Other experimental set-ups: IGISOL JANOSIK CUP Si Detectors BARRIERS SYRENA ICARE EAGLE
COULOMB EXCITATION AT THE WARSAW CYCLOTRON
the Warsaw Coulex Group:
Julian Srebrny, Katarzyna Hadyńska-Klęk,
Jędrzej Iwanicki, Paweł Napiorkowski,
Daniel Piętak, Kasia Wrzosek-Lipska, Magda Zielińska
The Warsaw Coulex Group was gathered in the early nineties around
Tomek Czosnyka, who was its leader until his death in 2006.
Under his supervision three PhD and two MSc theses were completed, all
pursuing the research using Coulomb excitation method.
Coulomb excitation method
Coulomb excitation (Coulex) is
a powerful method to study nuclear structure. Proper selection of
the beam energy assures that the interaction between the colliding
beam and target particles is purely electromagnetic, thus allowing
for the model-independent description in terms of classical
electrodynamics, free from the assumptions concerning the nuclear
forces. The use of different beams and impact parameter
information in principle allows to measure full sets of the
parameters of the electromagnetic structure up to high-spin levels
- transition matrix elements and static moments, the values which
determine spectroscopic observable - lifetimes, gamma intensities,
branching and mixing ratios. Finally, the knowledge of the full
sets of matrix elements can be used to reproduce the shape of the
nucleus independently for each excited level, thus serving as
"nuclear microscope". Heavy ion Coulex provides a
stringent test of existing models in a purely experimental way.
Recently new interest in Coulex is drawn by
commissioning the radioactive beam facilities opening the
perspectives to study the structure of unstable nuclei.
Heavy Ion Laboratory is capable of performing
the full-scale Coulex projects. The
cyclotron offers a wide range of heavy ion beams and the
flexibility of adjusting the beam energy according to the
requirements.
Coulex setups at HIL
At present two particle detector arrays, dedicated for Coulomb excitation,
are used at HIL. The older setup, CUDAC (Coulomb Universal Detector Array
Chamber)
was built in the Laboratory in the early nineties
and installed as one of the permanent experimental stands.
Recently a new scattering chamber, previously used with the NORDBALL setup,
has been adapted to work with the gamma detector array OSIRIS-II.
Both setups are built on the same principle. Coincident
detection of gamma radiation and scattered particles makes possible to
uniquely and precisely
ascribe the observed gamma rays to the kinematics of collision.
This in turn enhances the efficiency of experiments - one physical
accelerator run can be off-line divided into several data sets
differing by impact parameter. Such an operation is
equivalent to performing several experiments at the same real time.
In both scattering chambers small silicon detectors,
so-called PIN-diodes, are used for particle detection. As
PIN-diodes are not position-sensitive, the information on particle
detection angle is obtained by using many diodes in one setup. The
relatively small area of a single detector provides sufficiently precise
information on scattering angle.
The particle energy measurement is not essential in Coulomb
excitation
experiments. With thin targets the information on the particle scattering
angle
allows one to
determine the whole kinematics of the scattering process. However, the
information on the particle energy is useful to reject the events caused by
noise or scattering on admixtures in target. It is also crucial when
analysing
the experiments with thick targets when the incident energy changes due
to the beam stopping in target.
CUDAC
The CUDAC chamber is equipped with 32
PIN-diodes (1 x 1cm), placed at backward angles, which correspond to the
strongest excitation of the investigated nucleus.
To detect the deexcitation γ-radiation three HPGe
detectors are used, working in coincidence with PIN-diodes.
 |
 |
| Fig. 1, left: Schematic view of the CUDAC set-up. |
right:
The CUDAC chamber open to show the silicon detectors
inside. |
CUDAC has proven to be an excellent tool to study the
properties of well deformed nuclei, such as 165Ho. However, for the less
deformed ones, such as Mo isotopes, the gamma detection efficiency was too low
and therefore we decided to use a more compact Coulex scattering chamber with a
multi-detector germanium array OSIRIS-II.
It should be mentioned, that CUDAC was used for the experiments other than
Coulomb excitation, e.g.. for ionization or fusion barrier studies.
The data collected using the CUDAC setup were a basis for
3 PhD theses
(two on Coulomb excitation: J. Iwanicki (2002), M. Zielińska (2006) and one
on fusion barrier distribution: Ł. Świderski (2005)) as well as for several
MSc theses.
New scattering chamber
The scattering chamber, which has been recently succesfully
integrated into OSIRIS-II,
was constructed at LMU Munich as a dedicated
Coulomb excitation setup designed for use with the NORDBALL germanium array.
Its small size (10cm in diameter) allows to place
HPGe detectors at close distances from the target, thus increasing the gamma
detection efficiency. The chamber can accomodate up to 110 PIN-diodes of 0.5 x 0.5cm active
area, covering the backward angles (from 110 to 170 degrees with respect to
the beam direction). At present 48 PIN-diodes are used.
An original electronics was replaced by three 16-fold
digitally controlled fast/slow amplifiers (CAEN N568/LC) and constant
fraction discriminators (CAEN C808).
The first experiment using this new dedicated Coulex setup was performed in
2006. The future Coulex experiments at HIL can
benefit from higher overall efficiency and improved peak-to-Compton ratio of the
OSIRIS-II array (comprising 12 BGO-shielded HPGe detectors) and its planned
successor EAGLE.
 |
| Fig. 2:The backward hemisphere of the new scattering chamber.
|
Data analysis
Last, but not least, HIL Coulex team
is in command of the sophisticated software necessary to analyze
the wealth of data from the experiments. This includes both
processing of "raw" data and further physical analysis.
The analysis computer codes,
GOSIA and SIGMA, developed,
maintained and updated by Warsaw Coulex group members, are now
used by numerous world laboratories dealing with Coulomb
excitation. A list of collaborating centers include Rochester and
Argonne (USA), Saclay and Orsay (France), Liverpool (UK), Jyvaskyla (Finland),
Muenchen (Germany), Chandigarh (India), Tokai, Chiba, Osaka and
Kyushu (Japan).
It should be stressed, that
the available data from heavy ion Coulex are still scarce, so
Coulex project has obviously wide perspective for the future. It
already is and should remain for the years to come one of the home
specialties of the nuclear physics in Warsaw.
Other experimental set-ups: IGISOL JANOSIK CUP Si Detectors BARRIERS SYRENA ICARE EAGLE |