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REINA() DE TRABALHO SOBRE FiSICA NUCLEAR NO BRASIL

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16 Estruturn Nuclear - XX<br />

either as true or chance. For each master gate three<br />

parameters, the energy of both detectors and the coincidence<br />

tag, were recorded with a CAMAC input register,<br />

assisted by a MBD-11 microprocessor, connected<br />

to a PDP-11/84 computer. The measurements<br />

were made on 15 direct and 4 skip cascades, for the<br />

first time. Based on the angular correlation results<br />

it wns possible to determine the multipole mixing ratios.<br />

for 10 transitions: 6(402) = —0.07±0.07, 6(456)=-<br />

0.06±0.07, 6(472) = — 0.7911 6(571)=0.75±0.05,<br />

5(575) = 1.79!1:11, 6(695) = 0.40111 6(809)<br />

0.57111, 6(980)=-0.270.02, 6(1232) = 1.48±0.23 and<br />

6(1956) = 0.661 .1'7. The present results show that<br />

a large number of 7 transitions have considerable Mi<br />

admixtures which are difficult to explain in terms of<br />

simple vibrational model. More refined models which<br />

take in to account the interaction between collective<br />

and quasi-particle effects may be necessary to explain<br />

the level structure in this nucleus.<br />

TESTING THE DYSON EXPANSION<br />

WITHIN THE QUON ALGEBRA<br />

S. S. AVANCINI, J. R. MARINELLI, D. P. MENEZES,<br />

M. M. WATANABE <strong>DE</strong> MORASS<br />

Dept(' de Fisica - UFSC<br />

N. YOSIIINAGA<br />

Saitama University - Japan<br />

In the literature fermion pairs are replaced by bosons in<br />

many known physical situations [1,2]. This is normally<br />

performed with the help of boson mappings, that link<br />

the fermionic Hilbert space to another Hilbert space<br />

constructed with bosons. Of course boson mapping techniques<br />

are only useful when the Pauli Principle effects<br />

are somehow minimized.<br />

In this work, the quon algebra [3], which interpolates<br />

between the Bose and Fermi algebras and depends on a<br />

free paramenter q, is used to generate a deformed Dyson<br />

boson expansion of the quadrupole operator, which<br />

is written in terms of three deformed bosons (s, d and<br />

g bosons). Then we obtain a quadrupole-quadrupole<br />

harniltonian, for a single j-shell, in terms of this deformed<br />

bosonic operator. The hamiltonian is diagonalized<br />

and its eigenvalue,s are compared with the ones obtained<br />

from the fermionic quadrupole-quadrupole hamiltonian.<br />

The deformation parameter helps in achieving<br />

the correct energy levels, what cannot he encountered<br />

in practice with the usual non-deforrned Dyson expansion.<br />

We use a kinematical criterion for fixing the q<br />

parameters by invoking the Pauli principle and compare<br />

the results to a best fitting procedure.<br />

[1] S.T. Beliaev and V.G. Zelevinsky , Nucl. Phys. 39<br />

(1962) 582 ; E.R. Marshalek , Nucl. Phys. A161<br />

(1971)401, Nucl. Phys. A224 (1974) 221<br />

[2] F.J. Dyson , Phys. Rev. 102 0956) 1217<br />

[31 O.W. Greenberg , Physical Review 1) 43 (1991)<br />

4111<br />

Dipole excitations of low energy in deformed<br />

nucleus studied by Nuclear Resonance<br />

Fluorescence<br />

ANGELA EMILIA <strong>DE</strong> ALMEIDA PINTO<br />

Institute de Fisica - usP<br />

ULRICH KNEISSL, HEINZ-HERMANN Prrz, .)URGEN<br />

MARGRAF, HERMAN MASER, JORGEN BESSERER,<br />

DANIELA BELIC, ALEXAN<strong>DE</strong>R <strong>NO</strong>RD, THOMAS<br />

ECKART, BERND KRISCHOK, OLIVER BECK,<br />

ALEXAN<strong>DE</strong>R WOLPERT<br />

Institut fiir Strahlenphysik der Universitiit Stuttgart<br />

Low lying dipole excitations in heavy nuclei are of actual<br />

interest in modern nuclear structure physics. Low<br />

energy photon scaterring off bound states, nuclear resonance<br />

fluorescence (NRF"), represents a higly selective<br />

and sensitive tool to investigate low lying dipole excitations<br />

in heavy nuclei. The discovery of a new class<br />

of enhanced magnetic dipole excitations in heavy deformed<br />

nuclei in high resolution electron scattering experiments<br />

by Richter and coworkers in 1984 initiated<br />

a large number of both experimental and theoretical<br />

work( 1,2). Numerous electron and photon scattering<br />

experiments were performed to study the systematics<br />

and fragmentation of this low lying, predominantly orbital<br />

mode often referred to as "Scissors Mode"N. On<br />

the other hand, the recent NBF experiments also provided<br />

evidence for enhanced, low lying electric dipole<br />

excitations in deformed nuclei. The structure of the<br />

corresponding j"= states is discussed in terms of<br />

different collective excitation modes or two-phonon excitations.<br />

For odd mass nuclei by far less spectroscopy data are<br />

available. Recently the Stuttgart group succeeded to<br />

observe the first time the 'Scissors Mode" in an odd deformed<br />

Nucleus ( 163 1)y)(4). Similar results were found<br />

for 151 Dy, however, in ' 57Gd the dipole strength is completely<br />

fragmented into more than 80 transitions( 5).<br />

This different behavior of diverse odd deformed nuclei<br />

of the Rare Earth region is completely non understood.<br />

The purpose of these work is further investigation of<br />

the dipole strength distributions in odd-mass nuclei<br />

( 153Eu). The En nuclei are odd proton isotopes in between<br />

the well studied, deformed Gd isotopes and the<br />

already investigated Sm isotopes showing a transition<br />

from spherical to deformed nuclear shapes. NRF experiments<br />

in ' 53Eu were performed at the bremsstrahlung<br />

facility installed at the Stuttgart Dynarnitron accelerator,<br />

to contribute more experimental data on the dipole

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