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. 2024 Sep 4;19(1):140.
doi: 10.1186/s11671-024-04096-4.

FS-iTFET: advancing tunnel FET technology with Schottky-inductive source and GAA design

Affiliations

FS-iTFET: advancing tunnel FET technology with Schottky-inductive source and GAA design

Jyi-Tsong Lin et al. Discov Nano. .

Abstract

In this paper, we introduce a novel Forkshape nanosheet Inductive Tunnel Field-Effect Transistor (FS-iTFET) featuring a Gate-All-Around structure and a full-line tunneling heterojunction channel. The overlapping gate and source contact regions create a strong and uniform electric field in the channel. Furthermore, the metal-semiconductor Schottky junction in the intrinsic source region induces the required carriers without the need for doping. This innovative design achieves both a steeper subthreshold swing (SS) and a higher ON-state current (ION). Using calibration-based simulations with Sentaurus TCAD, we compare the performance of three newly designed device structures: the conventional Nanosheet Tunnel Field-Effect Transistor (NS-TFET), the Nanosheet Line-tunneling TFET (NS-LTFET), and the proposed FS-iTFET. Simulation results show that, compared to the traditional NS-TFET, the NS-LTFET with its full line-tunneling structure improves the average subthreshold swing (SSAVG) by 19.2%. More significantly, the FS-iTFET, utilizing the Schottky-inductive source, further improves the SSAVG by 49% and achieves a superior ION/IOFF ratio. Additionally, we explore the impact of Trap-Assisted Tunneling on the performance of the three different integrations. The FS-iTFET consistently demonstrates superior performance across various metrics, highlighting its potential in advancing tunnel field-effect transistor technology.

Keywords: Forkshape; Gate ALL around (GAA); Heterojunction; Line tunneling; Metal–semiconductor interface; Nanosheet; Schottky barrier; Subthreshold swing (SS); Tunnel field-effect transistor (TFET).

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Conflict of interest statement

The authors declare no competing interests.

Figures

Fig. 1
Fig. 1
Schematic device structures of a the 3-D structure of Forkshape Inductive Tunnel Field-Effect Transistor (FS-iTFET), b the cross-sectional view of traditional PIN Nanosheet TFET (NS-TFET), c the cross-sectional view of Nanosheet Line-tunneling TFET (NS-LTFET), and d the cross-sectional view of single stack FS-iTFET for performance comparison. Where, the cutlines A–A’, C–C’, and E–E’ are set 1 nm under the Silicon Channel/HfO2 interface; the cutlines B–B’, D–D’, and F–F’ are set 5 nm next to the left Spacer/Silicon Channel interface
Fig. 2
Fig. 2
Calibrations for a carrier transport, mobility, and quantum correction model [22], and b BTBT and SRH-TAT model [23]
Fig. 3
Fig. 3
al Cross-sectional views of key fabrication process steps for FS-iTFET
Fig. 4
Fig. 4
Performance comparison of NS-TFET, NS-LTFET, and FS-iTFET: a Transfer characteristics for different structures, b Corresponding subthreshold swing (SS) versus drain current, c Corresponding transconductance (gm) versus gate voltage, d SS behavior and ION/IOFF comparison of different structures
Fig. 5
Fig. 5
Energy band diagrams of NS-TFET, NS-LTFET, and FS-iTFET in different operational states: a, b Energy band diagrams of NS-TFET along cutlines A–A’ and B–B’, c, d Energy band diagrams of NS-LTFET along cutlines C–C’ and D–D’, e, f Energy band diagrams of FS-iTFET along cutlines E-E’ and D-D’
Fig. 6
Fig. 6
Cross-sectional comparison of the electron band-to-band tunneling (BTBT) generation rate for NS-TFET, NS-LTFET, and FS-iTFET
Fig. 7
Fig. 7
a Hole density along cutline I-I’ in a FS-iTFET, b Electric field diagram along the silicon channel for NS-LTFET and FS-iTFET, respectively
Fig. 8
Fig. 8
a Transfer characteristics of FS-iTFET with different Schottky Barrier Heights (SBH), b Corresponding subthreshold swing (SS) versus drain current, c Corresponding hole density along cutline I-I’, and d Corresponding band diagram along cutline I-I’
Fig. 9
Fig. 9
a Transfer characteristics of FS-iTFET with different channel/source materials, b Corresponding subthreshold swing (SS) versus drain current
Fig. 10
Fig. 10
a Transfer characteristics of FS-iTFET with and without inner oxide between the source/drain region, b-1 Cross-sectional view of FS-iTFET with inner oxide between the source/drain region, b-2 Cross-sectional view of FS-iTFET without inner oxide between the source/drain region, c, d Energy band diagram of NS-TFET in the OFF-state along cutlines G–G’ and H–H’. Where the cutlines G–G’ and H–H’ are set 1 nm below the silicon channel/germanium source interface
Fig. 11
Fig. 11
Electron band-to-band tunneling (BTBT) generation rate of FS-iTFET with and without inner oxide between the source/drain region
Fig. 12
Fig. 12
a Transfer characteristics of FS-iTFET with interface trap density (Nit) between Si/Ge, comparing different models, b Transfer characteristics of FS-iTFET with varying Nit between Si/Ge, c Transfer characteristics of FS-iTFET with Nit between Si/Ge, comparing different temperatures, d Corresponding subthreshold swing (SS) versus drain current at different temperatures
Fig. 13
Fig. 13
a Transfer characteristics of the corresponding device structure with interface traps between heterojunctions, b Corresponding subthreshold swing (SS) versus drain current, c Impact of interface traps between heterojunctions on ION in different structures, d Impact of interface traps between heterojunctions on IOFF in different structures
Fig. 14
Fig. 14
Benchmark comparison of the ION/IOFF ratio and average subthreshold swing (SSavg) of our devices with those proposed in other papers
Fig. 15
Fig. 15
Impact of subband quantum confinement effect (QCE) on FS-iTFET: a Transfer characteristics of FS-iTFET with and without subband QCE, b Corresponding subthreshold swing (SS) versus drain current
Fig. 16
Fig. 16
Impact of channel/source thickness on FS-iTFET: a Transfer characteristics of FS-iTFET for different channel/source thicknesses, b Corresponding subthreshold swing (SS) versus drain current

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References

    1. Kumar S, Tiwari P, Zymbler M. Internet of Things is a revolutionary approach for future technology enhancement: a review. J Big Data. 2019;6:111. 10.1186/s40537-019-0268-2.10.1186/s40537-019-0268-2 - DOI
    1. Boucart K, Ionescu AM. Double Gate Tunnel FET with ultrathin silicon body and high-k gate dielectric. In: 2006 European solid-state device research conference. Switzerland: Montreux; 2006. pp. 383–386. 10.1109/ESSDER.2006.307718.
    1. Choi WY, Park B-G, Lee JD, Liu T-JK. Tunneling field-effect transistors (TFETs) with subthreshold swing (SS) less than 60 mV/dec. IEEE Electron Device Lett. 2007;28(8):743–5. 10.1109/LED.2007.901273.10.1109/LED.2007.901273 - DOI
    1. Ionescu AM, Riel H. Tunnel feld-efect transistors as energy-efcient electronic switches. Nature. 2011;479(7373):329–37. 10.1038/nature10679. 10.1038/nature10679 - DOI - PubMed
    1. Molaei Imenabadi R, Saremi M, Vandenberghe WG. A novel PNPN-like Z-shaped tunnel field- effect transistor with improved ambipolar behavior and RF performance. IEEE Trans Electron Dev. 2017;64(11):4752–8. 10.1109/TED.2017.2755507.10.1109/TED.2017.2755507 - DOI

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