Volume 28, Issue 9 pp. 971-976
SHORT COMMUNICATION

Impact of bilayer structures on the surface passivation quality of high-rate-sputtered hydrogenated amorphous silicon for silicon heterojunction solar cells

Faris Akira Bin Mohd Zulkifly

Faris Akira Bin Mohd Zulkifly

Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Meguro-ku, Tokyo, 152-8550 Japan

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Yuta Shiratori

Yuta Shiratori

Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Meguro-ku, Tokyo, 152-8550 Japan

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Kazuyoshi Nakada

Kazuyoshi Nakada

Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Meguro-ku, Tokyo, 152-8550 Japan

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Shinsuke Miyajima

Corresponding Author

Shinsuke Miyajima

Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Meguro-ku, Tokyo, 152-8550 Japan

Correspondence

Shinsuke Miyajima, Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Meguro-ku, Tokyo 152-8550, Japan.

Email: [email protected]

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First published: 02 June 2020
Citations: 4

Faris Akira Bin Mohd Zulkifly and Yuta Shiratori contributed equally to this work.

Abstract

Crystalline silicon surface passivation effect of intrinsic hydrogenated amorphous silicon (i-a-Si:H) films deposited by radio-frequency facing target sputtering (RF-FTS) using a two-step deposition technique was investigated. In the two-step deposition technique, an i-a-Si:H layer was deposited at a high sputtering power condition after the deposition of i-a-Si:H at a low sputtering power condition. The two-step deposition technique drastically improved the passivation quality of i-a-Si:H compared with a conventional single-step deposition technique. Only 0.5-nm-thick i-a-Si:H deposited at a low sputtering power suppresses the initial sputtering damage to the crystalline silicon surface. A high average deposition rate of 14.1 nm/min was also achieved. A non-textured silicon heterojunction solar cell using an i-a-Si:H passivation layer deposited by the two-step method shows a conversion efficiency of 17.4% (Voc = 0.679 V, Jsc = 35.0 mA/cm2, FF = 0.732).

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