A nanoscale vacuum-channel transistor (NVCT) is a transistor in which the electron transport medium is a vacuum, much like a vacuum tube. In a traditional solid-state transistor, a semiconductor channel exists between the source and the drain, and the current flows through the semiconductor. However, in a nanoscale vacuum-channel transistor,[1] no material exists between the source and the drain, and therefore, the current flows through the vacuum.

Theoretically, a vacuum-channel transistor is expected to operate faster than a traditional solid-state transistor,[2] and have higher power output and lower operation voltage.[1] Moreover, vacuum-channel transistors are expected to operate at higher temperature and radiation level than a traditional transistor[2] making them suitable for space application.

The development of vacuum-channel transistors is still at a very early research stage, and there are only limited study in recent literature such as vertical field-emitter vacuum-channel transistor,[1][3][4] gate-insulated planar electrodes vacuum-channel transistor, vertical vacuum-channel transistor,[5] and all-around gate vacuum-channel transistor.[6]

History

The concept of using conventional field-emitted electron beam in a diode was first mentioned in a 1961 article by Kenneth Shoulders.[7] However, due to the technological difficulty of fabricating a field-emitter electron source, such a diode was not implemented.

As the field of microfabrication advanced, it became possible to fabricate field-emitted electron sources, thereby paving the way for vacuum-channel transistors. The first successful implementation was reported by Gary et al. in 1986.[3] However, early vacuum-channel transistors suffered from high gate threshold voltage and couldn't compete with solid-state transistors.

More recent advances in microfabrication have allowed the vacuum-channel length between the source and the drain to be shrunk, thereby significantly reducing the gate threshold voltage below 0.5V,[1][5] which is comparable to the gate threshold voltage of current solid-state transistors.

As the shrinking of solid-state transistors is reaching its theoretical limit,[8] vacuum-channel transistors may offer an alternative.

Simplified operation

A nanoscale vacuum-channel transistor is essentially a miniaturized version of a vacuum tube. It consists of a field-emitter electron source, a collector electrode, and a gate electrode. The electron source and the collector electrodes are separated by a small distance, usually of the order of several nanometers. When a voltage is applied across the source and the collector electrode, due to field-emission, electrons are emitted from the source electrode, travel through the gap and are collected by the collector electrode. A gate electrode is used to control the current flow through the vacuum-channel.

Despite the name, vacuum-channel transistors do not need to be evacuated. The gap traversed by the electrons is so small that collisions with molecules of gas at atmospheric pressure are infrequent enough not to matter.

Advantages

The nanoscale vacuum-channel transistors have several benefits over traditional solid-state transistors such as high speed, high output power, and operation at high temperature and immunity to strong radiations. The advantages of a vacuum-channel transistor over a solid-state transistor are discussed in detail below:

High speed

In a solid-state transistor, the electrons collide with the semiconductor lattice and suffer from scattering which slows down the speed of the electrons. In fact, in silicon, the velocity of electrons is limited to 1.4×107 cm/s.[9] However, in vacuum electrons do not suffer from scattering and can reach velocities approaching the speed of light (3×1010 cm/s). Therefore, a vacuum-channel transistor can operate at a faster speed than a silicon solid-state transistor.

Operation at high temperature

The band-gap of silicon is 1.11eV, and the thermal energy of electrons should remain lower than this value for silicon to retain its semiconductor properties. This places a limit on the operating temperature of silicon transistors. However, no such limitation exists in vacuum. Therefore, a vacuum-channel transistor can operate at a much higher temperature, only limited by the melting temperature of the materials used for its fabrication. The vacuum-transistor can be used in applications where a tolerance to high temperature is required.

Immunity to radiation

The radiation can ionize the atoms in a solid-state transistor. These ionized atoms and corresponding electrons can interfere with the electron transport between the source and collector. However, no ionization occur in the vacuum-channel transistors. Therefore, a vacuum-channel transistor can be used in a high radiation environment such as outer space or inside a nuclear reactor.

Disadvantage

The performance of a vacuum-channel transistor depends upon the field emission of electrons from the source electrode. However, due to the high electric field, the source electrodes degrades over time, thereby decreasing the emission current.[10] Due to the degradation of electrons source electrode, vacuum-channel transistors suffer from poor reliability.[10]

References

  1. ^ a b c d Nguyen, H. (2019). "High-performance field emission based on nanostructured tin selenide for nanoscale vacuum transistors". Nanoscale. 11 (7): 3129–3137. doi:10.1039/C8NR07912A. PMID 30706919. S2CID 73445584.
  2. ^ a b Greene, R.; Gray, H.; Campisi, G. (1985). "Vacuum integrated circuits". 1985 International Electron Devices Meeting. Vol. 31. pp. 172–175. doi:10.1109/IEDM.1985.190922. S2CID 11778656.
  3. ^ a b Gray, H. F.; Campisi, G. J.; Greene, R. F. (1986). "A vacuum field effect transistor using silicon field emitter arrays". 1986 International Electron Devices Meeting. Vol. 32. pp. 776–779. doi:10.1109/IEDM.1986.191310. S2CID 26572635.
  4. ^ Campisi, G. J.; Gray, H. F. (1986-01-01). "Microfabrication of Field Emission Devices for Vacuum Integrated Circuits using Orientation Dependent Etching". MRS Online Proceedings Library Archive. 76. doi:10.1557/PROC-76-67. ISSN 1946-4274.
  5. ^ a b Srisonphan, Siwapon; Jung, Yun Suk; Kim, Hong Koo (2012). "Metal–oxide–semiconductor field-effect transistor with a vacuum channel". Nature Nanotechnology. 7 (8): 504–508. Bibcode:2012NatNa...7..504S. doi:10.1038/nnano.2012.107. PMID 22751220.
  6. ^ Han, Jin-Woo; Moon, Dong-Il; Meyyappan, M. (2017-04-12). "Nanoscale Vacuum Channel Transistor". Nano Letters. 17 (4): 2146–2151. Bibcode:2017NanoL..17.2146H. doi:10.1021/acs.nanolett.6b04363. ISSN 1530-6984. PMID 28334531. S2CID 439350.
  7. ^ Shoulders, Kenneth R. (1961). Microelectronics Using Electron-Beam-Activated Machining Techniques* - ScienceDirect. Vol. 2. pp. 135–293. doi:10.1016/S0065-2458(08)60142-4. ISBN 9780120121021. ((cite book)): |journal= ignored (help)
  8. ^ Waldrop, M. Mitchell (2016-02-11). "The chips are down for Moore's law". Nature. 530 (7589): 144–147. Bibcode:2016Natur.530..144W. doi:10.1038/530144a. PMID 26863965.
  9. ^ Sze, S. M. (1981). Physics of semiconductor devices. USA: John wiley & sons. pp. 46. ISBN 978-0-471-05661-4.
  10. ^ a b Han, Jin-Woo (2012-05-21). "Vacuum nanoelectronics: Back to the future?—Gate insulated nanoscale vacuum channel transistor". Applied Physics Letters. 100 (21): 213505. Bibcode:2012ApPhL.100u3505H. doi:10.1063/1.4717751. ISSN 0003-6951.

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