4-8 July 2016
Kramer Law building
Africa/Johannesburg timezone
<a href="http://events.saip.org.za/internalPage.py?pageId=10&confId=86">The Proceedings of SAIP2016</a> published on 24 December 2017

Orientation of the Ge Crystals of the iThemba LABS Segmented Clover Detector

5 Jul 2016, 16:10
1h 50m
Kramer Law building

Kramer Law building

UCT Middle Campus Cape Town
Board: B.426
Poster Presentation Track B - Nuclear, Particle and Radiation Physics Poster Session (1)

Speaker

Dr Tshepo Dinoko (iThemba LABS)

Apply to be<br> considered for a student <br> &nbsp; award (Yes / No)?

No

Would you like to <br> submit a short paper <br> for the Conference <br> Proceedings (Yes / No)?

Yes

Level for award<br>&nbsp;(Hons, MSc, <br> &nbsp; PhD, N/A)?

N/A

Please indicate whether<br>this abstract may be<br>published online<br>(Yes / No)

Yes

Abstract content <br> &nbsp; (Max 300 words)<br><a href="http://events.saip.org.za/getFile.py/access?resId=0&materialId=0&confId=34" target="_blank">Formatting &<br>Special chars</a>

By using an automated scanning table, the position sensitive response of crystals A, B, C and D, of the iThemba LABS segmented clover detector were measured using the 241Am collimated source [1]. One of the primary parameters to describe a Ge detector for pulse shape analysis is the orientation of the crystallographic axis of the cubic centered Ge crystal. The drift mobility for the electron-hole pair in the Ge depends on the orientation of the electrical field with respect to this axis and causes deviation in the collection times of up to 30% [2].
The intention is to characterize the segmented iThemba LABS Ge clover detector, for pulse shape analysis and develop a technique that determines the individual position of each energy deposition caused by the interaction of a gamma-ray in the segmented Ge crystal [3]. The T30 to T90 rise-time distributions, which refers to the time needed for the pulse to rise from 10% to 90% of its amplitude, were measured from each core at 12 mm radial distance and with a step of 10o around the core. Our results suggest that the drift velocity is position sensitive for each crystal of the detector. This necessitates a measurement of the crystal orientations of the four crystals of the detector.
[1] M. Descovich, et al., Nucl. Instr. And Meth., A553, 512-521 (2005)
[2] B. Bruyneel, et al., Nucl. Instr. And Meth., A569, 764 (2006)
[3] C. E. Svensson, et al., Nucl. Inst. And Meth. A 540, 348-360 (2005)

Main supervisor (name and email)<br>and his / her institution

Tshepo Dinoko
tdinoko@tlabs.ac.za
iThemba LABS

Primary author

Dr Tshepo Dinoko (iThemba LABS)

Co-authors

Dr Elena Lawrie (iThemba LABS) Mr Jayson Easton (iThemba LABS and University of the Western Cape) Mr Nicholas Erasmus (University of the Western Cape) Dr OBED SHIRINDA (iThemba LABS) Ms Sinegugu Happiness Mthembu (Student) Mr Sive Noncolela (UWC) Dr Thifhelimbilu Daphney Bucher (iThemba LABS)

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