Search for Hyperdeformation in Uranium Isotopes

Search for Hyperdeformation
in Uranium Isotopes

   

    This work was presented by D. Hawcroft at the XXXIII Zakopane School of Physics 1998.

Introduction

   

   Actinide nuclei possess significant Octupole deformations.

   Predicted to possess Low lying SUPERDEFORMED (SD) and HYPERDEFORMED (HD) minima.


   TRS calculations predict the HD minima in Uranium isotopes to have a large OCTUPOLE component.

S. Cwiok et al, Phys. Lett. B322 (1994) 304.


    232Uranium has 92 protons and 140 neutrons and is predicted to have a "dinuclear" shape.

DI-NUCLEUS:

    nearly spherical heavier component (around doubly-magic 132Sn)

    well-deformed lighter component (from the neutron-rich A ~ 100 region)


Experimental signatures
of hyperdeformation

   

Octupole deformed interleaved levels of positive and negative parity which will decay strongly through E1 emission

low energy gamma-rays (Energies from 50 to 150keV)

E2's strongly converted

look for E1's regularly spaced gamma-rays, energy spacing ~ 5keV

Problem: Contaminants caused by fission....

HD states Fission
Mean Gamma Multiplicity 15 10
Gamma Energy 100 keV 1 MeV
Detection Efficiency 11% 1%
Cross section 10 microbarns 1 barn

Need a gamma-ray Array with
high efficiency
at low energy ....
AFRODITE


The picture below shows the AFRODITE array.


Experimental details

   

232Th(,4n)232U with a beam energy of 40 MeV

Target thickness 2mg/cm2.

Collected 5 x 108 four fold and higher events.


Method of Analysis

   

Data was sorted into a -- cube.

Using the predicted -ray energies as a starting point, a large number of gate lists were produced by slightly varying the moment of inertia of the deformed nucleus.

Each of these gate lists were applied to the cube.

However, no clear evidence for the existence of a hyperdeformed band was seen.


Monte Carlo Simulation

   

In order to test the sensitivity of the experiment a Monte Carlo simulation was carried out.

An assumed hyperdeformed band was populated at a varied fraction ranging from 0.5 to 5 percent of the ground state (yrast) band population.

The resulting gamma cascades were corrected for internal conversion and the spectrometer response was folded in. The background was modelled empirically to reproduce the experimental background in the -- cube.


Results

    The top figure below shows the experimental ground state band brought back from a sum of gates on the labelled transitions.

The bottom figure shows a simulation of the ground state band gated on the same transitions.

A Monte Carlo simulation of a hypothetical hyperdeformed band populated at a given level of the ground state band

Conclusions

   

An experiment was performed using the AFRODITE array to search for the existence of a rotational band built on the hyperdeformed minimum in the 232U nucleus.

No clear evidence for the existence of a hyperdeformed band was seen.

It was found through Monte Carlo Simulations that at a population level of 0.5 to 1.0 percent the experiment is no longer sensitive enough to pick out the signal of the hyperdeformed band from the background.


Collaborators

    D. Hawcroft1, D. E. Appelbe1, D. G. Aschman2, B. R. S. Babu3, R. Bark4, R. Beetge2, M. Benatar2, P. A. Butler1, A. J. Chewter1, G. D. Dracoulis4, R. Fearick2, S. V. Fortsch3, R.-D. Herzberg1, G. D. Jones1, S. Juutinen5, H. Kankaanpää5, J. J. Lawrie3, G. K. Mabala2, N. Mhlahlo2, S. Murray2, S. Naguleswaran3, D. P. Rea1, C. Rigollet3, J. F. Sharpey-Schafer3, B. Simpson3, R. Smit3, D. Steyn2, V. M. Tshivhase2 and W. Whittaker2.

1 Oliver Lodge Laboratory, University of Liverpool, Liverpool, L69 3BX, United Kingdom.

2Department of Physics, University of Cape Town, South Africa.

3National Accelerator Centre, Faure, 7131, South Africa.

4Australian National University, Canberra, ACT 0200, Australia.

5Department of Physics, University of Jyväskylä, FIN-40351, Jyväskylä, Finland.


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Last modified: 4 February 1999

Written by Debs Hawcroft, dh@ns.ph.liv.ac.uk