Effect of Device Parameters on Carbon Nanotube Field Effect Transistor in Nanometer Regime

2015 ◽  
Vol 36 ◽  
pp. 64-75 ◽  
Author(s):  
Sanjeet Kumar Sinha ◽  
Saurabh Chaudhury

In this paper, we have analyzed the effect of chiral vector, temperature, metal work function, channel length and High-K dielectric on threshold voltage of CNTFET devices. We have also compared the effect of oxide thickness on gate capacitance and justified the advantage a CNTFET provides over MOSFET in nanometer regime. Simulation on HSPICE tool shows that high threshold voltage can be achieved at low chiral vector pair in CNTFET. It is also observed that the temperature has a negligible effect on threshold voltage of CNTFET. After that we have simulated and observed the effect of channel length variation on threshold voltage of CNTFET as well as MOSFET devices and given a theoretical analysis on it. We found an unusual, yet, favorable characteristics that the threshold voltage increases with decreasing channel length in CNTFET devices in deep nanometer regime.

2002 ◽  
Vol 716 ◽  
Author(s):  
Krishna Kumar Bhuwalka ◽  
Nihar R. Mohapatra ◽  
Siva G. Narendra ◽  
V Ramgopal Rao

AbstractIt has been shown recently that the short channel performance worsens for high-K dielectric MOSFETs as the physical thickness to the channel length ratio increases, even when the effective oxide thickness (EOT) is kept identical to that of SiO2. In this work we have systematically evaluated the effective dielectric thickness for different Kgate to achieve targeted threshold voltage (Vt), drain-induced barrier lowering (DIBL) and Ion/Ioff ratio for different technology generations down to 50 nm using 2-Dimensional process and device simulations. Our results clearly show that the oxide thickness scaling for high-K gate dielectrics and SiO2 follow different trends and the fringing field effects must be taken into account for estimation of effective dielectric thickness when SiO2 is replaced by a high-K dielectric.


AIP Advances ◽  
2021 ◽  
Vol 11 (6) ◽  
pp. 065229
Author(s):  
Yanxiao Sun ◽  
Gang Niu ◽  
Wei Ren ◽  
Jinyan Zhao ◽  
Yankun Wang ◽  
...  

Nanomaterials ◽  
2019 ◽  
Vol 9 (8) ◽  
pp. 1085 ◽  
Author(s):  
Kemelbay ◽  
Tikhonov ◽  
Aloni ◽  
Kuykendall

As one of the highest mobility semiconductor materials, carbon nanotubes (CNTs) have been extensively studied for use in field effect transistors (FETs). To fabricate surround-gate FETs— which offer the best switching performance—deposition of conformal, weakly-interacting dielectric layers is necessary. This is challenging due to the chemically inert surface of CNTs and a lack of nucleation sites—especially for defect-free CNTs. As a result, a technique that enables integration of uniform high-k dielectrics, while preserving the CNT’s exceptional properties is required. In this work, we show a method that enables conformal atomic layer deposition (ALD) of high-k dielectrics on defect-free CNTs. By depositing a thin Ti metal film, followed by oxidation to TiO2 under ambient conditions, a nucleation layer is formed for subsequent ALD deposition of Al2O3. The technique is easy to implement and is VLSI-compatible. We show that the ALD coatings are uniform, continuous and conformal, and Raman spectroscopy reveals that the technique does not induce defects in the CNT. The resulting bilayer TiO2/Al2O3 thin-film shows an improved dielectric constant of 21.7 and an equivalent oxide thickness of 2.7 nm. The electrical properties of back-gated and top-gated devices fabricated using this method are presented.


2001 ◽  
Vol 686 ◽  
Author(s):  
Michele L. Ostraat ◽  
Jan W. De Blauwe

AbstractA great deal of research interest is being invested in the fabrication and characterization of nanocrystal structures as charge storage memory devices. In these flash memory devices, it is possible to measure threshold voltage shifts due to charge storage of only a few electrons per nanocrystal at room temperature. Although a variety of methods exist to fabricate nanocrystals and to incorporate them into device layers, control over the critical nanocrystal dimensions, tunnel oxide thickness, and interparticle separation and isolation remains difficult to achieve. This control is vital to produce reliable and consistent devices over large wafer areas. To address these control issues, we have developed a novel two-stage ultra clean reactor in which the Si nanocrystals are generated as single crystal, nonagglomerated, spherical aerosol particles from silane decomposition at 950°C at concentrations exceeding 108 cm−3 at sizes below 10 nm. Using existing aerosol instrumentation, it is possible to control the particle size to approximately 10% on diameter. In the second reactor, particles are passivated with a high quality oxide layer with shell thickness controllable from 0.7 to 2.0 nm. The two-stage aerosol reactor is integrated to a 200 mm wafer deposition chamber such that controlled particle densities can be deposited thermophoretically. With nanocrystal deposits of 1013 cm−2, contamination of transition metals and other elements can be controlled to less than 1010 atoms cm−2.We have fabricated 0.2 μm channel length aerosol nanocrystal floating gate memory devices using conventional MOS ULSI processing on 200 mm wafers. The aerosol nanocrystal memory devices exhibit normal transistor characteristics with drive current 30 μA/μm, subthreshold slope 200 mV/dec, and drain induced barrier lowering 100 mV/V, typical values for thick gate dielectric high substrate doped nonvolatile memory devices. Uniform Fowler-Nordheim tunneling is used to program and erase these memory devices. Despite 5 nm tunnel oxides, threshold voltage shifts > 2 V have been achieved with microsecond program and millisecond erase times at moderate operating voltages. The aerosol devices also exhibit excellent endurance cyclability with no window closure observed after 105 cycles. Furthermore, reasonable disturb times and long nonvolatility are obtained, illustrating the inherent advantage of discrete nanocrystal charge storage. No drain disturb was detected even at drain biases of 4V, indicating that little or no charge conduction occurs in the nanocrystal layer. We have demonstrated promise for aerosol nanocrystal memory devices. However, numerous issues exist for the future of nanocrystal devices. These technology issues and challenges will be discussed as directions for future work.


2011 ◽  
Vol 6 (2) ◽  
pp. 102-106
Author(s):  
Milene Galeti ◽  
Michele Rodrigues ◽  
Nadine Collaert ◽  
Eddy Simoen ◽  
Cor Claeys ◽  
...  

This work presents an analysis of the analog performance of SOI MuGFET devices and the impact of different TiN metal gate electrode thickness.Thinner TiN metal gate allows achieving large gain and this effect can be attributed to the increased Early voltage values observed for thinner TiN metal gate. This VEA increase suggests an increase of the transversal electrical field for thin TiN metal gate (reduced gate oxide thickness) that is confirmed with the increment of the GIDL current.This impact on the voltage gain is maintained for short channel length.The impact of different gate dielectrics was also studied where high-k dielectric indicated a higher VT due to a VFB variation. Additionally, lower intrinsic voltage gain was observed for hafnium dielectric and this can be related to the lower Early voltage (VEA) present in this devices.


2021 ◽  
Author(s):  
Vidyadhar Gupta ◽  
Himanshi Awasthi ◽  
Nitish Kumar ◽  
Amit Kumar Pandey ◽  
ABHINAV GUPTA

Abstract This present article interprets the analytical models of central channel potential, the threshold voltage, and subthreshold current for Graded-Doped Junctionless-Gate-All-Around (GD-JL-GAA) MOSFETs. The parabolic approximation equation with appropriate boundary conditions has been adopted to solve the 2D Poisson’s equation for determining the central channel potential. The minimum channel potential is obtained by potential channel expression, and it is utilized to determine the threshold voltage and subthreshold current by using the Drift-Diffusion method. The behaviour of GD-JL-GAA MOSFETs has been examined by varying physical device parameters such as doping concentration (NDn), channel thickness (tsi), oxide thickness (tox), and channel length ratio (L1 : L2). The mathematical analysis shows that the nominal gate leakage current in GD-JL-GAA MOSFETs due to high graded abrupt junction inside the channel region. The analytical model results have been verified with simulation data extracted from a TCAD simulator.


Author(s):  
Hakkee Jung

Transfer characteristics is presented using analytical potential distribution of accumulation-mode junctionless cylindrical surrounding-gate (JLCSG) MOSFET, and deviation of center electric field at threshold voltage is analyzed for channel length and oxide thickness. Threshold voltages presented in this paper is good agreement with results of other compared papers, and transfer characteristics is agreed with those of two-dimensional simulation. The most important factor to determine threshold voltage is center electric field at source because the greater part of electron flows through center axis of JLCSG MOSFET. As a result of analysis for center electric field at threshold voltage, center electric field is decreased with reduction of channel length due to drain induced barrier lowering. Center electric field is increased with decrease of oxide thickness, and deviation of center electric field for channel length is significantly occurred with decrease of oxide thickness.


Author(s):  
Hakkee Jung

In this paper, the subthreshold swing was observed when the stacked high-k gate oxide was used for a junctionless double gate (JLDG) MOSFET. For this purpose, a subthreshold swing model was presented using the series-type potential model derived from the Poisson equation. The results of the model presented in this paper were in good agreement with the two-dimensional numerical values and those from other papers. Using this model, the variation of the subthreshold swing for the channel length, silicon thickness, gate oxide thickness, and dielectric constant of the stacked high-k material was observed using the dielectric constant as a parameter. As a result, the subthreshold swing was reduced when the high-k materials were used as the stacked gate oxide film. In the case of the asymmetric structure, the subthreshold swing can be reduced than that of the symmetric JLDG MOSFET when the dielectric constant of the bottom stacked oxide film was greater than that of the top stacked oxide film. In the case of the asymmetric structure, the subthreshold swing could be also reduced by applying the bottom gate voltage lower than the top gate voltage.


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