Impact of impurities and crystal defects on the performance of CVD diamond detectors

被引:19
|
作者
Tarun, A. [1 ]
Lee, S. J. [1 ]
Yap, C. M. [1 ]
Finkelstein, K. D. [2 ]
Misra, D. S. [1 ]
机构
[1] Ila Technol Pte Ltd, 17 Tukang Innovat Dr, Singapore 618300, Singapore
[2] Cornell Univ, Cornell High Energy Synchrotron Source, Ithaca, NY 14853 USA
基金
美国国家卫生研究院; 美国国家科学基金会;
关键词
Single crystal CVD diamond; Particle detector; Spectroscopy; Nitrogen vacancy; Crystal defects and impurities;
D O I
10.1016/j.diamond.2015.08.018
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Radiation detectors based on diamond are highly favored for particle physics research due to the superior radiation hardness. In this work, we investigate the influence of impurities and crystalline imperfections on the charge collection efficiency (CCE) of single crystal diamond. Seventeen (17) ultra-low fluorescent diamond samples grown by microwave plasma chemical vapor deposition method from Ha Technologies PTE LTD are preselected for this study. The measured CCE of all samples using Am-241 (alpha-particles) as ionizing source are analyzed together with the concentration of trace impurities and crystalline imperfection in the crystal. The amounts of impurities are quantified from integrated fluorescence intensity arising from the nitrogen vacancies (NV) created during different CVD growth process conditions. The crystal imperfections are assessed by X-ray rocking curves from X-ray topography images obtained at the Cornell High Energy Synchrotron Source. The CCE decays rapidly as the intensity of NV (I-Nv), phonon sideband approaches that of diamond 2nd order Raman peak which follows the relation: CCE(I-NV) = 100/(1 + (I-NV/1.0)(5/2)). The energy resolution, Delta E/E (ratio of the energy spectrum width to the most probable peak) highly correlates with broader rocking curve width distribution. Prime novelty statement: This work provides an understanding on the most important factors that contribute to degradation of charge collection efficiency (CCE) in diamond based detectors and sensors. The CCE decays rapidly as the intensity of nitrogen vacancy phonon sideband approaches that of diamond 2nd order Raman peak which follows the relation: CCE(I-NV) = 100/(1 + (I-NV/1.0)5/2). The energy resolution, that is the ratio of the energy spectrum width to the most probable peak, highly correlates with broader X-ray rocking curve width distribution. (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:169 / 174
页数:6
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