Charge Collection properties of Double Sided Germanium Strip Detector

26 Oct 2021, 12:20
20m
Online (University of Jammu)

Online

University of Jammu

Talk Detectors in Nuclear Physics Oral presentations

Speaker

Arzoo Sharma (Department of Physics, Indian Institute of Technology Ropar, Rupnagar – 140 001, Punjab, India)

Description

The position sensitivity of a double-sided germanium strip detector has been studied using the coincidence method. The coincidences were demanded between an imaging scanner and a position-sensitive planar segmented germanium detector, comprising 10x10 electrical segmentation in orthogonal directions, using a positron source. The imaging scanner consists of a LYSO scintillation crystal coupled to a position-sensitive photomultiplier tube. The coincidence data have been analyzed by employing the Positron Annihilation Correlation (PSA) principle. The primary objective of this work is to study the charge carrier transportation for gamma-ray interaction inside the germanium detector, which has been studied using the pulse shape analysis procedure. The analysis has been performed to locate the gamma-ray interaction using the rise-time response of the detector for single interaction events along the depth of the germanium detector. The 2-dimensional image generated from the imaging scanner has been used to characterize the planar strip detector. Detailed scanning procedures and analysis of the present work will be presented at the conference.

References

[1] C. Domingo-Pardo et al., Nucl. Instru. Methods in Physics Research, 643 (2011) 79.
[2] J. Sethi, R. Palit, S. Saha, B. Naidu, AIP Conference Proceedings 1524 (2013) 287.

What is your experiment? Study response of segmented germanium detector

Primary author

Arzoo Sharma (Department of Physics, Indian Institute of Technology Ropar, Rupnagar – 140 001, Punjab, India)

Co-authors

R. Palit (Department of Nuclear and Atomic Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai – 400 005, India) Dr T. Habermann (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany) J. Gerl (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany) I. Kojouharov (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany) M. Górska (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany) H. Schaffner (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany) S. Saha (School of Advance Sciences, VIT University, Vellore - 632014, India) Biswajit Das (Department of Nuclear and Atomic Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai – 400 005, India) P. Dey (Department of Nuclear and Atomic Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai – 400 005, India) R. Donthi (Department of Nuclear and Atomic Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai – 400 005, India) B.S. Naidu (Department of Nuclear and Atomic Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai – 400 005, India) S. Mandal (Department of Physics, North Campus, University of Delhi, Delhi – 110 007, India) Pushpendra P. Singh (Department of Physics, Indian Institute of Technology Ropar, Rupnagar – 140 001, Punjab, India)

Presentation materials