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未掺杂和n型掺杂多晶硅线波导中的传播损耗。

Propagation losses in undoped and n-doped polycrystalline silicon wire waveguides.

作者信息

Zhu Shiyang, Fang Q, Yu M B, Lo G Q, Kwong D L

机构信息

Institute of Microelectronics, A*STAR (Agency for Science, Technology and Research), 11 Science Park Road, Science Park-II, Singapore 117685.

出版信息

Opt Express. 2009 Nov 9;17(23):20891-9. doi: 10.1364/OE.17.020891.

Abstract

Polycrystalline silicon (polySi) wire waveguides with width ranging from 200 to 500 nm are fabricated by solid-phase crystallization (SPC) of deposited amorphous silicon (a-Si) on SiO(2) at a maximum temperature of 1000 degrees C. The propagation loss at 1550 nm decreases from 13.0 to 9.8 dB/cm with the waveguide width shrinking from 500 to 300 nm while the 200-nm-wide waveguides exhibit quite large loss (>70 dB/cm) mainly due to the relatively rough sidewall of waveguides induced by the polySi dry etch. By modifying the process sequence, i.e., first patterning the a-Si layer into waveguides by dry etch and then SPC, the sidewall roughness is significantly improved but the polySi crystallinity is degraded, leading to 13.9 dB/cm loss in the 200-nm-wide waveguides while larger losses in the wider waveguides. Phosphorus implantation causes an additional loss in the polySi waveguides. The doping-induced optical loss increases relatively slowly with the phosphorus concentration increasing up to 1 x 10(18) cm(-3), whereas the 5 x 10(18) cm(-3) doped waveguides exhibit large loss due to the dominant free carrier absorption. For all undoped polySi waveguides, further 1-2 dB/cm loss reduction is obtained by a standard forming gas (10%H(2) + 90%N(2)) annealing owing to the hydrogen passivation of Si dangling bonds present in polySi waveguides, achieving the lowest loss of 7.9 dB/cm in the 300-nm-wide polySi waveguides. However, for the phosphorus doped polySi waveguides, the propagation loss is slightly increased by the forming gas annealing.

摘要

通过在二氧化硅(SiO₂)上沉积非晶硅(a-Si)并在最高温度1000℃下进行固相结晶(SPC),制备出宽度在200至500纳米范围内的多晶硅(polySi)线波导。当波导宽度从500纳米缩小到300纳米时,1550纳米处的传播损耗从13.0分贝/厘米降至9.8分贝/厘米,而200纳米宽的波导则表现出相当大的损耗(>70分贝/厘米),这主要是由于多晶硅干法蚀刻导致的波导侧壁相对粗糙。通过修改工艺顺序,即先通过干法蚀刻将a-Si层图案化为波导,然后进行SPC,侧壁粗糙度得到显著改善,但多晶硅结晶度下降,导致200纳米宽的波导损耗为13.9分贝/厘米,而较宽波导的损耗更大。磷离子注入会导致多晶硅波导出现额外损耗。随着磷浓度增加到1×10¹⁸厘米⁻³,掺杂引起的光学损耗增加相对缓慢,而5×10¹⁸厘米⁻³掺杂的波导则由于占主导地位的自由载流子吸收而表现出较大损耗。对于所有未掺杂的多晶硅波导,通过标准的形成气体(10%H₂ + 90%N₂)退火,由于多晶硅波导中存在的硅悬空键的氢钝化作用,进一步降低了1 - 2分贝/厘米的损耗,在300纳米宽的多晶硅波导中实现了7.9分贝/厘米的最低损耗。然而,对于磷掺杂的多晶硅波导,形成气体退火会使传播损耗略有增加。

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