Laser-induced Etching of Chlorinated Silicon Surfaces

Koji MAEDA; Hirotaka AMASUGA; Yoshiaki NAKAMURA; Yutaka MERA

doi:10.1380/jsssj.20.393

塩素吸着シリコン表面のレーザー励起エッチング

前田康二, 天清宗山, 中村芳明, 目良裕

著者情報

ジャーナルフリー

1999 年 20 巻 6 号 p. 393-400

DOI https://doi.org/10.1380/jsssj.20.393

詳細

発行日: 1999/06/10 受付日: 1999/02/26 J-STAGE公開日: 2009/08/07 受理日: 1999/02/26 早期公開日: - 改訂日: -
訂正情報
訂正日: 2009/08/07 訂正理由: - 訂正箇所: 論文抄録訂正内容: Wrong : Measurements of excitation spectra of photoetching of chlorinated Si(111)7×7 surfaces stimulated by ultraviolet nanosecond pulse laser light revealed that there are two distinct spectral peaks, one (α-peak) being located near 290nm and another (β-peak) at 245 nm. The α-peak exhibits a strong supralinear dependence on light intensity above laser fluence of&sim;100mJ/cm² pulse, while the β-peak grows linearly with light intensity. The red shift of the α-peak with increasing intensity coincides with the shift of laser abration, which strongly suggests that the origin of the α-peak photoetching is thermal etching enhanced by surface heating due to interband transition in the substrate. The dependence on polarization of the incident light suggests that the β-peak photoetching originates in excitation of hot carriers in the substrate which are captured resonantly by the anti-bonding states of the adsorbate chlorides resulting in destabilization of the molecules.
Right : Measurements of excitation spectra of photoetching of chlorinated Si(111)7×7 surfaces stimulated by ultraviolet nanosecond pulse laser light revealed that there are two distinct spectral peaks, one (α-peak) being located near 290nm and another (β-peak) at 245 nm. The α-peak exhibits a strong supralinear dependence on light intensity above laser fluence of∼100mJ/cm² pulse, while the β-peak grows linearly with light intensity. The red shift of the α-peak with increasing intensity coincides with the shift of laser abration, which strongly suggests that the origin of the α-peak photoetching is thermal etching enhanced by surface heating due to interband transition in the substrate. The dependence on polarization of the incident light suggests that the β-peak photoetching originates in excitation of hot carriers in the substrate which are captured resonantly by the anti-bonding states of the adsorbate chlorides resulting in destabilization of the molecules.

抄録

Measurements of excitation spectra of photoetching of chlorinated Si(111)7×7 surfaces stimulated by ultraviolet nanosecond pulse laser light revealed that there are two distinct spectral peaks, one (α-peak) being located near 290nm and another (β-peak) at 245 nm. The α-peak exhibits a strong supralinear dependence on light intensity above laser fluence of∼100mJ/cm² pulse, while the β-peak grows linearly with light intensity. The red shift of the α-peak with increasing intensity coincides with the shift of laser abration, which strongly suggests that the origin of the α-peak photoetching is thermal etching enhanced by surface heating due to interband transition in the substrate. The dependence on polarization of the incident light suggests that the β-peak photoetching originates in excitation of hot carriers in the substrate which are captured resonantly by the anti-bonding states of the adsorbate chlorides resulting in destabilization of the molecules.

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