Study of the charge sharing in a silicon pixel detector by means of α-particles interacting with a Medipix2 device
- 作者：M. Campbell ; E. Heijne ; T. Holý ; J. Idá ; rraga ; J. Jaků ; bek ; C. Lebel ; C. Leroy ; X. Llopart ; S. Pospí ; š ; il ; L. Tlustos ; Z. Vykydal
- 关键词：Medipix ; Charge sharing ; Silicon detector ; Plasma effect
- 刊名：Nuclear Instruments and Methods in Physics Research Section A ; Accelerators ; Spectrometers ; Detectors and Associated Equipment
- 出版年：2008
- 期刊代码：41_01689002
- 类别：ph
- 出版时间：11 June 2008
- 卷：591
- 期：1
- 页码：38-41
- 文件大小：152 K
摘要
The energy deposited in a silicon detector by a heavy charged particle, such as an 
-particle, creates a large number of electron–hole pairs. Under the influence of an electric field, the carriers drift towards the corresponding electrode. Due to diffusion, the charge carriers are spread. Lateral spreading depends on the collection time; hence it is expected to be smaller for larger fields. In the case of a pixellated detecting structure, this lateral spread can cause a sharing of the charge between the electrodes and many pixels will have a signal: that is, charge carriers generate a cluster of adjacent pixels. Also influencing the charge collection and its spread is the large concentration of electron–hole pairs generated locally by the -particle, which creates distortions of the electric field along the ionizing path, giving rise to the so-called plasma and funnelling effects. The results of the charge-sharing effect measured in the Medipix2 pixel detectors are shown as a function of the -particle energy and applied bias voltage. A model describing the effects of plasma and diffusion on the charge collection and charge sharing is presented.
-particle, creates a large number of electron–hole pairs. Under the influence of an electric field, the carriers drift towards the corresponding electrode. Due to diffusion, the charge carriers are spread. Lateral spreading depends on the collection time; hence it is expected to be smaller for larger fields. In the case of a pixellated detecting structure, this lateral spread can cause a sharing of the charge between the electrodes and many pixels will have a signal: that is, charge carriers generate a cluster of adjacent pixels. Also influencing the charge collection and its spread is the large concentration of electron–hole pairs generated locally by the -particle, which creates distortions of the electric field along the ionizing path, giving rise to the so-called plasma and funnelling effects. The results of the charge-sharing effect measured in the Medipix2 pixel detectors are shown as a function of the -particle energy and applied bias voltage. A model describing the effects of plasma and diffusion on the charge collection and charge sharing is presented.