Comparison of MOSFET, MESFET, FinFET and SOI-FinFET
INTRODUCTION
Now adays growth of technologies is rapid developed.
To this growth device structure plays basic and important role. basically, Transistors
are two types there are BJT (Bi-polar Junction Transistor) and FET (Field effect
transistor). The BJT having two types Npn and Pnp BJT and FET are also different
types they are MOSFET (Metal Oxide Semi-Conductor FET), FinFET, SOI-FinFET (Silicon
on Insulator FinFET), IGFET (Insulated Gate FET) and MESFET (Metal
Semi-Conductor FET) shown in below figure(a). every device having advantages
and disadvantages, suppose BJT and FET having some draw backs to overcome this,
MOSFET is implemented. Later while decreasing the channel length means reducing
the nano meters, MOSFET having drawbacks like short channel effect, parasitic
capacitance etc. To overcome these drawbacks FinFET is implemented. FinFET also
some drawbacks like DIBL (Drain Induced Barrier Lowering) to over this SOI-FinFET
is implemented. SOI-FinFET having good threshold swing compared FinFET and other
devices. DIBL is also very less in SOI-FinFET compared to the FinFET. Short channel
effect is less in SOI-FinFET compared to the FinFET and other devices.
SOI-FinFET gives good parameter in very low technologies. Cut Off Region: In cut,
off region transistor is in OFF state. Means current flow through the transistor
is ‘0’.
Saturation Region: In saturation region transistor
is in ON state and in this region, transistor acts as a closed switch. Means current
flow through the transistor is high.
Active Region: in this active region transistor acts as an amplifier.
Figure1: Transistor architecture
Theory
Basically, Field Effect Transistors (FET)
controls the flow of electrons and holes by using electric field. It is a
three-terminal device. Terminals are Gate, Source and Drain. These field effect
transistor uses electron or holes as charge carriers in operation. The
conductivity between source and drain is depending upon the gate voltage ‘Vg’.
If gate voltage is ‘1’ then the conductivity between source and drain is high.
If the gate voltage is ‘0’ then conductivity between source and drain is low.
We have different types of FETS, in that MOSFET is most widely used transistor.
MOSFET
MOSFET is having four terminals Source, Drain, Gate and Body. It is also known as Insulated gate FET. The MOSFET body terminal is always connected with source terminal. So, it forming three terminals like whereas FET. MOSFET is a transistor and it is used in both digital and analog circuits. It is voltage control device. In MOSFET, gate controls the flow of current from source to drain. MOSFET having two mode, one is Depletion Mode and an-other one is Enhancement Mode. In Depletion mode already inversion layer present without giving any voltage at gate terminal. if the gate voltage is ‘0’ then the current flow between Source and Drain is maximum. Else if gate voltage is not ‘0’ or increasing gradually, then the current flow between Source and Drain is ‘0’ or decreasing gradually. In Enhancement mode, normally there is no inversion layer present without giving gate voltage. If the gate voltage increasing gradually, then the current flow from Source to Drain increasing gradually. If there is no voltage on the gate terminal, then there is no current flow from Source to Drain. In MOSFET, while decreasing the Nano-meter technology short channel effect is increases. It consumes more power compared to the FinFET technology. The fabrication steps are more compared to the FinFET. Current leakage and Drain Induced Barrier Lowering are more compared to the FinFET.
Figure 2: (a) Structure of MOSFET. (b) N, P-channel MOSFET symbols. (c) N-channel Depletion mode and Enhancement mode MOSFET symbols.
FinFET
FinFET is totally different from the
MOSFET. In FinFET source and drain structure is look like a Fin and that Fin is
incusing into the substrate is shown in below figure. The channel surface is fully
surrounded by the gate. Because to get the good command on the channel. Then
gate having good control on the channel. In FinFET, doping of impurities is
very less compared to the MOSFET. In FinFET, direct connection between source, drain
and substrate due to this connection some amount of leakage takes place. Due to
the good control on the channel by gate terminal, leakages are highly reduced.
There are two ways to increase the drive current of FinFET device. One way of
increasing the width of the channel and another way is construct and connect
the multi-Fins together. Short channel effect (SCE) is also reduced due to the
less doping and good control by the gate. Compared to the SOI-FinFET, FinFET not
gives good parameter of SCE, DIBL, leakages, Power consumption and output current.
Figure 3: (a) FinFET Structure. (b) FinFET Symbols
MESFET
MESFET is a Metal Semiconductor Field Effect
Transistor. Depletion mode MESFET are widely and mostly used in the circuits. MESFET
having no oxide layer present between the gate and substrate. Schottky junction
is present in the place of oxide junction. The Schottky metal gate controls the
flow of electron from source to drain. MESFET having conducting channel between
the source and drain shown in the below Figure4. Compared to the MOSFET, MESFET
having higher mobility carriers in the channel. MESFET substrate is a semi-insulating substrate means MOSFET substrate is made with silicon, but in
MESFET the substrate is made with Gallium Arsenide (GaAs) or Indium Phosphide
or Silicon Carbide. In this paper considering semi-insulating GaAs substrate.
GaAs substrate provide two advantages compared to Silicon substrate. Frist, at
room temperature electron mobility is more than five times large. Second, fabrication
of Semi-Insulating GaAs substrate is possible and due to the free carrier absorption,
it overcomes the microwave power absorbing problem in the substrate. The flow of
current is controlled by varying the depletion region. Due to this, carriers
from the surface is separated by depletion region. Schottky diode turn on at
0.7V. if the gate voltage increases, it decreases the current flow between
source to drain, due to increasing the width of depletion region.
Figure 4: (a) MESFET structure. (b) MESFET symbol.
SOI-FinFET
SOI-FinFET is almost similar to the FinFET.
There is small difference i.e. The substrate of SOI-FinFET is fully occupied by
oxide layer or Buried Oxide layer (BOX). But in FinFET source and drain are
directly connected with the substrate and there is no oxide layer present
between the substrate and source, drain. Due to this BOX layer very, less leakages
will occur compared to the MOSFET, FinFET and MESFET. SOI-FinFET switches faster
than other devices like MOSFET, FinFET and MESFET. DIBL is also less compared to
the MOSFET, FinFET and MESFET. Gate terminal having more control on the channel
compared to the MOSFET, FINFET and MESFET. Drain current also more drawn at the
output and doping impurities is very less compared to the MOSFET, FinFET and
MESFET. The fabrication steps are also very less steps required compared to the
MOSFET, FinFET and MESFET.
Figure 5: SOI-FinFET Structure
DISCUSSION (MOSFET, MESFET, FinFET and SOI-FinFET)
Drain Induced Barrier Lowering
Due to the short channel effect DIBL will
occur. If we increasing the drain terminal voltage greater than gate voltage.
There is losing of connection between the source and drain. SOI-FinFET having
less DIBL value compared to other devices MOSFET, FinFET and MESFET. Because
SOI-FinFET doping impurities are very less compared to the MOSFET, FinFET and
MESFET. The values of the MOSFET, MESFET, FinFET and SOI-FinFET is shown below tabular
form and the graphical represent is also shown below.
Table 1: Comparison DIBL value of different
devices.
S.NO |
Devices |
DIBL
(mV) |
1 |
MOSFET |
47 |
2 |
MESFET |
120 |
3 |
FinFET |
0.000053 |
4 |
SOI-FinFET |
0.00005 |
Figure 6: Graphical representation of DIBL of different devices is shown in above.
Leakage Current
Current leakage is occurring mainly between source and drain when device in OFF state. MOSFET and MESFET current leakage is very high compared to the FinFET and SOI-FinFET. Compared to the SOI-FinFET (7.77x10^-8 nA), FinFET having more leakage is about 8.62x10^-8 nA. Current leakage of MOSFET, MESFET, FinFET and SOI-FinFET is shown below tabular form.
Table 2: Comparison
of current leakages of different devices.
S.NO |
Devices |
Leakage
Current |
1 |
MOSFET |
High |
2 |
MESFET |
High |
3 |
FinFET |
Less
(8.62x10^-8 nA) |
4 |
SOI-FinFET |
Very
Less (7.77x10^-8 nA) |
Short Channel Effect
Short channel effect will increase, by
decreasing the nano-meter technology. In MOSFET decreasing the nano-meter, SCE
will increase rapidly. To overcome this FinFET is used. SCE is very less in
FinFET, even nano-meter is decreasing. But compared to the FinFET, SOI-FinFET
having less SCE. Because the doping impurities is very less in SOI-FinFET.
Comparison of SCE of different devices is shown in below tabular form.
Table 3: Comparison of SCE of different devices.
S.NO |
Devices |
SCE |
1 |
MOSFET |
High |
2 |
MESFET |
High |
3 |
FinFET |
Less |
4 |
SOI-FinFET |
Very
Less |
Subthreshold Slope
Subthreshold slope is good swing that
device performance better parameter than other devices. The subthreshold slope
of MOSFET is 70mV per dec at room temperature. The subthreshold slope is displaying
a fast transition between ON and OFF states of the device. FinFET having good
subthreshold slope is about 0.982. but subthreshold slope of SOI-FinFET is
0.062, it is better than FinFET. MESFET Subthreshold voltage is also same
MOSFET and it is also not better than the SOI-FinFET. Comparison of the
Subthreshold slope of different devices is shown below tabular form.
Table 4: Comparison of subthreshold slope of different devices is shown below.
S.NO |
Devices |
S.S
V/dec |
1 |
MOSFET |
0.70 |
2 |
MESFET |
~0.60 |
3 |
FinFET |
0.982 |
4 |
SOI-FinFET |
0.062 |
Figure 7: Graphical representation of Subthreshold slope of different devices is shown above.
REFERENCES
- D. Singh; S. K. Mohapatra; K. P. Pradhan; P. K. Sahu, IEEE, “Variation study of process parameters in Trigate SOI- FinFET,” 2014 Annual IEEE India Conference (INDICON), Pages: 1 – 4, 2014.
- Anterpreet Gill; Charu Madhu; Pardeep Kaur, IEEE, '' Investigation of short channel effects in Bulk MOSFET and SOI FinFET at 20nm node technology,'' 2015 Annual IEEE India Conference (INDICON), pp. 1-4, 2015.
- P. Francis, A. Terao, D. Flandre and F. Van de Wiele. "Moderate Inversion Model of Ultra-Thin Double-Gate nMOS/SOI Transistors", Solid-State Electronics, vol. 38, no. 1, pp. 171-176, 1995.
- O. Moldovan, A. Cerdeira, D. Jiménez, J-P. Raskin, V. Kilchystka, D. Flandre. N. Collaert, B. Iñiguez, "Compact model for highly-doped double-gate SOI MOSFETs targeting baseband analog applications", Solid-State Electronics, vol. 51, pp 655-661, 2007.
- A. Ortiz-Conde, F. J. Garcia-Sanchez, J. Muci, S. Malobabic, and J. J. Liou, "A Review of Core Compact Models for Undoped Double-Gate SOI MOSFETs," IEEE Trans. Electron Devices, vol. 54, no. 1, pp. 131-140, 2007.
- G. Baccarani, S. Reggiani, "A Compact Double-Gate MOSFET Model Comprising Quantum-Mechanical and Nonstatic Effects", IEEE Transactions on Electron Devices, vol. 46, no. 8, pp. 1656-1666, 1999.
- Y. Taur, X. Liang, W. Wang and H. Lu, "Continuous, Analytic Drain-Current Model for DG MOSFETs", Electron Device Letters, vol. 25, no. 2, pp. 107-109, 2004.
- H. Lu and Y. Taur, "An Analytical Potential Model for Symmetric and Asymmetric DG MOSFETs", IEEE Trans. on Electron Devices, vol. 53, no. 5, pp. 1161-1168, 2006.
- B. Yu, H. Lu, M. Liu and Y. Taur, "Explicit Continuous Models for Double-Gate nd Surrounding-Gate MOSFETs", IEEE Trans. on Electron Devices, vol. 54, no. 10, pp. 2715-2722, 2007.
- M. Dunga, C.-H. Lin, A. Niknejad, and C. Hu, “Bsim-cmg: A compactmodel for multi-gate transistors,” inFinFETs and Other Multi-GateTransistors, J.-P. Colinge, Ed. Springer US, 2008, pp. 113–153.
- T. C. et al., “Benchmarking {SOI} and bulk finfet alternatives for {PLANAR}{CMOS}scaling succession,” Solid-State Electronics, vol. 54, no. 9, pp. 855–860, 2010.
- V. K. De and J. D. Meindl, “Three-region analytical models for MESFET’s in low-voltage digital circuits,” IEEE J. Solid- Srate Circuits. vol. 26, pp. 850-858, June 1991.
- J. R. Brews, W. Fichtner, E. H. Nicollian, and S. M. Sze, “Generalized guide for MOSFET miniaturization,” IEEE Electron Device Leu., vol. EDL-I, pp. 24, Jan. 1980.
- J. D. Marshall, “Performance limits of silicon enhancement/depletion MESFET integrated circuits,” Integrated Circuits Lab., Stanford Univ., Stanford, CA, Tech. Rep. (3541-6, pp. 4647, Feb. 1988.
- G. W. Taylor, H. M. Darley, R. C. Frye, and P. K. Chatterjee, “A device model for an ion-implanted MESFET,” IEEE Trans. Electron Devices.
- J. D. Marshall and J. D. Meindl, “An analytical two-dimensional moel for silicon MESFET’s,” IEEE Trans. Electron Devices, vol. 35, pp. 373-383, Mar. 1988.
- K. N. Ratnakumar and J. D. Meindl, “Short-channel MOSFET threshold voltage model,” IEEE J. Solid-State Circuirs, vol. SC-17, pp. 937-948, Oct. 1982.
- H. Daembkes, W. Brockerhoff, K. Heime, and A. Cappy, “Improved short-channel GaAs MESFET’s by use of higher doping concentration,” IEEE Trans. Electron Devices, vol. ED-31, pp. 1032-1037, Aug. 1984.
Comments
Post a Comment