W. Meczynski
Polish Academy of Sciences
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Physics Letters B | 1993
J. Heese; K.H. Maier; H. Grawe; J. Grebosz; H. Kluge; W. Meczynski; M. Schramm; R. Schubart; K. M. Spohr; J. Styczen
Yrast states of the nuclei 188Pb and 186Pb located in the middle of the 82 < N < 126 shell have been studied for the first time in the reactions 156,154Gd (36Ar, 4n ) at 175 MeV. Gamma rays following the heavy-ion fusion-evaporation reactions were detected in coincidence with evaporation residues. Both nuclei exhibit a structure very different from the heavier even-even lead isotopes and show low-lying, probably prolate rotational bands.
Physics Letters B | 1988
W. Starzecki; G. de Angelis; B. Rubio; J. Styczen; K. Zuber; H. Güven; W. Urban; W. Gast; P. Kleinheinz; S. Lunardi; F. Soramel; A. Facco; C. Signorini; M. Morando; W. Meczynski; A. M. Stefanini; G. Fortuna
Abstract The N = 78 isotones 140Sm and 142Gd have been studied with α-particle- and HI-induced reactions. In both nuclei two close-lying 10+ isomers at ∼ 3.2 MeV have been established, and from the feeding E2 cascades they are characterized as the prolate ν h 11 2 −2 and the oblate π h 11 2 2 excitations. A third E2 cascade feeding into the 142Gd 8+ state is interpreted as the continuation of the collective ground state sequence that might assume the properties of a perfect deformed rotor for spins above 10.
Physical Review Letters | 2008
S. Leoni; G. Benzoni; N. Blasi; A. Bracco; S. Brambilla; F. Camera; A. Corsi; F. C. L. Crespi; P. Mason; B. Million; D. Montanari; M. Pignanelli; E. Vigezzi; O. Wieland; Masayuki Matsuo; Yoshifumi R. Shimizu; D. Curien; G. Duchêne; J. Robin; P. Bednarczyk; M. Castoldi; B. Herskind; M. Kmiecik; A. Maj; W. Meczynski; J. Styczen; M. Zieblinski; K. Zuber; A. Zucchiatti
The gamma decay associated with the warm rotation of the superdeformed nuclei 151Tb and 196Pb has been measured with the EUROBALL IV array. Several independent quantities provide a stringent test of the population and decay dynamics in the superdeformed well. A Monte Carlo simulation of the gamma decay based on microscopic calculations gives remarkable agreement with the data only assuming a large enhancement of the B(E1) strength for 1-2 MeV gamma rays, which may be related to the evidence for octupole vibrations in both mass regions.
European Physical Journal A | 2003
A. Maj; M. Kmiecik; M. Brekiesz; J. Grebosz; W. Meczynski; J. Styczen; M. Zieblinski; K. Zuber; A. Bracco; F. Camera; G. Benzoni; B. Million; N. Blasi; S. Brambilla; S. Leoni; M. Pignanelli; O. Wieland; B. Herskind; P. Bednarczyk; D. Curien; J.P. Vivien; E. Farnea; G. de Angelis; D. R. Napoli; J. Nyberg; M. Kicińska-Habior; C. M. Petrache; J. Dudek; K. Pomorski
Abstract.The
European Physical Journal A | 1990
M. Piiparinen; P. Kleinheinz; S. Lunardi; M. Ogawa; G. de Angelis; F. Soramel; W. Meczynski; J. Blomqvist
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NUCLEAR STRUCTURE AND DYNAMICS ’09: Proceedings of the International Conference | 2009
D. Montanari; S. Leoni; G. Benzoni; N. Blasi; A. Bracco; S. Brambilla; F. Camera; A. Corsi; F. C. L. Crespi; B. Million; R. Nicolini; O. Wieland; L. Corradi; G. de Angelis; F. Della Vedova; E. Fioretto; A. Gadea; B. Guiot; D. R. Napoli; R. Orlandi; F. Recchia; R. Silvestri; A. M. Stefanini; R. P. Singh; S. Szilner; J. J. Valiente-Dobón; D. Bazzacco; E. Farnea; S. M. Lenzi; S. Lunardi
-rays following the reaction 105 MeV 18O + 28Si have been measured using the EUROBALL IV, HECTOR and EUCLIDES arrays in order to investigate the predicted Jacobi shape transition. The high-energy
NUCLEAR STRUCTURE AND DYNAMICS 2012 | 2012
M. Matejska-Minda; P. Bednarczyk; B. Fornal; M. Ciemała; M. Kmiecik; M. Krzysiek; A. Maj; W. Meczynski; S. Myalski; J. Styczen; M. Zieblinski; G. de Angelis; T. Hüyük; C. Michelagnoli; E. Sahin; S. Aydin; E. Farnea; R. Menegazzo; F. Recchia; C. A. Ur; S. Brambilla; S. Leoni; D. Montanari; G. Jaworski; M. Palacz; R. Wadsworth
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Journal of Physics: Conference Series | 2011
S. Leoni; D. Montanari; G. Benzoni; N. Blasi; G. Bocchi; A. Bracco; F. Camera; A. Corsi; F. C. L. Crespi; B. Million; R. Nicolini; O. Wieland; L. Corradi; G. De Angelis; F. Della Vedova; E. Fioretto; A. Gadea; B. Guiot; D. R. Napoli; R. Orlandi; F. Recchia; R. Silvestri; A. M. Stefanini; R. P. Singh; S. Szilner; J. J. Valiente-Dobón; D. Bazzacco; E. Farnea; S. M. Lenzi; S. Lunardi
-ray spectrum from the GDR decay indicates the presence of large deformations in the hot 46Ti nucleus, in agreement with new theoretical calculations based on the rotating liquid-drop model.
FRONTIERS IN NUCLEAR STRUCTURE, ASTROPHYSICS, AND REACTIONS (FINUSTAR 3) | 2011
D. Montanari; S. Leoni; G. Benzoni; N. Blasi; G. Bocchi; A. Bracco; S. Brambilla; F. Camera; A. Corsi; F. C. L. Crespi; B. Million; R. Nicolini; O. Wieland; L. Corradi; G. De Angelis; F. Della Vedova; E. Fioretto; A. Gadea; B. Guiot; D. R. Napoli; R. Orlandi; F. Recchia; R. Silvestri; A. M. Stefanini; R. P. Singh; S. Szilner; J. J. Valiente-Dobón; D. Bazzacco; E. Farnea; S. M. Lenzi
Through (α, 4n) and (τ, 3n) reactions the high-spin states in the two-neutron nucleus148Gd were populated up toIπ=21− at 7.2 MeV, including numerous states above the yrast line. The148Gd energy spectrum is interpreted in terms of the spherical shell model. Identification of the (νf7/2i1 3/2)10− state gives the νi13/2 single particle energy free of octupole admixtures as 2.1(1) MeV. Eight high-spin states between 1.2 and 3.7 MeV were identified as the couplings of the two valence-particles to the146Gd octupole phonon, and three above-lying levels are assigned as double-octupole excitations including a 12+ state which decays by anE3-E3 stretched cascade. All these octupole levels can be quantitatively predicted from the one-particle x phonon spectrum of147Gd. The high-spin states above 3 MeV are four-quasiparticle excitations ofπ+1π−1ν2 andπ2ν2 type and their energies are in good accord with shell model estimates.
THE LABYRINTH IN NUCLEAR STRUCTURE: International Conf. on The Labyrinth in Nuclear Structure, an EPS Nuclear Physics Divisional Conference | 2004
A. Maj; M. Kmiecik; M. Brekiesz; J. Grebosz; W. Meczynski; J. Styczen; M. Zieblinski; K. Zuber; A. Bracco; F. Camera; G. Benzoni; B. Million; N. Blasi; S. Brambilla; S. Leoni; M. Pignanelli; O. Wieland; A. Airoldi; B. Herskind; P. Bednarczyk; D. Curien; E. Farnea; G. de Angelis; D. R. Napoli; J. Nyberg; M. Kicińska-Habior; C. M. Petrache; D. Petrache; N. Dubray; J. Dudek
The reaction 48Ca+64Ni has been studied in the deep inelastic regime at approximately 6 MeV/A, by the CLARA‐PRISMA setup. Angular distributions of the reaction cross sections have been obtained for the most intense reaction products, taking into account the response function of the magnetic spectrometer. The response of PRISMA has been calculated making use of a MonteCarlo simulation of the transport of the ions in the spectrometer, starting from known events distributions. For the one‐nucleon transfer channels, the experimental data are in good agreement with predictions from a semiclassical multi‐nucleon transfer model.