{"title":"揭示纳米片场效应管的输出电导动态:低温是否有影响?","authors":"Malvika , Prabhat Singh , Navjeet Bagga , Mohd. Shakir , Ankit Dixit , Naveen Kumar , Vihar Georgiev , S. Dasgupta","doi":"10.1016/j.sse.2026.109348","DOIUrl":null,"url":null,"abstract":"<div><div>Channel length modulation (CLM) and drain-induced barrier lowering (DIBL) are well-known short-channel effects that result in a finite output conductance (g<sub>ds</sub>). In a simplified analysis, g<sub>ds</sub> is predominantly governed by the drain voltage (V<sub>DS</sub>) and can be approximated by the slope of the I<sub>DS</sub>–V<sub>DS</sub> characteristics in the saturation regime. However, will the conceptual governance of g<sub>ds</sub> be the same at the cryogenic temperatures? To answer this question, we thoroughly investigate the Cryogenic Nanosheet FET (NSFET) using well-calibrated TCAD models. The results reveal that incomplete ionization in the cryogenic temperature (CT) regime provides additional expansion of the depletion at the drain side. This significantly increases g<sub>ds</sub> (i.e., the slope of the IDS-VDS characteristics) in CT compared to that at room temperature (RT). Therefore, in a Cryogenic FET, CLM becomes the function of temperature. Further, we extracted the CLM parameter (λ), early voltage (V<sub>A</sub>), and intrinsic gain (g<sub>max</sub>/g<sub>ds</sub>) of the Nanosheet FET with varying temperatures and found that the g<sub>max</sub>/g<sub>ds</sub> is maximum at 4 K.</div></div>","PeriodicalId":21909,"journal":{"name":"Solid-state Electronics","volume":"234 ","pages":"Article 109348"},"PeriodicalIF":1.4000,"publicationDate":"2026-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Unveiling the output conductance dynamics in Nanosheet FET: Does cryogenic temperature Make a Difference?\",\"authors\":\"Malvika , Prabhat Singh , Navjeet Bagga , Mohd. Shakir , Ankit Dixit , Naveen Kumar , Vihar Georgiev , S. Dasgupta\",\"doi\":\"10.1016/j.sse.2026.109348\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Channel length modulation (CLM) and drain-induced barrier lowering (DIBL) are well-known short-channel effects that result in a finite output conductance (g<sub>ds</sub>). In a simplified analysis, g<sub>ds</sub> is predominantly governed by the drain voltage (V<sub>DS</sub>) and can be approximated by the slope of the I<sub>DS</sub>–V<sub>DS</sub> characteristics in the saturation regime. However, will the conceptual governance of g<sub>ds</sub> be the same at the cryogenic temperatures? To answer this question, we thoroughly investigate the Cryogenic Nanosheet FET (NSFET) using well-calibrated TCAD models. The results reveal that incomplete ionization in the cryogenic temperature (CT) regime provides additional expansion of the depletion at the drain side. This significantly increases g<sub>ds</sub> (i.e., the slope of the IDS-VDS characteristics) in CT compared to that at room temperature (RT). Therefore, in a Cryogenic FET, CLM becomes the function of temperature. Further, we extracted the CLM parameter (λ), early voltage (V<sub>A</sub>), and intrinsic gain (g<sub>max</sub>/g<sub>ds</sub>) of the Nanosheet FET with varying temperatures and found that the g<sub>max</sub>/g<sub>ds</sub> is maximum at 4 K.</div></div>\",\"PeriodicalId\":21909,\"journal\":{\"name\":\"Solid-state Electronics\",\"volume\":\"234 \",\"pages\":\"Article 109348\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2026-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Solid-state Electronics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0038110126000183\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2026/2/8 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q3\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Solid-state Electronics","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0038110126000183","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/2/8 0:00:00","PubModel":"Epub","JCR":"Q3","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Unveiling the output conductance dynamics in Nanosheet FET: Does cryogenic temperature Make a Difference?
Channel length modulation (CLM) and drain-induced barrier lowering (DIBL) are well-known short-channel effects that result in a finite output conductance (gds). In a simplified analysis, gds is predominantly governed by the drain voltage (VDS) and can be approximated by the slope of the IDS–VDS characteristics in the saturation regime. However, will the conceptual governance of gds be the same at the cryogenic temperatures? To answer this question, we thoroughly investigate the Cryogenic Nanosheet FET (NSFET) using well-calibrated TCAD models. The results reveal that incomplete ionization in the cryogenic temperature (CT) regime provides additional expansion of the depletion at the drain side. This significantly increases gds (i.e., the slope of the IDS-VDS characteristics) in CT compared to that at room temperature (RT). Therefore, in a Cryogenic FET, CLM becomes the function of temperature. Further, we extracted the CLM parameter (λ), early voltage (VA), and intrinsic gain (gmax/gds) of the Nanosheet FET with varying temperatures and found that the gmax/gds is maximum at 4 K.
期刊介绍:
It is the aim of this journal to bring together in one publication outstanding papers reporting new and original work in the following areas: (1) applications of solid-state physics and technology to electronics and optoelectronics, including theory and device design; (2) optical, electrical, morphological characterization techniques and parameter extraction of devices; (3) fabrication of semiconductor devices, and also device-related materials growth, measurement and evaluation; (4) the physics and modeling of submicron and nanoscale microelectronic and optoelectronic devices, including processing, measurement, and performance evaluation; (5) applications of numerical methods to the modeling and simulation of solid-state devices and processes; and (6) nanoscale electronic and optoelectronic devices, photovoltaics, sensors, and MEMS based on semiconductor and alternative electronic materials; (7) synthesis and electrooptical properties of materials for novel devices.