas, B.Lott, V.Rauch, F.Scheibling, J.P.Vivien, S.K.Basu, E.Bozek, K.Zuber, D.Di Gregorio, J.Fernandez-Niello

Angular Momentum Distributions for ¹⁶O + ¹⁴⁴Nd

NUCLEAR REACTIONS, ICPND ¹⁴⁴Nd(¹⁶O, X), E=67-90 MeV; measured fusion σ(E), γ-multiplicity. Model comparison. Off-line residual X-ray emission detection.

doi: 10.1103/PhysRevC.47.2043
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1990HA25 Phys.Lett. 245B, 13 (1990)

B.Haas, J.P.Vivien, S.K.Basu, F.A.Beck, Ph.Benet, T.Byrski, D.Curien, G.Duchene, C.Gehringer, H.Kluge, J.C.Merdinger, P.Romain, D.Santos, S.Flibotte, J.Gascon, P.Taras, E.Bozek, K.Zuber

Feeding of the Superdeformed Yrast Band in ¹⁴⁹Gd

NUCLEAR REACTIONS ¹²⁴Sn(³⁰Si, 5n), E=150-160 MeV; measured γ-spectra. ¹⁴⁹Gd deduced superdeformed yrast band relative Iγ.

doi: 10.1016/0370-2693(90)90156-Z
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1990KR05 Phys.Lett. 245B, 17 (1990)

M.Kramer, B.Blank, E.Bozek, E.Ditzel, E.Kankeleit, G.Klotz-Engmann, C.Muntz, H.Oeschler, M.Rhein

On the Systematics of Positron Production in Elastic Heavy Ion Collisions

NUCLEAR REACTIONS ²⁰⁸Pb(²⁰⁸Pb, X), E=8.6 MeV/nucleon; ²³⁸U(²⁰⁸Pb, X), E=8.4 MeV/nucleon; measured γ-spectra, positron spectra; deduced atomic positron integral production probability.

doi: 10.1016/0370-2693(90)90157-2
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1989KR09 Phys.Rev. C40, 1662 (1989)

M.Kramer, B.Blank, E.Bozek, E.Ditzel, E.Kankeleit, G.Klotz-Engmann, C.Muntz, H.Oeschler, M.Rhein, P.Senger

δ-Electron Spectroscopy, a Tool to Study the Dynamics of Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁰⁸Pd, ¹⁶⁹Tm, ²⁰⁸Pb, ²³⁸U(²⁰⁸Pb, X), E=8.5 MeV/nucleon; measured (fragment e⁺)-, (fragment e^-)-, γ(fragment)-coin; deduced nuclear trajectories. Reaction models, dissipative collisions.

doi: 10.1103/PhysRevC.40.1662
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1989ZU01 Z.Phys. A332, 231 (1989)

K.Zuber, E.Bozek, F.A.Beck, P.Benet, T.Byrski, D.Curien, G.Duchene, C.Gehringer, B.Haas, A.Kreiner, J.C.Merdinger, P.Romain, J.P.Vivien

Non-Yrast States in ¹⁵²Dy Around 22(h-bar), the Region into which the Discrete Superdeformed Band Drains

NUCLEAR REACTIONS ¹²⁴Sn(³²S, 4n), E=132 MeV; measured γγ-coin. ¹⁵²Dy deduced levels, J, π, superdeformed band drainage.

1986BO05 Nucl.Phys. A451, 171 (1986)

E.Bozek, D.M.De Castro-Rizzo, S.Cavallaro, B.Delaunay, J.Delaunay, H.Dumont, A.D'Onofrio, M.-G.Saint-Laurent, L.Sperduto, F.Terrasi

De-Excitation of ^58,60,62Ni Compound Nuclei Formed via Symmetric and Asymmetric Entrance Channels

NUCLEAR REACTIONS, ICPND ⁴⁶Ti(¹²C, X), E(cm)=17.21-45.05 MeV; ³⁰Si(²⁸Si, X), E(cm)=25.79-43.9 MeV; ⁴⁸Ti(¹²C, X), E(cm)=16.43-46.18 MeV; ³⁰Si(³⁰Si, X), E(cm)=27.18-47.43 MeV; ⁵⁰Ti(¹²C, X), E(cm)=17.23-47.27 MeV; ⁴⁴Ca(¹⁸O, X), E(cm)=19.44-42.25 MeV; measured absolute residue production σ for ^57,56,55,59Co, ^{56,55,54,57,58,59,53}Fe, ^58,57,60,59Ni, ^{55,54,53,52,51}Mn, ^51,49,50V.

doi: 10.1016/0375-9474(86)90250-2
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1985HA03 Phys.Rev.Lett. 54, 398 (1985)

B.Haas, G.Duchene, F.A.Beck, T.Byrski, C.Gehringer, J.C.Merdinger, A.Nourredine, V.Rauch, J.P.Vivien, J.Barrette, S.Tobbeche, E.Bozek, J.Styczen, J.Keinonen, J.Dudek, W.Nazarewicz

Strong Angular Momentum Effects in Near-Barrier Fusion Reactions

NUCLEAR REACTIONS ¹⁴⁴Nd(¹⁶O, xn), ¹²³Sb(³⁷Cl, xn), ⁹⁶Zr(⁶⁴Ni, xn), ⁸⁰Se(⁸⁰Se, xn), E=tandem; measured σ for x=2-5, evaporation residue σ, average γ-multiplicities. ¹⁶⁰Er deduced near barrier angular momentum transfer entrance channel dependence. Ground state zero-point vibrations.

doi: 10.1103/PhysRevLett.54.398
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1984DE38 Nucl.Phys. A427, 151 (1984)

D.M.De Castro Rizzo, E.Bozek, S.Cavallaro, B.Delaunay, J.Delaunay, H.Dumont, M.G.Saint-Laurent, F.Terrasi

Fusion Excitation Functions near and below the Coulomb Barrier for Symmetric and Asymmetric Medium-Mass Systems

NUCLEAR REACTIONS, ICPND ^46,48,50Ti(¹²C, X), ⁴⁴Ca(¹⁸O, X), E(cm) ≈ 20-45 MeV; ^28,30Si(³⁰Si, X), E(cm) ≈ 25-45 MeV; measured fusion σ(E). ^48,50Ti(¹²C, ¹²C'), E=20-60 MeV; ⁴⁴Ca(¹⁸O, ¹⁸O'), E=30-60 MeV; measured inelastic σ(E); deduced barrier parameters. Hyperpure Ge, Ge(Li) detectors, in-beam γ-rays, rotating target. Zero-point motion, neck formation.

doi: 10.1016/0375-9474(84)90143-X
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1981DU21 Fizika(Zagreb) 13, Suppl.No.1, 64 (1981)

H.Dumont, E.Bozek, A.Brondi, B.Delaunay, J.Delaunay, A.D'Onofrio, D.Rizzo, M.G.Saint Laurent, F.Terrasi

Evidence for Massive Transfer Processes in the Reaction ⁴⁸Ti + ¹³C at 46 MeV

NUCLEAR REACTIONS ⁴⁸Ti(¹³C, X), E=46 MeV; measured (particle)γ-coin; deduced massive transfer process, production of ^52,51Cr, ⁵⁰V, ^49,48Ti, ^47,46Sc. ΔE-E telescopes.

1981RI13 Fizika(Zagreb) 13, Suppl.No.1, 53 (1981)

D.Rizzo, E.Bozek, B.Delaunay, J.Delaunay, A.D'Onofrio, H.Dumont, M.G.Saint Laurent, F.Terrasi

Excitation Functions of the Neutron Transfer and Inelastic Scattering for ¹³C on ⁴⁸Ti (25-60 MeV lab)

NUCLEAR REACTIONS ⁴⁸Ti(¹³C, ¹²C), (¹³C, ¹³C'), E=25-60 MeV; measured σ(E). In-beam γ-spectroscopy.

1980ME11 Nucl.Phys. A346, 281 (1980)

J.C.Merdinger, F.A.Beck, E.Bozek, T.Byrski, C.Gehringer, Y.Schutz, J.P.Vivien

Magnetic Moments of the I(π) = 10⁺ Isomers in Ce and Nd N = 80 Isotones

NUCLEAR REACTIONS ¹³⁰Te(¹²C, 4n), E=60 MeV; ¹²⁸Te(¹⁶O, 4n), E=70 MeV; measured Iγ(θ, H, t). ¹³⁸Ce, ¹⁴⁰Nd levels deduced g. Time differential perturbed angular distribution method, enriched targets.

doi: 10.1016/0375-9474(80)90501-1
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1979BE02 Phys.Rev.Lett. 42, 493 (1979)

F.A.Beck, E.Bozek, T.Byrski, C.Gehringer, J.C.Merdinger, Y.Schutz, J.Styczen, J.P.Vivien

Second Irregularity in the Yrast Line of ¹⁶⁰Yb

NUCLEAR REACTIONS ¹⁴⁸Sm(¹⁶O, 4nγ), E=95, 105 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, γγ(θ), oriented nuclei. ¹⁶⁰Yb deduced yrast states, second backbend.

doi: 10.1103/PhysRevLett.42.493
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1979ME01 Phys.Rev.Lett. 42, 23 (1979)

J.C.Merdinger, F.A.Beck, T.Byrski, C.Gehringer, J.P.Vivien, E.Bozek, J.Styczen

Yrast Isomers and Possible Oblate Shape in ¹⁵²Dy

NUCLEAR REACTIONS ¹⁴⁰Ce(¹⁶O, 4n), E=88 MeV; ¹⁴¹Pr(¹⁵N, 4n), E=80 MeV; measured Eγ, Iγ, γγ-coin, nγ(t). ¹⁵²Dy levels deduced E, J, π. Comparison with microscopic calculations.

doi: 10.1103/PhysRevLett.42.23
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1979ST13 Nucl.Phys. A327, 295 (1979)

J.Styczen, E.Bozek, T.Pawlat, Zb.Stachura, F.A.Beck, C.Gehringer, B.Haas, J.C.Merdinger, N.Schulz, P.Taras, M. Toulemonde, J.P.Vivien, A.Muller-Arnke

High-Spin States in ⁵⁰Ti, ⁵²Cr and ⁵⁴Fe

NUCLEAR REACTIONS ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr(α, 2nγ), E=24-33 MeV; measured Eγ, σ(E, θγ), linear polarization, γγ-coin, σ(θγ, t). ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe deduced levels, J, π, δ, T_1/2. Enriched targets.

doi: 10.1016/0375-9474(79)90261-6
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1979VI10 Phys.Lett. 85B, 325 (1979)

J.P.Vivien, Y.Schutz, F.A.Beck, E.Bozek, T.Byrski, C.Gehringer, J.C.Merdinger

Multipolarity of the Continuum γ-Rays in ¹⁵²Dy and ¹⁶⁰Er via Linear Polarisation Measurements

NUCLEAR REACTIONS ¹⁴⁰Ce(¹⁶O, 4n), E=89 MeV; ¹⁴⁸Nd(¹⁶O, 4n), E=85 MeV; measured γ-linear polarization γ(θ). ¹⁵²Dy, ¹⁶⁰Er deduced δ of continuum transitions.

doi: 10.1016/0370-2693(79)91263-2
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1978HA17 Phys.Rev.Lett. 40, 1313 (1978)

B.Haas, F.A.Beck, C.Gehringer, J.C.Merdinger, N.Schulz, P.Taras, M.Toulemonde, J.P.Vivien, J.Styczen, E.Bozek, Z.Stachura, T.Pawlat, A.Muller-Arnke

High-Spin Neutron Particle-Hole States in Even N = 28 Isotones

NUCLEAR REACTIONS ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr(α, 2nγ), E=27-33 MeV; measured σ(E, Eγ, θ), γγ-coin, γγ(θ), linear polarization, γ(t). ⁵⁰Ti deduced levels, J, π, λ, δ, B(λ). ⁵²Cr deduced configuration mixing.

doi: 10.1103/PhysRevLett.40.1313
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1976BO21 Nucl.Phys. A264, 151 (1976)

E.Bozek, C.Gehringer, J.C.Merdinger, K.Ogawa, J.P.Vivien

Magnetic Moment of the 2543 keV 7⁺ State in ⁴⁰K

NUCLEAR REACTIONS ²⁴Mg(¹⁹F, n2p), ²⁸Si(¹⁴N, 2p), E=42, 38 MeV; measured Iγ(θ, H). ⁴⁰K level deduced g-factor. Enriched ²⁴Mg target, Ge(Li) detectors.

doi: 10.1016/0375-9474(76)90150-0
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1976BO25 Nucl.Phys. A266, 457 (1976)

E.Bozek, B.Haas, B.Ingarden-Butkiewicz, K.Krolas, J.C.Merdinger, J.Styczen, J.P.Vivien

The g-Factor of the 6⁺ State in ⁵⁰Ti

NUCLEAR REACTIONS ⁴⁸Ca(α, 2n), E=26 MeV; measured γ(θ, H, t). ⁵⁰Ti level deduced g-factor. Enriched target.

doi: 10.1016/0375-9474(76)90369-9
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1975BO30 Nucl.Phys. A250, 257 (1975)

E.Bozek, C.Gehringer, C.Jaeger, J.C.Merdinger

Lifetime of the Second Excited State of ⁴³K

NUCLEAR REACTIONS ⁴⁰Ar(α, pγ), E=11.7 MeV; measured Eγ(θ), p-γ delay. ⁴³K level deduced T_1/2, J, π.

doi: 10.1016/0375-9474(75)90257-2
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1975BO44 Phys.Rev. C12, 1873 (1975)

E.Bozek, A.Z.Hrynkiewicz, J.C.Merdinger, J.P.Vivien

Hyperfine Interactions of Light Nuclei Recoil-Implanted into Iron

NUCLEAR REACTIONS ²⁷Al(¹⁶O, xnyp), ²⁸Si(¹⁴N, xnyp), E=30-35 MeV; measured Iγ(θ, H). ³⁷Ar, ^39,40,41K, ⁴¹Ca deduced hyperfine field parameters. Recoil implantation into Fe.

doi: 10.1103/PhysRevC.12.1873
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1975ME19 Phys.Lett. 59B, 38 (1975)

J.C.Merdinger, E.Bozek, C.Gehringer, Z.Stachura

The Unusual Strength of the 5.14 → 1.27 Mev, 2^- → 2⁺, Transition in ²²Ne

NUCLEAR REACTIONS ¹⁹F(α, pγ), E=9.9 MeV; measured pγ-coin, recoil distance DSA. ²²Ne level deduced T_1/2, E1 strength.

doi: 10.1016/0370-2693(75)90150-1
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1972CH25 Nucl.Phys. A191, 201 (1972)

A.Chevallier, E.Bozek, J.Chevallier, A.Pape, R.Armbruster

Etude des Niveaux de ³⁸Ar Formes dans la Reaction ³⁴S(α, γ)³⁸Ar

NUCLEAR REACTIONS ³⁴S(α, γ), E=3.6-4.8 MeV; measured σ(E, θ(γ), θ(γγ)). ³⁸Ar levels deduced J, π, γ-width. Enriched target.

doi: 10.1016/0375-9474(72)90602-1
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1972HA61 Nucl.Phys. A194, 249 (1972)

B.Haas, C.Gehringer, J.Chevallier, J.C.Merdinger, E.Bozek

Vies Moyennes des Niveaux a 53.2 keV et 111.5 keV et Moment Magnetique Du Niveau a 111.5 keV du ⁵⁸Co

NUCLEAR REACTIONS ⁵⁸Fe(p, nγ), E=3.9 MeV; measured Eγ, Iγ, nγ-delay, nγ(θ), pγ(θ, H), σ(θ(γ), H). ⁵⁸Co deduced levels J, T_1/2, g, γ-branching. Enriched target.

doi: 10.1016/0375-9474(72)91039-1
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1971CH52 Nucl.Phys. A176, 401 (1971)

A.Chevallier, E.Bozek, A.Pape, J.C.Sens, R.Armbruster, M.Langevin, J.Vernotte

Etude des Niveaux du ³²S Formes au Moyen de la Reaction ²⁸Si(α, γ)³²S

NUCLEAR REACTIONS ²⁸Si(α, γ), E=4.2-6.0 MeV; measured σ(E, θ), Doppler shift attenuation. ³²S deduced levels, J, π, γ-width, T_1/2. Enriched target.

doi: 10.1016/0375-9474(71)90278-8
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1969BO41 Acta Phys.Polon. 36, 1065 (1969)

E.Bozek, R.Broda, J.Golczewski, A.Z.Hrynkiewicz, R.Kulessa, M.Rybicka, S.Szymczyk, W.Walus

The g-Factor of the 184 keV State of ⁶⁷Zn

RADIOACTIVITY ⁶⁷Ga; measured γγ(θ, H), γγ-delay. ⁶⁷Zn level deduced g, T_1/2.

1969VE01 Nucl.Phys. A124, 350(1969)

J.Vernotte, M.Langevin, S.Fortier, E.Bozek, A.Chevallier, A.J.Pape, J.C.Sens

Desexcitation Similaire de Deux Niveaux Voisins Formes dans la Reaction ²⁸Si(α, γ)³²S

NUCLEAR REACTIONS ²⁸Si(α, γ), E=3.753, 3.820 MeV; measured σ(Eγ, θ), γγ(θ). ³²S levels deduced J, γ-mixing, γ-branching. Natural targets.

doi: 10.1016/0375-9474(69)90359-5
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1968BO41 Nucl.Instr.Methods 58, 325 (1968)

E.Bozek, A.Z.Hyrnkiewicz, G.Zapalski, R.Kulessa, W.Walus

Application of the Sum-Coincidence Method for g-Factor Measurements of Short-Lived Excited Nuclear States

NUCLEAR STRUCTURE ¹²⁴Te; measured not abstracted; deduced nuclear properties.

1968BO47 Nucl.Phys. A122, 184 (1968)

E.Bozek, R.Broda, J.Golczewski, A.Z.Hrynkiewicz, R.Kulessa, H.Niewodniczanski, M.Rybicka, W.Walus

Level Scheme of ¹⁴⁷Sm and g-Factors of its Two Lowest Excited States

RADIOACTIVITY ¹⁴⁷Eu [from 660 MeV protons on Ta]; measured Eγ, γγ-coin, γγ(θ), γγ(θ, H). ¹⁴⁷Sm levels deduced, T_1/2, g. Ge(Li) detector.

doi: 10.1016/0375-9474(68)90712-4
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1968BO50 Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.158 (1968)

E.Bozek, R.Broda, J.Golczewski, A.Z.Hrynkiewicz, R.Kulessa, S.Ogaza, M.Rybicka, W.Walus

g-Factors of the Excited States in ¹²⁴Te and ¹⁴⁷Sm

RADIOACTIVITY ¹²⁴Sb, ¹⁴⁷Eu; measured γγ(θ, H). ¹²⁴Te, ¹⁴⁷Sm levels deduced g.

1966GO19 Nucl.Phys. 85, 519 (1966)

S.Gorodetzky, N.Schulz, E.Bozek, A.Knipper

Periodes des Niveaux a 405 keV du ²¹¹Bi et a 377 keV du ⁵³Mn

RADIOACTIVITY ²¹¹Pb; measured γγ-delay. ²¹¹Bi level deduced T_1/2. ⁵³Cr(p, n), E = 3.1 MeV; measured γγ-delay. ⁵³Mn level deduced T_1/2. Natural target.

doi: 10.1016/0029-5582(66)90319-1
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1966GO20 Nucl.Phys. 85, 529 (1966)

S.Gorodetzky, N.Schulz, E.Bozek, A.C.Knipper

Application de la Technique des Coincidences Differees a la Mesure de Vies Moyennes Breves dans le ¹³¹Xe et le ¹⁴³Pr

RADIOACTIVITY ¹³¹I, ¹⁴³Ce, ¹⁹⁸Au; measured βγ-delay. ¹³¹Xe, ¹⁴³Pr, ¹⁹⁸Hg levels deduced T_1/2.

doi: 10.1016/0029-5582(66)90320-8
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1966GO21 Nucl.Phys. 85, 576 (1966)

S.Gorodetzky, F.A.Beck, R.Bertini, E.Bozek, A.Knipper

Distribution Angulaire, Correlations Angulaires et Polarisation Plane des Rayons Gamma de la Reaction ⁵³Cr(p, n)⁵³Mn

NUCLEAR REACTIONS ⁵³Cr(p, nγ), E = 3.15, 3.25 MeV; measured σ(Eγ, θ), γ-polarization (θ), γγ(θ). ⁵³Mn levels deduced, J, π, deltaγ. Natural, enriched targets.

doi: 10.1016/0029-5582(66)90323-3
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1964BO16 Phys. Letters 11, 63 (1964)

E.Bozek, A.Z.Hrynkiewicz, S.Ogaza, J.Styczen

HFS-Interaction of the Gd¹⁵⁵ Nucleus in the 87 keV Excited State

NUCLEAR STRUCTURE ¹⁵⁵Gd, ¹⁵⁵Tb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90260-4
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1963BO22 Phys.Letters 6, 89 (1963)

E.Bozek, A.Z.Hrynkiewicz, S.Ogaza, M.Rybicka, J.Styczen

The Half-Life of the 57 keV First Excited State in Pr¹⁴³

NUCLEAR STRUCTURE ¹⁴³Ce; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(63)90233-6
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1963BO24 PAN-231 (1963); Nucl.Sci.Abstr. 17, 3463, Abstr. 26460 (1963)