• Title/Summary/Keyword: vertical tunneling operation

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Sub-10 nm Ge/GaAs Heterojunction-Based Tunneling Field-Effect Transistor with Vertical Tunneling Operation for Ultra-Low-Power Applications

  • Yoon, Young Jun;Seo, Jae Hwa;Cho, Seongjae;Kwon, Hyuck-In;Lee, Jung-Hee;Kang, In Man
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.16 no.2
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    • pp.172-178
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    • 2016
  • In this paper, we propose a sub-10 nm Ge/GaAs heterojunction-based tunneling field-effect transistor (TFET) with vertical band-to-band tunneling (BBT) operation for ultra-low-power (LP) applications. We design a stack structure that is based on the Ge/GaAs heterojunction to realize the vertical BBT operation. The use of vertical BBT operations in devices results in excellent subthreshold characteristics with a reduction in the drain-induced barrier thinning (DIBT) phenomenon. The proposed device with a channel length ($L_{ch}$) of 5 nm exhibits outstanding LP performance with a subthreshold swing (S) of 29.1 mV/dec and an off-state current ($I_{off}$) of $1.12{\times}10^{-11}A/{\mu}m$. In addition, the use of the highk spacer dielectric $HfO_2$ improves the on-state current ($I_{on}$) with an intrinsic delay time (${\tau}$) because of a higher fringing field. We demonstrate a sub-10 nm LP switching device that realizes a good S and lower $I_{off}$ at a lower supply voltage ($V_{DD}$) of 0.2 V.

Electrical Characteristics of Tunneling Field-effect Transistors using Vertical Tunneling Operation Based on AlGaSb/InGaAs

  • Kim, Bo Gyeong;Kwon, Ra Hee;Seo, Jae Hwa;Yoon, Young Jun;Jang, Young In;Cho, Min Su;Lee, Jung-Hee;Cho, Seongjae;Kang, In Man
    • Journal of Electrical Engineering and Technology
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    • v.12 no.6
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    • pp.2324-2332
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    • 2017
  • This paper presents the electrical performances of novel AlGaSb/InGaAs heterojunction-based vertical-tunneling field-effect transistor (VTFET). The device performance was investigated in views of the on-state current ($I_{on}$), drain-induced barrier thinning (DIBT), and subthreshold swing (SS) as the gate length ($L_G$) was scaled down. The proposed TFET with a $L_G$ of 5 nm operated with an $I_{on}$ of $1.3mA/{\mu}m$, a DIBT of 40 mV/V, and an SS of 23 mV/dec at a drain voltage ($V_{DS}$) of 0.23 V. The proposed TFET provided approximately 25 times lower DIBT and 12 times smaller SS compared with the conventional $L_G$ of 5 nm TFET. The AlGaSb/InGaAs VTFET showed extremely high scalability and strong immunity against short-channel effects.

A Study of Memory Device based on Tunneling Mechanism (터널링 메커니즘을 이용한 메모리 소자 연구)

  • Lee Jun-Ha
    • Journal of the Semiconductor & Display Technology
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    • v.5 no.1 s.14
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    • pp.17-20
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    • 2006
  • This paper presents of a new type of memory cell that could potentially replace both DRAM and flash memory. The proposed device cell operates by sensing the state of about 1,000 electrons trapped between unique insulating barriers in the channel region of the upper transistor. These electrons are controlled by a side gate on the transistor, and their state in turn controls the gate of the larger transistor, providing signal gain within the memory cell. It becomes faster and more reliable memory with lower operation voltage. Moreover, the use of a multiple tunnel junction (MTJ) fur the vertical transistor can significantly improve the data retention and operation speed.

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Design of MTP memory IP using vertical PIP capacitor (Vertical PIP 커패시터를 이용한 MTP 메모리 IP 설계)

  • Kim, Young-Hee;Cha, Jae-Han;Jin, Hongzhou;Lee, Do-Gyu;Ha, Pan-Bong;Park, Mu-Hun
    • The Journal of Korea Institute of Information, Electronics, and Communication Technology
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    • v.13 no.1
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    • pp.48-57
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    • 2020
  • MCU used in applications such as wireless chargers and USB type-C require MTP memory with a small cell size and a small additional process mask. Conventional double poly EEPROM cells are small in size, but additional processing masks of about 3 to 5 sheets are required, and FN tunneling type single poly EEPROM cells have a large cell size. In this paper, a 110nm MTP cell using a vertical PIP capacitor is proposed. The erase operation of the proposed MTP cell uses FN tunneling between FG and EG, and the program operation uses CHEI injection method, which reduces the MTP cell size to 1.09㎛2 by sharing the PW of the MTP cell array. Meanwhile, MTP memory IP required for applications such as USB type-C needs to operate over a wide voltage range of 2.5V to 5.5V. However, the pumping current of the VPP charge pump is the lowest when the VCC voltage is the minimum 2.5V, while the ripple voltage is large when the VCC voltage is 5.5V. Therefore, in this paper, the VPP ripple voltage is reduced to within 0.19V through SPICE simulation because the pumping current is suppressed to 474.6㎂ even when VCC is increased by controlling the number of charge pumps turned on by using the VCC detector circuit.

Characterization of the Vertical Position of the Trapped Charge in Charge-trap Flash Memory

  • Kim, Seunghyun;Kwon, Dae Woong;Lee, Sang-Ho;Park, Sang-Ku;Kim, Youngmin;Kim, Hyungmin;Kim, Young Goan;Cho, Seongjae;Park, Byung-Gook
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.17 no.2
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    • pp.167-173
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    • 2017
  • In this paper, the characterization of the vertical position of trapped charges in the charge-trap flash (CTF) memory is performed in the novel CTF memory cell with gate-all-around structure using technology computer-aided design (TCAD) simulation. In the CTF memories, injected charges are not stored in the conductive poly-crystalline silicon layer in the trapping layer such as silicon nitride. Thus, a reliable technique for exactly locating the trapped charges is required for making up an accurate macro-models for CTF memory cells. When a programming operation is performed initially, the injected charges are trapped near the interface between tunneling oxide and trapping nitride layers. However, as the program voltage gets higher and a larger threshold voltage shift is resulted, additional charges are trapped near the blocking oxide interface. Intrinsic properties of nitride including trap density and effective capture cross-sectional area substantially affect the position of charge centroid. By exactly locating the charge centroid from the charge distribution in programmed cells under various operation conditions, the relation between charge centroid and program operation condition is closely investigated.