The 78th JSAP Autumn Meeting, 2017

Presentation information

Oral presentation

13 Semiconductors » 13.2 Exploratory Materials, Physical Properties, Devices

[7a-C13-1~12] 13.2 Exploratory Materials, Physical Properties, Devices

Thu. Sep 7, 2017 9:00 AM - 12:15 PM C13 (office 2-2)

Takashi Suemasu(Univ. of Tsukuba), Kosuke Hara(Univ. of Yamanashi)

11:45 AM - 12:00 PM

[7a-C13-11] Photoresponse properties of low B-doped p-BaSi2 on
P+ ion-implanted Si (111)

Emha Bayu Miftahullatif1, Takabe Ryota1, Yachi Suguru1, Toko Kaoru1, Suemasu Takashi1 (1.Univ. of Tsukuba)

Keywords:semiconductor, silicide, solar cell

Semiconducting BaSi2 has an indirect band gap of approximately 1.3 eV, matching the solar spectrum, and has large absorption coefficients, reaching 3.0´104 cm-1 at 1.5 eV [1,2]. We have successfully fabricated n-Si/B-doped p-BaSi2 heterojunction solar cells that achieved a conversion efficiency of 9.9% [3]. In the work mentioned, we used an n-Si(111) substrate with n~1015 cm-3, and a 20-nm-thick B-doped p-BaSi2 layer with hole concentration p = 2.2 × 1018 cm-3 [3]. In order to utilize B-doped p-BaSi2 as an active layer, we need to employ n-Si with higher electron concentration n and low p p-BaSi2, so that the depletion region stretches toward the p-BaSi2 layer. However, the rectifying current density versus voltage (J-V) characteristics degraded as we utilized heavily-doped n-Si substrate due to the defects around steps with 3-4 MLs (~1 nm) in height. They were formed during thermal cleaning due to step bunching, confirmed by TEM (Fig. 1). High impurity concentration near the surface is suspected to be one of the origins of this step bunching. In order to reduce this step bunching by maintaining low impurities at the surface, we implant P+ ions into the Si substrate to the depth of 50 nm to form heavily-doped n+-Si embedding layer. We then formed a low B doped p-BaSi2 layer and measured the external quantum efficiency (EQE) as well as the J-V characteristics.