• Title/Summary/Keyword: JLFET

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Comparison of Electrical Coupling of Monolithic 3D Inverter with MOSFET and JLFET (MOSFET와 JLFET의 3차원 인버터 전기적 상호작용의 비교)

  • Ahn, Tae-Jun;Choi, Bum Ho;Yu, Yun Seop
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2018.05a
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    • pp.173-174
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    • 2018
  • This paper compared the electrical coupling of the monolithic 3D inverter consisting of MOSFET and JLFET. In the case of both the MOSFET and the JLFET, MOSFET and JLFET have a small threshold voltage variation when the thickness of inter-layer dielectric (ILD) = 100 nm. However, when the thickness of ILD = 10 nm, the threshold voltage variation is larger and the JLFET is twice as much as the MOSFET.

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Electrical Coupling of Monolithic 3D Inverter Consisting of Junctionless FET (Junctionless FET로 구성된 적층형 3차원 인버터의 전기적 상호작용에 대한 연구)

  • Jang, Ho-Yeong;Kim, Kyung-won;Ahn, Tae-Jun;Yu, Yun Seop
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2016.10a
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    • pp.614-615
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    • 2016
  • I studied electrical coupling of monolithic 3D inverter(M3D-INV) consisting of Junctionless FET(JLFET). If the thickness of Inter Layer Dielectric (ILD) between top JLFET and bottom JLFET is less than 50nm, current-voltage characteristic of top JLFET is rapidly changed by the gate voltage of bottom JLFET. Therefore, you have to consider about the electrical interaction according to the thickness between top JLFET and bottom JLFET in M3D-INV.

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AC Electrical Coupling of Monolithic 3D Inverter Consisting of Junctionless FET (Junctionless FET로 구성된 적층형 3차원 인버터의 AC 특성에 대한 연구)

  • Kim, Kyung-won;Ahn, Tae-Jun;Yu, Yun Seop
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2017.05a
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    • pp.529-530
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    • 2017
  • Electrical coupling of monolithic 3D inverter(M3D-INV) consisting of Junctionless FET(JLFET) was investigated. Depending on the thickness of Inter Layer Dielectirc (ILD) between top and bottom JLFETs, $N_{gate}-N_{gate}$ capacitance and transconductance $g_m$ are changed by the gate voltage of bottom JLFET. Therefore, when using a stacked structure with the ILD below tens nm, AC electrical coupling between two transistors in M3D-INV should be considered.

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High-Speed Low-Power Junctionless Field-Effect Transistor with Ultra-Thin Poly-Si Channel for Sub-10-nm Technology Node

  • Kim, Youngmin;Lee, Junsoo;Cho, Yongbeom;Lee, Won Jae;Cho, Seongjae
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.16 no.2
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    • pp.159-165
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    • 2016
  • Recently, active efforts are being made for future Si CMOS technology by various researches on emerging devices and materials. Capability of low power consumption becomes increasingly important criterion for advanced logic devices in extending the Si CMOS. In this work, a junctionless field-effect transistor (JLFET) with ultra-thin poly-Si (UTP) channel is designed aiming the sub-10-nm technology for low-power (LP) applications. A comparative study by device simulations has been performed for the devices with crystalline and polycrystalline Si channels, respectively, in order to demonstrate that the difference in their performances becomes smaller and eventually disappears as the 10-nm regime is reached. The UTP JLFET would be one of the strongest candidates for advanced logic technology, with various virtues of high-speed operation, low power consumption, and low-thermal-budget process integration.

Si CMOS Extension and Ge Technology Perspectives Forecast Through Metal-oxide-semiconductor Junctionless Field-effect Transistor

  • Kim, Youngmin;Lee, Junsoo;Cho, Seongjae
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.16 no.6
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    • pp.847-853
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    • 2016
  • Applications of Si have been increasingly exploited and extended to More-Moore, More-than-Moore, and beyond-CMOS approaches. Ge is regarded as one of the supplements for Si owing to its higher carrier mobilities and peculiar band structure, facilitating both advanced and optical applications. As an emerging metal-oxide device, the junctionless field-effect transistor (JLFET) has drawn considerable attention because of its simple process, less performance fluctuation, and stronger immunity against short-channel effects due to the absence of anisotype junctions. In this study, we investigated lateral field scalability, which is equivalent to channel-length scaling, in Si and Ge JLFETs. Through this, we can determine the usability of Si CMOS and hypothesize its replacement by Ge. For simulations with high accuracy, we performed rigorous modeling for ${\mu}_n$ and ${\mu}_p$ of Ge, which has seldom been reported. Although Ge has much higher ${\mu}_n$ and ${\mu}_p$ than Si, its saturation velocity ($v_{sat}$) is a more determining factor for maximum $I_{on}$. Thus, there is still room for pushing More-Moore technology because Si and Ge have a slight difference in $v_{sat}$. We compared both p- and n-type JLFETs in terms of $I_{on}$, $I_{off}$, $I_{on}/I_{off}$, and swing with the same channel doping and channel length/thickness. $I_{on}/I_{off}$ is inherently low for Ge but is invariant with $V_{DS}$. It is estimated that More-Moore approach can be further driven if Si is mounted on a JLFET until Ge has a strong possibility to replace Si for both p- and n-type devices for ultra-low-power applications.

Investigation of Junction-less Tunneling Field Effect Transistor (JL-TFET) with Floating Gate

  • Ali, Asif;Seo, Dongsun;Cho, Il Hwan
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.17 no.1
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    • pp.156-161
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    • 2017
  • This work presents a novel structure for junction-less tunneling field effect transistor (JL-TFET) with a floating gate over the source region. Introduction of floating gate instead of fixed metal gate removes the limitation of fabrication process suitability. The proposed device is based on a heavily n-type-doped Si-channel junction-less field effect transistor (JLFET). A floating gate over source region and a control-gate with optimized metal work-function over channel region is used to make device work like a tunnel field effect transistor (TFET). The proposed device has exhibited excellent ID-VGS characteristics, ION/IOFF ratio, a point subthreshold slope (SS), and average SS for optimized device parameters. Electron charge stored in floating gate, isolation oxide layer and body doping concentration are optimized. The proposed JL-TFET can be a promising candidate for switching performances.