1997
DOI: 10.1063/1.118853
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Direct current and high frequency performance of thin film InP-based tunneling hot electron transfer amplifiers

Abstract: We report the dc and high frequency performance of thin-film InP-based tunneling hot electron transfer amplifiers bonded to a variety of host substrates. The high-frequency device performance is slightly degraded since the InP substrate removal and bonding process for these devices have not yet been optimized. This demonstration represents an important step toward the development of high-frequency, thin-film InP-based electronic devices integrated with conventional Si-based circuit elements.

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Cited by 4 publications
(5 citation statements)
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“…The effective gain may be overestimated when a collector bias is applied because of the quantum capacitance of graphene . The values of the effective gain α* for the five devices range from ∼0.3 to 2.1%, which are still relatively low compared to state-of-the-art HETs. , …”
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confidence: 89%
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“…The effective gain may be overestimated when a collector bias is applied because of the quantum capacitance of graphene . The values of the effective gain α* for the five devices range from ∼0.3 to 2.1%, which are still relatively low compared to state-of-the-art HETs. , …”
mentioning
confidence: 89%
“…24 The values of the effective gain α* for the five devices range from ∼0.3 to 2.1%, which are still relatively low compared to state-of-the-art HETs. 12,13 There are two other important factors that affect the gain α (and α*) in addition to the collector/emitter area ratio. One is the energy of hot electrons.…”
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confidence: 99%
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“…The OFF current measured is around two orders of magnitude lower than the reported in recent literature [20] and, accordingly, our HET devices exhibit a large ON/OFF ratio of ~10 5 . The equivalent subthreshold swing (defined as the required V E for a ten-fold change in I C ) is ~96 mV/dec at ~80 K and below, a very suitable value for applications in high-speed and frequency integrated-circuits [24,25]. Figure 2 (b) shows in detail (in 5 K steps) the evolution of the hot electron current for temperatures below 190 K, while Figure 2 (c) displays an exponential decrease with decreasing temperature for the thermal leakage down to 160 ± 20 K. However, at temperatures below 160 K, the hotelectron current increases linearly for V E voltages larger than the metal/semiconductor barrier height.…”
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confidence: 99%
“…The ongoing need for improved speed and density in high-performance multifunctional electronics has motivated extensive research into the transfer and bonding of electronic and optoelectronic devices to host substrates, including silicon [1][2][3][4][5]. Hybrid thin-film integration of III-V devices onto CMOS circuitry is a promising technique which has been successfully applied to optoelectronic circuits, allowing each component to be independently optimized with proven technologies at relatively low cost [6][7][8].…”
Section: Introductionmentioning
confidence: 99%