Title: Investigation of the CoreHalo Structure of the NeutronRich Nuclei 6He and 8He by IntermediateEnergy
1Measurement of the 6He ? ? d e- ?-
branching ratio
Farouk Aksouh et al.Brussels Meeting December
15 - 16, 2003
1 - Introduction Motivation 2 - Experimental
Setup 3 - Data Analysis and results 4 -
Conclusion Perspectives
21 - Introduction motivation
- 6He ? 6Li(g.s.) e- ?- Branch 1 ?
99.999 Half-life 0.807 sec - 6He ? 6Li ? ? d e- ?- Branch 2 ?
10-3-10-4 (Q 2.033 MeV) 1
- Specific case of 6He among exotic n-rich halo
nuclei e. g. 11Li interaction cross section,
breakup cross section, nuclear magnetic moment,
momentum distribution of fragments, elastic cross
sections (protons, ?)
- 6He is a cluster of an ? core (internal part) and
two valence neutrons forming the halo (external
part) - Measurement of the ?-delayed (?d) emission ?
probe of the halo w.f. up to large distances 2
3Present knowledge
4Experimental setupPH196 Experiment at CRC
Beam line at CRC
6He Beam at 8 MeV implanted at the middle of the
detectorReduced intensity (5000 pps) and
uniformly distributed on the detector active
areaPeriodic Implantation 1 sec beam ON and 2
sec beam OFF (for 100 implanted nuclei, 60
registered decays)Beam suppression factor of 5.5
X 10-4 (all E) 3.7 X 10-7 (E lt 2 MeV)?-
spectrum end-point at 3.508 MeV 18Ne Beam at
10 MeV Periodic Implantation 1 sec beam ON
and 1 sec beam OFF ? spectrum end-point at
3.424 MeV
5Double Sided Silicon Strip Detector( Micron
Semiconductor )
Active area 16mm X 16mm Thickness 78um Front
face 48 p strips horizontal Back face 48 n
strips vertical Strip width 300 um Strip pitch
335 um
Energy Resolution (5805 keV ? line of
244Cm) Front face 25 keV Back face 30 keV
Si wafer
Connector for 48 strips
Printed circuit board
Front View
6Data Analysis
6He
Normalized spectra of 6He and 18Ne
18Ne
Number of implantationsN(6He) 1.86 X
109N(18Ne) 1.31 X 109
7Experimental results
Preliminary
Branching ratio ()B 1.0(2) X 10-6
() Only statistical uncertainties are shown
8CONCLUSION PERSPECTIVES
Validity of the experimental methodSeparation of
the very weak decay channel from the main decay
modeThe branching ratio value is closer to 10-6
Experimental discrepancy (Borge93 Anthony02)
is solvedImportance of the region at low
energyUse of a more sensitive electronics at low
E new measurementMore statistics improve the
shape of the transition probability distribution
9COLLABORATORS
F. Aksouh, D. Smirnov, S. Dean, H. de Witte, J.
Gentens, I. Mukha, M. Huyse, O. Ivanov, P. Mayet,
R. Raabe, J.-C. Thomas, P. Van den Bergh, K. Van
de Vel, J. Van de Walle, P. Van Duppen C.
Angulo, J. Cabrera, A. Ninane, P. Demaret T.
Davinson
Institut voor Kern- en Stralingsfysica, Catholic
University of Leuven, Leuven, Belgium
Institut de Physique Nucléaire, Université
Catholique de Louvain, LLN, Belgium
Department of Physics Astronomy, The University
of Edinburgh, Edinburgh, UK