Substrate temperature measurement and control by emissivity compensated pyrometry during metalorganic vapor phase epitaxy of III-V device structures in large scale rotating disc reactors

J. Ramer, B. Patel, V. Boguslavskiy, A. Patel, M. Schurman, A. Gurary
{"title":"Substrate temperature measurement and control by emissivity compensated pyrometry during metalorganic vapor phase epitaxy of III-V device structures in large scale rotating disc reactors","authors":"J. Ramer, B. Patel, V. Boguslavskiy, A. Patel, M. Schurman, A. Gurary","doi":"10.1109/LEOSST.2000.869727","DOIUrl":null,"url":null,"abstract":"The growth process for many III-V semiconductor devices is quite temperature sensitive. The temperature window for some of the more challenging device structures can be as narrow as 2-3/spl deg/C, depending upon how tight the final device specifications are. Clearly, measurement and control of the growth temperature in a MOVPE production environment is critical to maintaining high yields from the growth process. We have solved this problem by using a pyrometric technique known as emissivity compensated pyrometry. This in-situ measurement technique requires the combined functionality of a conventional pyrometer and a reflectometer. The reflectance of the substrate is measured at the same wavelength that the pyrometer measures the thermal radiance. By using the equation /spl epsi/=1-R the spectral directional emissivity of the substrate surface can be calculated from the measured spectral directional reflectivity. This allows the measured thermal emission to be constantly corrected for the changing emissivity of the growth surface. In this way, the accurate temperature of the substrate can be measured at any time during growth.","PeriodicalId":415720,"journal":{"name":"2000 Digest of the LEOS Summer Topical Meetings. Electronic-Enhanced Optics. Optical Sensing in Semiconductor Manufacturing. Electro-Optics in Space. Broadband Optical Networks (Cat. No.00TH8497)","volume":"24 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2000-07-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2000 Digest of the LEOS Summer Topical Meetings. Electronic-Enhanced Optics. Optical Sensing in Semiconductor Manufacturing. Electro-Optics in Space. Broadband Optical Networks (Cat. No.00TH8497)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/LEOSST.2000.869727","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

The growth process for many III-V semiconductor devices is quite temperature sensitive. The temperature window for some of the more challenging device structures can be as narrow as 2-3/spl deg/C, depending upon how tight the final device specifications are. Clearly, measurement and control of the growth temperature in a MOVPE production environment is critical to maintaining high yields from the growth process. We have solved this problem by using a pyrometric technique known as emissivity compensated pyrometry. This in-situ measurement technique requires the combined functionality of a conventional pyrometer and a reflectometer. The reflectance of the substrate is measured at the same wavelength that the pyrometer measures the thermal radiance. By using the equation /spl epsi/=1-R the spectral directional emissivity of the substrate surface can be calculated from the measured spectral directional reflectivity. This allows the measured thermal emission to be constantly corrected for the changing emissivity of the growth surface. In this way, the accurate temperature of the substrate can be measured at any time during growth.
大型转盘反应器III-V型金属有机气相外延器件结构中衬底温度的测量与控制
许多III-V型半导体器件的生长过程对温度非常敏感。一些更具挑战性的器件结构的温度窗口可能窄至2-3/spl度/C,具体取决于最终器件规格的严格程度。显然,在MOVPE生产环境中测量和控制生长温度对于保持生长过程的高产量至关重要。我们已经解决了这个问题,通过使用高温测量技术称为发射率补偿高温测量。这种原位测量技术需要结合传统高温计和反射计的功能。基材的反射率是在高温计测量热辐射的同一波长测量的。利用/spl epsi/=1-R的公式,可以由测量的光谱定向反射率计算出衬底表面的光谱定向发射率。这使得测量的热发射可以不断地校正生长表面发射率的变化。这样,可以在生长过程中随时测量衬底的精确温度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信