{"title":"用于冰辅助电子束光刻技术的液氢温度低温恒温器","authors":"Rui Zheng;Limin Qi;Sizhuo Li;Zhihua Gan;Ding Zhao;Min Qiu","doi":"10.1109/TIM.2024.3485441","DOIUrl":null,"url":null,"abstract":"Liquid nitrogen (LN2) typically acts as a coolant in ice-assisted electron-beam lithography (iEBL) systems, so that the cryostage temperature cannot be lower than 77 K. To condense more gaseous precursors, such as carbon dioxide (CO2) in a high vacuum environment, a cooling system that does not rely on LN2 is necessary. In this article, we integrate a Gifford-McMahon (GM) cryocooler into the iEBL system, which can cool down samples from room temperature to 21 K in 2.25 h. The cold head and sample holder reach minimum temperatures of \n<inline-formula> <tex-math>$5.37~\\pm ~0.012$ </tex-math></inline-formula>\n K and \n<inline-formula> <tex-math>$19.14~\\pm ~0.009$ </tex-math></inline-formula>\n K, respectively, which lies within the temperature zone of liquid hydrogen. Furthermore, a gas-gap isolation system and discrete rotary valve are employed to minimize the vibration effects on the scanning electron microscope (SEM), with the vibration being limited to about 30 nm. Finally, CO2 has been investigated as the precursor, revealing itself as the second positive resist in iEBL, with a critical dose one order of magnitude less than water ice. Gold nanostructures are also successfully fabricated using such a resist. Our system achieves the lowest temperature in iEBL system to date, substantially expanding the range of precursors that can be used in iEBL.","PeriodicalId":13341,"journal":{"name":"IEEE Transactions on Instrumentation and Measurement","volume":"73 ","pages":"1-4"},"PeriodicalIF":5.6000,"publicationDate":"2024-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Liquid Hydrogen Temperature Cryostage for Ice-Assisted Electron-Beam Lithography\",\"authors\":\"Rui Zheng;Limin Qi;Sizhuo Li;Zhihua Gan;Ding Zhao;Min Qiu\",\"doi\":\"10.1109/TIM.2024.3485441\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Liquid nitrogen (LN2) typically acts as a coolant in ice-assisted electron-beam lithography (iEBL) systems, so that the cryostage temperature cannot be lower than 77 K. To condense more gaseous precursors, such as carbon dioxide (CO2) in a high vacuum environment, a cooling system that does not rely on LN2 is necessary. In this article, we integrate a Gifford-McMahon (GM) cryocooler into the iEBL system, which can cool down samples from room temperature to 21 K in 2.25 h. The cold head and sample holder reach minimum temperatures of \\n<inline-formula> <tex-math>$5.37~\\\\pm ~0.012$ </tex-math></inline-formula>\\n K and \\n<inline-formula> <tex-math>$19.14~\\\\pm ~0.009$ </tex-math></inline-formula>\\n K, respectively, which lies within the temperature zone of liquid hydrogen. Furthermore, a gas-gap isolation system and discrete rotary valve are employed to minimize the vibration effects on the scanning electron microscope (SEM), with the vibration being limited to about 30 nm. Finally, CO2 has been investigated as the precursor, revealing itself as the second positive resist in iEBL, with a critical dose one order of magnitude less than water ice. Gold nanostructures are also successfully fabricated using such a resist. Our system achieves the lowest temperature in iEBL system to date, substantially expanding the range of precursors that can be used in iEBL.\",\"PeriodicalId\":13341,\"journal\":{\"name\":\"IEEE Transactions on Instrumentation and Measurement\",\"volume\":\"73 \",\"pages\":\"1-4\"},\"PeriodicalIF\":5.6000,\"publicationDate\":\"2024-10-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Transactions on Instrumentation and Measurement\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/10739984/\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Transactions on Instrumentation and Measurement","FirstCategoryId":"5","ListUrlMain":"https://ieeexplore.ieee.org/document/10739984/","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Liquid Hydrogen Temperature Cryostage for Ice-Assisted Electron-Beam Lithography
Liquid nitrogen (LN2) typically acts as a coolant in ice-assisted electron-beam lithography (iEBL) systems, so that the cryostage temperature cannot be lower than 77 K. To condense more gaseous precursors, such as carbon dioxide (CO2) in a high vacuum environment, a cooling system that does not rely on LN2 is necessary. In this article, we integrate a Gifford-McMahon (GM) cryocooler into the iEBL system, which can cool down samples from room temperature to 21 K in 2.25 h. The cold head and sample holder reach minimum temperatures of
$5.37~\pm ~0.012$
K and
$19.14~\pm ~0.009$
K, respectively, which lies within the temperature zone of liquid hydrogen. Furthermore, a gas-gap isolation system and discrete rotary valve are employed to minimize the vibration effects on the scanning electron microscope (SEM), with the vibration being limited to about 30 nm. Finally, CO2 has been investigated as the precursor, revealing itself as the second positive resist in iEBL, with a critical dose one order of magnitude less than water ice. Gold nanostructures are also successfully fabricated using such a resist. Our system achieves the lowest temperature in iEBL system to date, substantially expanding the range of precursors that can be used in iEBL.
期刊介绍:
Papers are sought that address innovative solutions to the development and use of electrical and electronic instruments and equipment to measure, monitor and/or record physical phenomena for the purpose of advancing measurement science, methods, functionality and applications. The scope of these papers may encompass: (1) theory, methodology, and practice of measurement; (2) design, development and evaluation of instrumentation and measurement systems and components used in generating, acquiring, conditioning and processing signals; (3) analysis, representation, display, and preservation of the information obtained from a set of measurements; and (4) scientific and technical support to establishment and maintenance of technical standards in the field of Instrumentation and Measurement.