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REINA() DE TRABALHO SOBRE FiSICA NUCLEAR NO BRASIL

REINA() DE TRABALHO SOBRE FiSICA NUCLEAR NO BRASIL

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XX RTFNB - Resumos - 02/09/97 19<br />

The 7—ray spectroscopy of low- Z or very neutron defficient<br />

evaporation residues is difficult because of the<br />

strong competition among 'many open channels. Typically<br />

2 to 5 particles are evaporated from a heavyion<br />

reaction, in varied combinations of protons, neutrons<br />

and alpha particles. A partial selection of specific<br />

channels can be made by detecting and identifying<br />

some or all of the evaporating particles. Indeed, the use<br />

of ancillary charged particle detectors can significantly<br />

improve the resolving power of 7—ray spectrometers.<br />

The 7-spectroscopy group of the Pelletron Laboratory<br />

has interest in the study of the A re. 100, 80 and 30<br />

mass regions, which would benefit from the use of an<br />

evaporation-- channel filtering device. The design of the<br />

4x charged particle telescope array was based on ref. [1].<br />

The system consists of 12 plastic phnswich scintillators,<br />

disposed in the geometry of a dodecahedron. Each telescope<br />

consists of a 0.1 mm thick fast scintillation decay<br />

time BC400 AE detector bonded to a 10 mm thick<br />

long decay time BC444 E detector. The detector faces<br />

have a diameter of 2 cm. The E and AE detectors are<br />

bonded toghether by the vacuum heat press technique<br />

[2] in order to avoid the presence of a dead layer. The<br />

target chamber also serves as a support for the detectors,<br />

and has the shape of a semi-regular polyhedron<br />

with 12 pentagonal and 20 triangular faces. It is built<br />

of aluminum and is divided in two hemispheres excavated<br />

inside in order Lo minimize 7 ray absorption. The<br />

chamber has a diameter of 14 cm, and the whole system,<br />

including the photornultiplier tubes and bases fits<br />

in a sphere of 24 cm diameter. The 7-ray detectors are<br />

aligried with the triangular faces.<br />

[1]F. Lidiin, Nucl. Inst. and Meth. A288 (1990), 455<br />

[2]C. A. Pruneau et at, Nucl. Inst. and Meth. A297<br />

(1990), 404.<br />

DSAM LIFETIMES IN THE DOUBLY ODD<br />

NUCLEUS 134Pr<br />

M. N. Rao, H.. V. RIBAS, N. H. MEDINA, M. A.<br />

Rizzurro, E. W. CYBULSKA. J. R. B. OLIVEIRA<br />

Department() de Fisica Nuclear, Institute de Fitica USP<br />

F. ft. ESPI<strong>NO</strong>ZA-QUIFIONES<br />

Departamento de Alien CCE, Universidade Estadual de<br />

Lendrina, Londrina, PR, Brasil<br />

1). BAZZACCO, S. LUNARDI, C. M. PETRACHE, ZS.<br />

PODOLYAK, C. ROSSI ALVAREZ, T. SCANEERLA, C.<br />

A.. UR<br />

Dipartimento de Fisica and INFN„ Sezione di Padova,<br />

Padova, Italy<br />

R. VENTURELLI, D. <strong>DE</strong> ACuRA., G. <strong>DE</strong> ANGELIS, M.<br />

<strong>DE</strong> POLL, E. FARNEA, A. OA<strong>DE</strong>A, D. R. NAPOLI, L.<br />

H. ZHU<br />

INFN, Laborateri Nazionati di Legnero, Ugrian+, Italy<br />

A. <strong>DE</strong>WALD, J. OARLESKE, P. VON BRENTA<strong>NO</strong>.<br />

Institut fiir Kernphysik der Universitat zu Koln, Kan,<br />

Germany<br />

Information on highly deformed rotational hands in the<br />

doubly odd ' 34Pr nucleus has become available quite<br />

recently [1,2]. One of these bands has been tentatively<br />

assigned a r(h1v2) 3 0 v(I7/2,119/2) configuration, while<br />

the other band is thought to have the ir(h1i/2) 3 0 vilayz<br />

configuration. Thus one would expect the latter band<br />

to have a more deformed nuclear shape.<br />

The present note reports on a Doppler broadened lineshape<br />

lifetime measurement in this nucleus. The rotational<br />

bands in 134Pr were populated by bombarding a Aubacked<br />

110Pd target with 130 MeV 'Si beam provided<br />

by the XTU tandem accelerator of the Legnaro National<br />

Laboratory. The GASP array, BOO inner ball and<br />

the multi-telescope particle detector ball (ISIS) were<br />

utilized in order to select the proton gated events. Data<br />

were of sufficiently good statistics to obtain dean gated<br />

spectra for the positive parity E2 band. The Doppler<br />

broadened lineshapes for a cascade of 6 transitions in<br />

this band were fitted for 5 of the 7 rings of detectors<br />

(36°, 60°, 90°, 120° and 146") in the GASP array. The<br />

analysis of data was performed with the computer code<br />

LINESHAPE [3], assuming rotational-band side feeding<br />

for each of the levels of interest. The slowing down<br />

of the Pr recoiling nuclei was described with two sets<br />

of electronic stopping, viz., shell-corrected Northcliffe-<br />

Schilling and Ziegler's heavy-ion stopping powers.<br />

[1]K.Ilausehild et.al ., Phys. Rev. C50 (1994) 707<br />

[2]C.M.Petrache et al., Nucl. Phys. A.597 (3996) 106<br />

[3]J.C.Wells and N.lt.Johnson, OItNL Report (1996),<br />

unpublished<br />

PRELIMINARY RESULTS FOR. THE I'La<br />

NUCLEUS<br />

M. A. RTZZUTTO, E. W. CYBULSKA, .1. B., B.<br />

OLIVEIRA., R.. V. RIBAS, N. H. MEDINA, M. N.<br />

Rao, W. A. SEALE, 0. ZAHN, C. FRANCA, 3.<br />

A LCANTAII -Nrili,*EZ<br />

Institato de Fisica, Universidade de san Paulo, Sao Paulo,<br />

Brazil<br />

. R. ESPI<strong>NO</strong>ZA-QUISIONES<br />

Departamento de Pisicu - CCE, Universidade Estadual do<br />

bondrina, Londrina, PR, Brazil<br />

With the view of extending the systematics of odd and<br />

odd-odd nuclei in the A = 130 - 140 mass region towards<br />

to the N = 82 closed shell, the nucleus 1"La was<br />

studied with in-beam -y-ray spectroscopy. The nuclei<br />

in the region Z 50 and N re 80 are of interest because<br />

the Fermi surface is close to the top of the neutron<br />

intruder h1112 subshell and the proton one is at the<br />

bottom of this subshell, causing a competition between<br />

the neutron oblate and proton prolate driving forces.<br />

This competition can result in shape transitions from<br />

prolate (N = 73) to triaxial or oblate (N = 80) forms.

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