• 沒有找到結果。

Study of Si/SiGe Multiple Quantum Well(MQW) Infrared Photodetector 王宗良、黃俊達

N/A
N/A
Protected

Academic year: 2022

Share "Study of Si/SiGe Multiple Quantum Well(MQW) Infrared Photodetector 王宗良、黃俊達"

Copied!
2
0
0

加載中.... (立即查看全文)

全文

(1)

Study of Si/SiGe Multiple Quantum Well(MQW) Infrared Photodetector 王宗良、黃俊達

E-mail: [email protected]

ABSTRACT

The SiGe based separate-absorption-multiplication avalanche-photodiode(SAMAPD)and has been implemented for the first time. The structure of SAMAPD, in our work, is P +-Si/MQW-(SiGe/Si)/ i-SiGe/N+-Si, in which the i-SiGe and quantum well structure of SiGe/Si are deposited by ultra-high-vacuum chemical-vapor-deposition (UHVCVD) system. In this structure,the thickness of i-Si0.8Ge0.2 layer is about 150nm and quantum structure is of Si (25 nm)/Si0.8Ge0.2( 5 nm) with five periods.

Experiment results shows that the current increases sharply at about 2 V reverse bias, we speculates that the avalanche effect occurred at this voltage. Two structures of dot and net are processed in our studies. We found that the photo-to-dark current ratio of Iphoto/Idark was 15.19 without and 17.9 with covered by Al thin film for dot electrodes at 1 V reverse bias voltage. A higher photo-to-dark current ratio was obtained for net electrodes, the Iphoto/Idark is 52.6 without covered by Al thin film; after covered by Al thin film, the Iphoto/Idark achieved a high value of 134. In addition, the solar cell performance with this structure is measured by using a simulated solar source of 1000W/cm2 and a high conversion efficiency of 8.26% is obtained for dot electrodes with Al thin films.

Keywords : MQW ; SiGe ; photodetector ; evaporation ; solar cells

Table of Contents

封面內頁 簽名頁 授權書.........................iii 中文摘要............

............iv 英文摘要........................v 誌謝 .........

.............. ..vi 目錄..........................vii 圖目錄...

......................ix 表目錄.........................xi 第 一章 前言 ......................01 第二章 原理 ....................

..03 2.1 矽鍺的基本特性...................03 2.2光檢測器原理..............

.......07 2.2.1 光的種類................ .... 07 2.2.2 輻射轉換..........

...........07 2.2.3 光的吸收.....................08 2.2.4 P-N接面......

............... 09 2.2.5 P-N與PIN感光二極體................12 第三章 元件製程

、光電量測與材料分析 ...........17 3.1薄膜成長系統.....................17 3.2 樣品清洗.......................18 3.3蒸鍍機系統(Thermal Evaporator System)......

.19 3.4傳統爐管退火系統(Conventional Furnace Annealing).19 3.5光電量測系統..................

...20 3.5.1電性量測(Current ─ Voltage measurement)....20 3.5.2光譜響應量測(Spectral response measurement) .

.21 3.5.3響應率量測(Responsivity measurement).... ..21 第四章 實驗結果與討論...............

... 25 4.1歐姆電極.......................25 4.2 PL量測 ..............

.........28 4.3電性量測.......................29 4.4光譜響應........

...............39 4.5太陽能電池之量測...................41 第五章 結論與未 來展望..................44

REFERENCES

[1] J. C. Bean, T. T. Sheng, L. C. Feldman, A. T. Fiory, and R. T. Lynch, "Pseudomorphic growth of GexSi1-x on silicon by molecular beam epitaxy," Appl. Phys. Lett, Vol.44, pp. 102-104 (1984) [2] R. People, and J. C. Bean, "Calculation of critical layer thickness versus lattice mismatch for GexSi1-x/Si strained-layer heterostructures," Appl. Phys. Lett, Vol.47, pp. 322-324 (1985).

[3]J.-S. Rieh, D. Klotzkin, O. Qasaimeh, L.-H. Lu, K. Yang, L. P. B. Katehi, P. Bhattacharya, and E. T. Croke, “Monolithically integrated SiGe-Si,PIN-HBT front-end photoreceivers,” IEEE Photon. Technol. Lett., vol.10, pp. 415–417, Mar., 1998.

[4]F.G.Della Corte and F.Pezzimenti,”Design considerations for a-Si:/SiGe/Si heterojunction,”Quantum Electronics, IEEE journal of,22,pp.1696-1710(1986) [5]J.Poortmans, S.C.Jain,DHJ Totterdell, M. Caymax, J.f.Nijs,R.P.Mertens and R. Van Overstraeten, ‘Theoretical calculation and experimental evidence of the real and apparent bandgap narrowing due to heavy doping in p-type silicon and strained Si1-x+Gex

(2)

layers’,Solid State Electronics,36,1763(1993) [6] People, R., Quantum Electronics, IEEE Journal of, Volume: 22, Issue: 9, pp.1696-1710 (1986) [7] Splett, A.; Zinke, T.; Petermann, K.; Kasper, E.; Kibbel, H.; Herzog, H.-J.; Presting, H., Photonics Technology Letters, IEEE, Volume: 6, Issue: 1, pp.59-61 (1994) [8] Shi, Jin-Wei; Pei, Z.; Yuan, F.; Hsu, Y.-M.; Liu, C.-W.; Lu, S. C.; Tsai, M., Journal of Applied Physics, Vol. 85 Issue 14, pp.2947-2949 (2004) [9] People, R.; Bean, J. C., Applied Physics Letters, Vol. 47 Issue 3, pp.322-324 (1985) [10] S. M. Sze, J. Y. Zhang,

”Semiconductor Devices Physics and Technology”, Wiley Intersciwnce, pp.336.

[11]S. M. Sze, Physics of Semiconductor Devices,2nd ed., Wiley, New York, 1981, Chapter 12-14.

參考文獻

相關文件

at each point of estimation, form a linear combination of a preliminary esti- mator evaluated at nearby points with the coefficients specified so that the asymptotic bias

– By analyzing Pre-S1 HKAT and S3 TSA results, English proficiency was improved and more profound improvement was found for speaking skill (Objective 1). – About % of

Hybrid solar cell (amorphous Si & thin - - film film polycrystal polycrystal Si) Si)..

With respect to the effect of shareholding ratio of the board of directors on repurchase motivations, we find that firms with lower shareholding ratios by board members are

Animal or vegetable fats and oils and their fractiors, boiled, oxidised, dehydrated, sulphurised, blown, polymerised by heat in vacuum or in inert gas or otherwise chemically

remember from Equation 1 that the partial derivative with respect to x is just the ordinary derivative of the function g of a single variable that we get by keeping y fixed.. Thus

Consistent with the negative price of systematic volatility risk found by the option pricing studies, we see lower average raw returns, CAPM alphas, and FF-3 alphas with higher

Survivor bias is that when we choose a sample from a current population to draw inferences about a past population, we leave out members of the past population who are not in