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Development of a dynamic gas lock inhibited model for EUV-induced carbon deposition.
Hao, Ming; Teng, Shuai; Liu, Jiaxing; Xie, Yuanhua; Ba, Dechun; Bian, Xin; Ba, Yaoshuai; Chen, Zhengwei; Liu, Kun.
Afiliação
  • Hao M; School of Mechanical Engineering and Automation, Northeastern University, Shenyang, China.
  • Teng S; School of Mechanical Engineering and Automation, Northeastern University, Shenyang, China.
  • Liu J; Tobacco Machinery Co., Ltd., Qinhuangdao, China.
  • Xie Y; School of Mechanical Engineering and Automation, Northeastern University, Shenyang, China.
  • Ba D; School of Mechanical Engineering and Automation, Northeastern University, Shenyang, China.
  • Bian X; National Frontiers Science Center for Industrial Intelligence and Systems Optimization, Northeastern University, Shenyang, China.
  • Ba Y; Key Laboratory of Data Analytics and Optimization for Smart Industry (Northeastern University), Ministry of Education, Shenyang, China.
  • Chen Z; Institute of Fluid Engineering, Zhejiang University, Hangzhou, China.
  • Liu K; School of Mechanical Engineering and Automation, Northeastern University, Shenyang, China.
J Chem Phys ; 160(4)2024 Jan 28.
Article em En | MEDLINE | ID: mdl-38284653
ABSTRACT
The optical surface of extreme ultraviolet (EUV) lithography machines is highly vulnerable to contamination by hydrocarbons, resulting in the formation of carbon deposits that significantly degrade the quality and efficiency of lithography. The dynamic gas lock (DGL) has been proven as an effective approach to alleviate carbon deposition. However, the majority of existing studies on carbon deposition neglect the influence of the DGL. This paper is dedicated to investigating the phenomena of hydrocarbon adsorption, desorption, and cleavage with considering the effects of the DGL. A comprehensive mathematical model of the carbon deposition process is established, and the impact of radiation intensity, temperature, and hydrocarbon types on the depositing rate is considered. The results suggest that the primary cause of carbon deposition is the direct cracking of hydrocarbons induced by photons with a wavelength range between 12.5 and 14.5 nm. Additionally, it has been observed that the carbon deposition rate decreases exponentially as clean gas flow increases when EUV radiation intensity exceeds 50 mW/mm2. Conversely, at low EUV radiation intensity, clean gas flow has little effect on the carbon deposition rate. An effective approach to mitigate carbon deposition is to elevate the temperature of the optical surface and employ light hydrocarbon materials in the EUV process.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Revista: J Chem Phys Ano de publicação: 2024 Tipo de documento: Article País de afiliação: China

Texto completo: 1 Base de dados: MEDLINE Idioma: En Revista: J Chem Phys Ano de publicação: 2024 Tipo de documento: Article País de afiliação: China