Long channel carbon nanotube transistor (CNT) can be used to overcome the high electric field effects in nanoscale length silicon channel. When maximum electric field is reduced, the gate of a field-effect transistor (FET) is able to gain control of the channel at varying drain bias. The device performance of a zigzag CNTFET with the same unit area as a nanoscale silicon metal-oxide semiconductor field-effect transistor (MOSFET) channel is assessed qualitatively. The drain characteristic of CNTFET and MOSFET device models as well as fabricated CNTFET device are explored over a wide range of drain and gate biases. The results obtained show that long channel nanotubes can significantly reduce the drain-induced barrier lowering (DIBL) effects in silicon MOSFET while sustaining the same unit area at higher current density. 1. Introduction Carbon nanotubes (CNTs) are gaining momentum in the current silicon technology as a complementary nanostructure that could reform the device architecture. CNT modeling has been rigorously studied and examined [1–5] to assess the performance of the device at the circuit level. Advancement of the nanotechnology devices modeling is vital for the foreseeable future of carbon nanotube as switching device, interconnect and memory in integrated circuits (ICs). An in situ growth single-walled carbon nanotube (SWCNT), which integrates long channel 600?nm CNT channel, thin Al2O3 top gate contact, and Palladium (Pd) metal source/drain contacts, has been demonstrated [6]. In addition, we report the potential of long channel 65?nm CNT as substitute to 45?nm silicon metal-oxide semiconductor field-effect transistor (Si MOSFET) from the perspective of modeling for future CNT-logic applications. We observe good agreement between CNTFET and Si MOSFET, respectively, when simulating two-terminal drain current–voltage ( ) characteristic. The projection has shed light on the reduction of DIBL and high field effects [7] as well as reduction in long channel CNT which is a widespread phenomenon in nanoscale Si MOSFET [8, 9]. We also demonstrate the effects of the channel area restructuring on the maximum electric field as well as density of states (DOS) in the conductance of CNT. Unlike MOSFET, it is revealed that the performance of CNT is enhanced when the source and drain width is minimized rather than the length, primarily due to the gate-to-source-drain parasitic fringe capacitances [10]. MOSFET scaling in accordance with Moore’s Law will reach its fundamental limitation as a result of process controllability in the next 10 years.
References
[1]
J. Deng and H.-S. P. Wong, “A compact SPICE model for carbon-nanotube field-effect transistors including nonidealities and its application. Part I: model of the intrinsic channel region,” IEEE Transactions on Electron Devices, vol. 54, no. 12, pp. 3186–3194, 2007.
[2]
J. Deng and H.-S. P. Wong, “A compact SPICE model for carbon-nanotube field-effect transistors including nonidealities and its application. Part II: full device model and circuit performance benchmarking,” IEEE Transactions on Electron Devices, vol. 54, no. 12, pp. 3195–3205, 2007.
[3]
J. Guo, S. Datta, M. Lundstrom et al., “Assessment of silicon MOS and carbon nanotube FET performance limits using a general theory of ballistic transistors,” in Proceedings of the IEEE International Devices Meeting (IEDM), pp. 711–714, December 2002.
[4]
J. M. Marulanda, A. Srivastava, and A. K. Sharma, “Transfer characteristics and high frequency modeling of logic gates using carbon nanotube field effect transistors (CNT-FETs),” in Proceedings of the 20th Symposium on Integrated Circuits and System Design, pp. 202–206, Rio de Janeiro, Brazil, September 2007.
[5]
K. Natori, Y. Kimura, and T. Shimizu, “Characteristics of a carbon nanotube field-effect transistor analyzed as a ballistic nanowire field-effect transistor,” Journal of Applied Physics, vol. 97, no. 3, Article ID 034306, 2005.
[6]
G. A. J. Amaratunga, A. S. Teh, S. N. Cha et al., “Nanotube and nanowire transistors,” in Proceedings of the Interational Semiconductor Conference (CAS '05), vol. 1, pp. 3–8, October 2005.
[7]
V. K. Arora and M. L. P. Tan, “High-field transport in graphene and carbon nanotubes,” in Proceedings of the IEEE International Conference of Electron Devices and Solid-State Circuits (EDSSC '13), pp. 1–2, 2013.
[8]
M. T. Ahmadi, R. Ismail, M. L. P. Tan, and V. K. Arora, “The ultimate ballistic drift velocity in carbon nanotubes,” Journal of Nanomaterials, vol. 2008, Article ID 769250, 8 pages, 2008.
[9]
R. Vidhi, M. L. P. Tan, T. Saxena, A. M. Hashim, and V. K. Arora, “The drift response to a high-electric-field in carbon nanotubes,” Current Nanoscience, vol. 6, no. 5, pp. 492–495, 2010.
[10]
B. C. Paul, S. Fujita, M. Okajima, and T. Lee, “Modeling and analysis of circuit performance of ballistic CNFET,” in Proceedings of the 43rd Design Automation Conference, pp. 717–722, 2006.
[11]
V. K. Arora, M. L. P. Tan, I. Saad, and R. Ismail, “Ballistic quantum transport in a nanoscale metal-oxide-semiconductor field effect transistor,” Applied Physics Letters, vol. 91, no. 10, Article ID 103510, 2007.
[12]
M. L. P. Tan, R. Ismail, R. Muniandy, and V. K. Wong, “Velocity saturation dependence on temperature, substrate doping concentration and longitudinal electric field in nanoscale MOSFET,” in Proceedings of the IEEE National Symposium on Microelectronics, 2005.
[13]
A. Rahman, J. Guo, S. Datta, and M. S. Lundstrom, “Theory of ballistic nanotransistors,” IEEE Transactions on Electron Devices, vol. 50, no. 9, pp. 1853–1864, 2003.
[14]
S. Datta, Electronic Transport in Mesoscopic Systems, Cambridge University Press, Cmabridge, UK, 1994.
[15]
J. W. Mintmire and C. T. White, “Universal density of states for carbon nanotubes,” Physical Review Letters, vol. 81, no. 12, pp. 2506–2509, 1998.
[16]
J. Appenzeller, J. Knoch, M. Radosavljevi?, and P. Avouris, “Multimode transport in schottky-barrier carbon-nanotube field-effect transistors,” Physical Review Letters, vol. 92, no. 22, Article ID 226802, 2004.
[17]
Z. Dawei, Z. Hao, Y. Zhiping, and T. Lilin, “A unified charge model comprising both 2D quantum mechanical effects in channels and in poly-silicon gates of MOSFETs,” Solid-State Electronics, vol. 49, no. 10, pp. 1581–1588, 2005.
[18]
A. Javey, J. Guo, M. Paulsson et al., “High-field quasiballistic transport in short carbon nanotubes,” Physical Review Letters, vol. 92, no. 10, Article ID 106804, 2004.
[19]
M. L. P. Tan and G. A. J. Amaratunga, “Performance prediction of graphene nanoribbon and carbon nanotube transistors,” in Proceedings of the AIP Conference Proceedings,, vol. 1341, pp. 365–369, 2011.
[20]
M. L. P. Tan, G. Lentaris, and G. A. Amaratunga, “Device and circuit-level performance of carbon nanotube field-effect transistor with benchmarking against a nano-MOSFET,” Nanoscale Research Letters, vol. 7, article 467, 2012.
[21]
Y. Imry and R. Landauer, “Conductance viewed as transmission,” Reviews of Modern Physics, vol. 71, no. 2, pp. S306–S312, 1999.
[22]
D. C. Y. Chek, M. L. P. Tan, M. T. Ahmadi, R. Ismail, and V. K. Arora, “Analytical modeling of high performance single-walled carbon nanotube field-effect-transistor,” Microelectronics Journal, vol. 41, no. 9, pp. 579–584, 2010.
[23]
M. L. P. Tan, V. K. Arora, I. Saad, M. Taghi Ahmadi, and R. Ismail, “The drain velocity overshoot in an 80 nm metal-oxide-semiconductor field-effect transistor,” Journal of Applied Physics, vol. 105, no. 7, Article ID 074503, 2009.
[24]
Z. Arefinia and A. A. Orouji, “Novel attributes in the performance and scaling effects of carbon nanotube field-effect transistors with halo doping,” Superlattices and Microstructures, vol. 45, no. 6, pp. 535–546, 2009.
[25]
J. Chen, C. Klinke, A. Afzali, and P. Avouris, “Self-aligned carbon nanotube transistors with charge transfer doping,” Applied Physics Letters, vol. 86, no. 12, Article ID 123108, pp. 1–3, 2005.
[26]
K. Alam and R. Lake, “Role of doping in carbon nanotube transistors with source/drain underlaps,” IEEE Transactions on Nanotechnology, vol. 6, no. 6, pp. 652–659, 2007.
[27]
N. Bahador, M. L. P. Tan, M. T. Ahmadi, and R. Ismail, “A unified drain-current model of silicon nanowire field-effect transistor (SiNWFET) for performance metric evaluation,” Science of Advanced Material, vol. 6, pp. 354–360, 2014.