Turn-on and turn-off voltages of an avalanche p-n junction
Characteristics of the turn-on and turn-off voltage of avalanche p-n junctions were demonstrated and studied. As opposed to existing reports, the differences between the turn-on and turn-offvoltage cannot be neglected when the size of the p-n junction is in the order of microns. The difference incre...
Saved in:
| Published in | Journal of semiconductors Vol. 33; no. 9; pp. 55 - 59 |
|---|---|
| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
01.09.2012
|
| Subjects | |
| Online Access | Get full text |
| ISSN | 1674-4926 |
| DOI | 10.1088/1674-4926/33/9/094003 |
Cover
| Summary: | Characteristics of the turn-on and turn-off voltage of avalanche p-n junctions were demonstrated and studied. As opposed to existing reports, the differences between the turn-on and turn-offvoltage cannot be neglected when the size of the p-n junction is in the order of microns. The difference increases inversely with the area of a junction, exerting significant influences on characterizing some parameters of devices composed of small avalanche junctions. Theoretical analyses show that the mechanism for the difference lies in the increase effect of the threshold multiplication factor at the turn-on voltage of a junction when the area of a junction decreases. Moreover, the "breakdown voltage" in the formula of the avalanche asymptotic current is, in essence, the avalanche turn-off voltage, and consequently, the traditional expression of the avalanche asymptotic current and the gain of a Geiger mode avalanche photodiode were modified. |
|---|---|
| Bibliography: | Characteristics of the turn-on and turn-off voltage of avalanche p-n junctions were demonstrated and studied. As opposed to existing reports, the differences between the turn-on and turn-offvoltage cannot be neglected when the size of the p-n junction is in the order of microns. The difference increases inversely with the area of a junction, exerting significant influences on characterizing some parameters of devices composed of small avalanche junctions. Theoretical analyses show that the mechanism for the difference lies in the increase effect of the threshold multiplication factor at the turn-on voltage of a junction when the area of a junction decreases. Moreover, the "breakdown voltage" in the formula of the avalanche asymptotic current is, in essence, the avalanche turn-off voltage, and consequently, the traditional expression of the avalanche asymptotic current and the gain of a Geiger mode avalanche photodiode were modified. Geiger mode avalanche photodiode; p-n junction; turn-on voltage; turn-off voltage 11-5781/TN Zhang Guoqing , Han Dejun , Zhu Changjun , and Zhai Xuejun 1 School of Science, Xi'an Polytechnic University, Xi'an 710048, China 2The Key Laboratory of Beam Technology and Materials Modification of the Ministry of Education, Beijing Normal University Beijing Radiation Center, Beijing 100875, China ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
| ISSN: | 1674-4926 |
| DOI: | 10.1088/1674-4926/33/9/094003 |