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2 - Multigate and Nanowire Transistors

Published online by Cambridge University Press:  05 April 2016

Jean-Pierre Colinge
Affiliation:
Taiwan Semiconductor Manufacturing Company Limited (TSMC)
James C. Greer
Affiliation:
Tyndall National Institute, Ireland
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Summary

As presented in Chapter 1, the use of a multigate architecture is a technology booster that allows improved electrostatic control of a channel region by the gate electrode, and therefore mitigates short-channel effects. Currently existing multigate architectures for the MOSFET are described, and then compared in terms of short-channel effect control. It is concluded that the gate-all-around structure associated with a nanowire-shaped semiconductor offers the best possible electrostatic control of a channel. Different effects arising from carrier confinement effects in semiconductor nanowires are considered. The chapter concludes with a discussion of novel phenomena arising from quantum confinement, such as the semimetal–semiconductor transition, band folding of the electronic structure in nanowires, and novel devices that can be devised on the nanometer length scale.

Introduction

In the classical planar MOSFET, the gate dielectric and gate electrode sit above the channel region. Electrostatic control of the channel by the gate is achieved through the capacitive coupling between the gate and the channel. To maintain transistor scaling laws, a reduction in the depths of the source and drain regions by the same factor as the gate length reduction is required. This reduces short-channel effects at the cost of rendering less effective the control of the channel region through source and drain voltages. High-κdielectrics are used as gate oxide materials to increase current drive without having to pay a stiff penalty in gate oxide leakage, which is in turn largely responsible for standby power consumption. Decreasing the equivalent gate oxide thickness (EOT) through the replacement of the silicon dioxide insulating layer by metallic oxides with higher dielectric constant improves the capacitive coupling between the gate and the channel, and thus also reduces short-channel effects.

The electrostatics of a planar, long-channel MOSFET can be reduced in a first approximation to a one-dimensional problem. Early textbooks on semiconductor device physics introduced the “gradual channel approximation,” which can be solved by Poisson's equation – the equation that governs the relationship between electric fields and electrical charges – in one dimension, vertically from the gate through the channel and down through the silicon substrate. Short-channel effects whereby electric fields from the source and the drain encroach laterally (horizontally) in the channel region introduce a second dimension to the problem. In planar MOSFETs on bulk silicon, short-channel effects become insurmountable once the gate length becomes smaller than approximately 15 to 20 nm.

Type
Chapter
Information
Nanowire Transistors
Physics of Devices and Materials in One Dimension
, pp. 18 - 53
Publisher: Cambridge University Press
Print publication year: 2016

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References

Sze, S.M., Modern Semiconductor Device Physics, Wiley-Interscience (1997)
Lundstrom, M., Guo, J., Nanoscale Transistors: Device Physics, Modeling and Simulation, Springer (2006)
Colinge, J.-P. (ed.), FinFETs and other Multigate Transistors, Springer (2008)
[1] Planes, N.et al., “28nm FDSOI technology platform for high-speed low-voltage digital applications,” Symposium on VLSI Technology Digest of Technical Papers, pp. 133–134 (2012)
[2] Auth, C.et al., “A 22nm high performance and low-power CMOS technology featuring fully-depleted tri-gate transistors, self-aligned contacts and high density MIM capacitors,” Symposium on VLSI Technology Digest of Technical Papers, pp. 131–132 (2012)
[3] Colinge, J.P., “Multiple-gate SOI MOSFETs,” Solid-State Electronics, vol. 48, no. 6, pp. 897–905 (2004)Google Scholar
[4] Skotnicki, T.et al., “Innovative materials, devices, and CMOS technologies for low-power mobile multimedia,” IEEE Transactions on Electron Devices, vol. 55, no. 1, pp. 96–130 (2008)Google Scholar
[5] Sekigawa, T., Hayashi, Y., “Calculated threshold-voltage characteristics of an XMOS transistor having an additional bottom gate,” Solid-State Electronics, vol. 27, no. 8–9, pp. 827–828 (1984)Google Scholar
[6] Hisamoto, D.et al., “A fully depleted lean-channel transistor (DELTA) – a novel vertical ultra thin SOI MOSFET,” Technical Digest of the International Electron Device Meeting (IEDM), pp. 833–836 (1989)
[7] Huang, X.et al., “Sub 50-nm FinFET: PMOS,” Technical Digest of the International Electron Device Meeting (IEDM), pp. 67–70 (1999)
[8] Choi, S.et al., “Fabrication of body-tied FinFETs (Omega MOSFETs) using bulk Si wafers,” Symposium on VLSI Technology Digest of Technical Papers, pp. 135–136 (2003)
[9] Baie, X.et al., “Quantum-wire effects in thin and narrow SOI MOSFETs,” Proceedings IEEE International SOI Conference, pp. 66–67 (1995)
[10] Doyle, B.S.et al., “High performance fully-depleted tri-gate CMOS transistors,” IEEE Electron Device Letters, vol. 24, no. 4, pp. 263–265 (2003)Google Scholar
[11] Park, J.T., Colinge, J.P., Diaz, C.H, “Pi-gate SOI MOSFET,” IEEE Electron Device Letters, vol. 22, no. 8, pp. 405–406 (2001)Google Scholar
[12] Yang, F.-L.et al., “25 nm CMOS omega FETs,” Technical Digest of the International Electron Device Meeting (IEDM), pp. 255–258 (2002)
[13] Colinge, J.P.et al., “Silicon-on-insulator gate-all-around device,” Technical Digest of the International Electron Device Meeting (IEDM), pp. 595–598 (1990)
[14] Colinge, J.P.et al., “Nanowire transistors without junctions,” Nature Nanotechnology, vol. 5, pp. 225–229 (2010)Google Scholar
[15] Ansari, L.et al., “Simulation of junctionless Si nanowire transistors with 3 nm gate length,” Applied Physics Letters, vol. 97, p. 062105 (2010)Google Scholar
[16] Ansari, L.et al., “First principle-based analysis of single-walled carbon nanotube and silicon nanowire junctionless transistors,” IEEE Transactions on Nanotechnology, vol. 12, no. 6, pp. 1075–1081 (2013)Google Scholar
[17] Hofmann, F.et al., “NVM based on FinFET device structures,” Solid-State Electronics, vol. 49, no. 11, pp. 1799–1804 (2005)Google Scholar
[18] Tang, X.et al., “Self-aligned SOI nano flash memory device,” Solid State Electronics, vol. 44, pp. 2259–2264 (2000)Google Scholar
[19] Suk, S.D.et al., “Characteristics of sub 5nm tri-gate nanowire MOSFETs with single and poly Si channels in SOI structure,” Symposium on VLSI Technology Digest of Technical Papers, pp. 142–143 (2009)
[20] Park, J.T., Colinge, C.A., Colinge, J.P., “Comparison of gate structures for short-channel SOI MOSFETs,” Proceedings of the IEEE International SOI Conference, pp. 115–116 (2001)
[21] Park, J.T., Colinge, J.P., “Multiple-gate SOI MOSFETs: device design guidelines,” IEEE Transactions on Electron Devices, vol. 49, no. 12, pp. 2222–2229 (2002)Google Scholar
[22] Colinge, J.P., “Multiple-gate SOI MOSFETs,” Solid-State Electronics, vol. 48, no. 6, pp. 897–905 (2004)Google Scholar
[23] Ferain, I., Colinge, C.A., Colinge, J.P., “Multigate transistors as the future of classical metal-oxide-semiconductor field-effect transistors,” Nature, vol. 479, pp. 310–316 (2011)Google Scholar
[24] Kuhn, K.J., “Considerations for Ultimate CMOS Scaling,” IEEE Transactions on Electron Devices, vol. 59, no. 7, pp. 1813–1828 (2012)Google Scholar
[25] Goldberger, J.et al., “Silicon vertically integrated nanowire field effect transistors,” Nano Letters, vol. 6, no. 5, pp. 973–977 (2006)Google Scholar
[26] Yan, R.H., Ourmazd, A., Lee, K.F., “Scaling the Si MOSFET: from bulk to SOI to bulk,” IEEE Transactions on Electron Devices, vol. 39, no. 7, pp. 1704–1710 (1992)Google Scholar
[27] Suzuki, K.et al., “Scaling theory for double-gate SOI MOSFETs,” IEEE Transactions on Electron Devices, vol. 40, no. 12, pp. 2326–2329 (1993)Google Scholar
[28] Colinge, J.P., “Multiple-gate SOI MOSFETs,” Solid-State Electronics, vol. 48, no. 6, pp. 897–905 (2004)Google Scholar
[29] Lee, C.-W.et al., “Device design guidelines for nano-scale MuGFETs,” Solid-State Electronics, vol. 51, pp. 505–510 (2007)Google Scholar
[30] Auth, C.P., Plummer, J.D., “Scaling theory for cylindrical, fully depleted, surrounding-gate MOSFET's,” IEEE Electron Device Letters, vol. 18, no. 2, pp. 74–76 (1997)Google Scholar
[31] Chiang, T.-K., “A novel scaling theory for fully depleted, multiple-gate MOSFET, including effective number of gates (ENGs),” IEEE Transactions on Electron Devices, vol. 61, no. 2, pp. 631–632 (2014)Google Scholar
[32] Yu, Bo, Wang, L.et al., “Scaling of nanowire transistors,” IEEE Transactions on Electron Devices, vol. 55, no. 11, pp. 2836–2858 (2008)Google Scholar
[33] Shankar, R.et al., “A degradation model of double gate and gate-all-around MOSFETs with interface trapped charges including effects of channel mobile charge carriers,” IEEE Transactions on Device and Materials Reliability, vol. 14, no. 2, pp. 689–697 (2014)Google Scholar
[34] Liu, C.et al., “Negative-bias temperature instability in gate-all-around silicon nanowire MOSFETs: characteristic modeling and the impact on circuit aging,” IEEE Transactions on Electron Devices, vol. 57, no. 12, pp. 3442–3450 (2010)Google Scholar
[35] Kuhn, K.J., “Considerations for ultimate CMOS scaling,” IEEE Transactions on Electron Devices, vol. 59, no. 7, pp. 1813–1828 (2012)Google Scholar
[36] Nayak, K.et al., “Metal-gate granularity-induced threshold voltage variability and mismatch in Si gate-all-around nanowire n-MOSFETs,” IEEE Transactions on Electron Devices, vol. 61, no. 12 (2014) DOI: 10.1109/TED.2014.2351401Google Scholar
[37] Colinge, C.A., Colinge, J.P., Physics of Semiconductor Devices, Kluwer Academic Publishers (now: Springer), pp. 336–348 (2002)
[38] Moreno, E., Roldán, J.B., Ruiz, F.G., Barrera, D., Godoy, A., Gámiz, F., “An analytical model for square GAA MOSFETs including quantum effects,” Solid-State Electronics, vol. 54, pp. 1463–1469 (2010)Google Scholar
[39] Colinge, J.P., “Quantum-wire effects in trigate SOI MOSFETs,” Solid-State Electronics, vol. 51, pp. 1153–1160 (2007)Google Scholar
[40] Balestra, F.et al., “Double-gate silicon-on-insulator transistor with volume inversion: a new device with greatly enhanced performance,” IEEE Electron Device Letters, vol. 8, pp. 410–412 (1987)Google Scholar
[41] Colinge, J.P., “Quantum-wire effects in trigate SOI MOSFETs,” Solid-State Electronics, vol. 51 –9, pp. 1153–1160 (2007)Google Scholar
[42] Jimenéz, D.et al., “Unified compact model for the ballistic quantum wire and quantum well metal-oxide-semiconductor field-effect-transistor,” Journal of Applied Physics, vol. 94, pp. 1061–1068 (2003)Google Scholar
[43] Rustagi, S.C.et al., “Low-temperature transport characteristics and quantum-confinement effects in gate-all-around Si-nanowire N-MOSFET,” IEEE Electron Device Letters, vol. 28, no. 10, pp. 909–912 (2007)Google Scholar
[44] Colinge, J.P.et al., “A silicon-on-insulator quantum wire,” Solid-State Electronics, vol. 39, pp. 49–51 (1996)Google Scholar
[45] Colinge, J.P., “The new generation of SOI MOSFETs,” Romanian Journal of Information Science and Technology, vol. 11, no. 1, pp. 3–15 (2008)Google Scholar
[46] Colinge, J.P.et al., “Low-temperature electron mobility in trigate SOI MOSFETs,” IEEE Electron Device Letters, vol. 27, no. 2, pp. 120–122, 2006Google Scholar
[47] Singh, N.et al., “Ultra-narrow silicon nanowire gate-all-around CMOS Devices: Impact of diameter, channel-orientation and low temperature on device performance,” Extended Abatracts of the IEEE International Electron Device Meeting (IEDM), pp. 547–550 (2006)
[48] Yoshioka, H.et al., “Mobility oscillation by one-dimensional quantum confinement in Si-nanowire metal-oxide-semiconductor field effect transistors,” Journal of Applied Physics, vol. 106, p. 034312 (2009)Google Scholar
[49] Yi, K.S.et al., “Room-temperature quantum confinement effects in transport properties of ultrathin Si nanowire field-effect transistors,” Nano Letters, vol. 11, no. 12, pp. 5465–5470 (2011)Google Scholar
[50] Park, J.-T., Kim, J.Y., Lee, C.-W., Colinge, J.P., “Low-temperature conductance oscillations in junctionless nanowire transistors,” Applied Physics Letters, vol. 97, p. 172101 (2010)Google Scholar
[51] Coquand, R.et al., “Low-temperature transport characteristics in SOI and sSOI nanowires down to 8nm width: evidence of IDS and mobility oscillations,” Proceedings of European Solid-State Device Research Conference (ESSDERC), pp. 198–201 (2013)
[52] Li, X.et al., “Low-temperature electron mobility in heavily n-doped junctionless nanowire transistor,” Applied Physics Letters, vol. 102, p. 223507 (2013)Google Scholar
[53] Colinge, J.P.et al., “Low-temperature electron mobility in trigate SOI MOSFETs,” IEEE Electron Device Letters, vol. 27, no. 2, pp. 120–122, 2006Google Scholar
[54] Singh, N.et al., “Ultra-narrow silicon nanowire gate-all-around CMOS devices: impact of diameter, channel-orientation and low temperature on device performance,” Extended Abstracts of the IEEE Electron Devices Meeting (IEDM), pp. 547–550 (2006)
[55] Je, M., Han, S., Kim, I., Shin, H., “A silicon quantum wire transistor with one-dimensional subband effects,” Solid-State Electronics, vol. 44, pp. 2207–2212 (2000)Google Scholar
[56] Nolan, M.et al., “Silicon nanowire band gap modification,” Nano Letters, vol. 7, no. 1, pp. 34–38 (2007)Google Scholar
[57] Bescond, M.et al., “Tight-binding calculations of Ge-nanowire bandstructures,” Journal of Computational Electronics, vol. 6, pp. 341–344 (2007)Google Scholar
[58] Jena, D., “Tunneling transistors based on graphene and 2-D crystals,” Proceedings of the IEEE, vol. 101, no. 7, pp. 1585–1602 (2013)Google Scholar
[59] Bescond, M.et al., “Tight-binding calculations of Ge-nanowire bandstructures,” Journal of Computational Electronics, vol. 6, pp. 341–344 (2007)Google Scholar
[60] Khayer, M.A., Lake, R.K., “Performance of n-type InSb and InAs nanowire field effect transistors,” IEEE Transactions on Electron Devices, vol. 55, no. 11, pp. 2939–2345 (2008)Google Scholar
[61] Ansari, L.et al., “A proposed confinement modulated gap nanowire transistor based on a metal (tin),” Nano Letters, vol. 15, no. 5, pp. 2222–2227 (2012)Google Scholar
[62] Dresselhaus, M.S., Rabin, O., “Carbon nanotubes and bismuth nanowires,” in Nanoengineering of Structural, Functional and Smart Materials, Schulz, M.J., Kelkar, A.D. and Sundaresan, M.J. (eds.), CRC Press (2005)
[63] Lee, S.et al., “Direct observation of the semimetal-to-semiconductor transition of individual single-crystal bismuth nanowires grown by on-film formation of nanowires,” Nanotechnology, vol. 21, pp. 405701/1–6 (2010)Google Scholar
[64] Luryi, S., “Quantum capacitance devices,” Applied Physics Letters, vol. 52, no. 16, pp. 501–503 (1987)Google Scholar
[65] Afzalian, A.et al., “Quantum confinement effects in capacitance behavior of multigate silicon nanowire MOSFETs,” IEEE Transactions on Nanotechnology, vol. 10, no. 2, pp. 300–309 (2011)Google Scholar
[66] Marin, E.G.et al., “Analytical gate capacitance modeling of III–V nanowire transistors,” IEEE Transactions on Electron Devices, vol. 60, no. 5, pp. 1590–1599 (2013)Google Scholar
[67] Khayer, A., Lake, R.K., “The quantum capacitance limit of high-speed, low-power InSb nanowire field-effect transistors,” Technical Digest of the International Electron Device Meeting (IEDM), pp. 193–196 (2008)
[68] Takiguchi, N.et al., “Comparisons of performance potentials of Si and InAs nanowire MOSFETs under ballistic transport,” IEEE Transactions on Electron Devices, vol. 59, no. 1, pp. 206–211 (2012)Google Scholar
[69] Lind, E.et al., “Band structure effects on the scaling properties of [111] InAs nanowire MOSFETs,” IEEE Transactions on Electron Devices, vol. 56, no. 2, pp. 201–205 (2009)Google Scholar
[70] Knoch, J., Riess, W., Appenzeller, J., “Outperforming the conventional scaling rules in the quantum capacitance limit,” IEEE Electron Device Letters, vol. 29, no. 4, pp. 372–374 (2008)Google Scholar
[71] Skotnicki, T., Boeuf, F., “How can high-mobility channel materials boost or degrade performance in advanced CMOS,” Proceedings VLSI Symposium, pp. 153–154 (2010)
[72] Fischetti, M.V.et al., “Theoretical study of some physical aspects of electronic transport in nMOSFETs at the 10-nm gate-length,” IEEE Transactions on Electron Devices, vol. 54, no. 9, pp. 2116–2163 (2007)Google Scholar
[73] Kim, R., Avci, U.E., Young, I.A., “Comprehensive performance benchmarking of III-V and Si nMOSFETs (gate length = 13 nm) considering supply voltage and OFF-current,” IEEE Transactions on Electron Devices (2015), DOI: 10.1109/TED.2015.2388708
[74] Razavi, P.et al., “Influence of channel material properties on performance of nanowire transistors,” Journal of Applied Physics, vol. 111, no. 12, pp. 124509-1–124509-8 (2012)Google Scholar
[75] Neophytou, N.et al., “Dependence of injection velocity and capacitance of Si nanowires on diameter, orientation, and gate bias: an atomistic tight-binding study,” International Conference on Simulation of Semiconductor Processes and Devices (SISPAD), pp. 71–74 (2009)
[76] Neophytou, N.et al., “On the bandstructure velocity and ballistic current of ultra-narrow silicon nanowire transistors as a function of cross section size, orientation, and bias,” Journal of Applied Physics, vol. 107, pp. 113701.1–9 (2010)Google Scholar
[77] Neophytou, N., Kosina, H., “Confinement-induced carrier mobility increase in nanowires by quantization of warped bands,” Solid-State Electronics, vol. 70, pp. 81–91 (2012)Google Scholar
[78] Nolan, M.et al., “Silicon nanowire band gap modification,” Nano Letters, vol. 7, no. 1, pp. 34–38 (2007)Google Scholar
[79] Bescond, M.et al., “Tight-binding calculations of Ge-nanowire bandstructures,” Journal of Computational Electronics, vol. 6, pp. 341–344 (2007)Google Scholar
[80] Boukai, A., Xu, Ke, Heath, J.R., “Size-dependent transport and thermoelectric properties of individual polycrystalline bismuth nanowires,” Advanced Materials, vol. 18, pp. 864–869 (2006)Google Scholar
[81] Tian, Y.T.et al., “Step-shaped bismuth nanowires with metal–semiconductor junction characteristics,” Nanotechnology, vol. 17, pp. 1041–1045 (2006)Google Scholar
[82] Cronin, S.B., “Electronic properties of Bi nanowires,” Ph.D. thesis, Massachusetts Institute of Technology Department of Physics (June 2002), available at: http://dspace.mit.edu/bitstream/handle/1721.1/16820/50762540.pdf?sequence=1
[83] Shim, W.et al., “On-film formation of Bi nanowires with extraordinary electron mobility,” Nano Letters, vol. 9, no. 1, pp. 18–22 (2009)Google Scholar
[84] Ansari, L.et al., “A proposed confinement modulated gap nanowire transistor based on a metal (tin),” Nano Letters, vol. 12, no. 5, pp. 2222–2227 (2012)Google Scholar
[85] Kane, C.L., Mele, E.J., “Z2 topological order and the quantum spin Hall effect,” Physical Review Letters, vol. 95, no. 14, pp. 146802:1–4 (2005)Google Scholar
[86] Zhu, H.et al., “Topological insulator Bi2Se3 nanowire high performance field-effect transistors,” Nature Scientific Reports, vol. 3, pp. 1757:1–5, DOI: 10.1038/srep01757 (2013)Google Scholar
[87] Colinge, C.A., Colinge, J.P., Physics of Semiconductor Devices, Kluwer Academic Publishers (now: Springer), pp. 358–360 (2002)
[88] Akhavan, N. Dehdashtiet al., “Nanowire to single-electron transistor transition in trigate SOI MOSFETs,” IEEE Transactions on Electron Devices, vol. 58, no. 1, pp. 26–32 (2011)Google Scholar
[89] Deshpande, V.et al., “Scaling of trigate nanowire (NW) MOSFETs to sub-7 nm width: 300 K transition to single electron transistor,” Solid-State Electronics, vol. 84, pp. 179–184 (2013)Google Scholar
[90] Kononchuk, O., Nguyen, B.-Y. (eds.), Silicon-On-Insulator (SOI) Technology: Manufacture and Applications, Elsevier (2014)
[91] Barraud, S., Berthomé, M., Coquand, R., et al., “Scaling of trigate junctionless nanowire MOSFET with gate length down to 13 nm,” IEEE Electron Device Letters, vol. 33, no. 9, pp. 1225–1227 (2012)Google Scholar
[92] Lilienfeld, J.E., “Method and apparatus for controlling electric current,” US patent 1745175 first filed in Canada on 22 October 1925
[93] Migita, S., Morita, Y., Masahara, M., Ota, H., “Electrical performances of junctionless-FETs at the scaling limit (LCH = 3 nm),” Technical Digest of the IEEE International Electron Device Meeting (IEDM), pp. 191–194 (2012)
[94] Ionescu, A., Riel, H., “Tunnel field-effect transistors as energy-efficient electronic switches,” Nature, vol. 479, pp. 329–337 (2011)Google Scholar
[95] Gnani, E.et al., “Steep-slope nanowire FET with a superlattice in the source extension,” Proceedings of the European Solid-State Device Research Conference (ESSDERC), pp. 380–383 (2010)
[96] Afzalian, A., Colinge, J.P., Flandre, D., “Physics of gate modulated resonant tunneling (RT)-FETs: multi-barrier MOSFET for steep slope and high on-current,” Solid-State Electronics, vol. 59, No 1, pp. 50–61 (2011)Google Scholar
[97] Lu, H., Seabaugh, A., “Tunnel field-effect transistors: state-of-the-art,” IEEE Journal of the Electron Devices Society, vol. 2, no. 4, pp. 44–49 (2014)Google Scholar
[98] Vandooren, A.et al., “Impact of process and geometrical parameters on the electrical characteristics of vertical nanowire silicon n-TFETs,” Solid-State Electronics, vol. 72, pp. 82–87 (2012)Google Scholar
[99] Gandhi, R.et al., “Vertical Si-nanowire n-type tunneling FETs with low subthreshold swing (≤ 50 mV/decade) at room temperature,” IEEE Electron Device Letters, vol. 32, no. 4, pp. 437–439 (2011)Google Scholar
[100] Gandhi, R.et al., “CMOS-compatible vertical-silicon-nanowire gate-all-around p-type tunneling FETs with ≤ 50-mV/decade subthreshold swing,” IEEE Electron Device Letters, vol. 32, no. 11, pp. 1504–1506 (2011)Google Scholar
[101] Villalon, A.et al., “First demonstration of strained SiGe nanowires TFETs with ION beyond 700μA/μm,” Symposium on VLSI Technology Digest of Technical Papers, pp. 84–85 (2014)
[102] Dey, A.W.et al., “Combining axial and radial nanowire heterostructures: radial Esaki diodes and tunnel field-effect transistors,” Nano Letters, vol. 13, no. 12, pp. 5919−5924 (2013)Google Scholar
[103] Wan, J.et al., “Novel bipolar-enhanced tunneling FET with simulated high on-current,” IEEE Electron Device Letters, vol. 34, no. 1, pp. 24−26 (2013)Google Scholar

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