2017
DOI: 10.1109/tsm.2017.2749479
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Pt Gate Sink-In Process Details Impact on InP HEMT DC and RF Performance

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Cited by 15 publications
(4 citation statements)
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“…[18] Besides, the smaller d of device A caused by "Pt sinking" can also increase the V th and g m max . [19][20][21][22] Therefore, the formation of Pt distribution in Schottky contact metal can be explained as being due to the middle metal layer Pt spreading into the gate recess during the gate metal evaporation, which not only expands the gate length but also increases the Ti-based Schottky barrier height. The differences in V th and g m max between device A and device B are exactly caused by the differences in Pt distribution.…”
Section: Characteristicsmentioning
confidence: 99%
“…[18] Besides, the smaller d of device A caused by "Pt sinking" can also increase the V th and g m max . [19][20][21][22] Therefore, the formation of Pt distribution in Schottky contact metal can be explained as being due to the middle metal layer Pt spreading into the gate recess during the gate metal evaporation, which not only expands the gate length but also increases the Ti-based Schottky barrier height. The differences in V th and g m max between device A and device B are exactly caused by the differences in Pt distribution.…”
Section: Characteristicsmentioning
confidence: 99%
“…The Tgate electrode was formed with two separate exposures of a multilayer photoresist stack to define the gate foot and head separately and deposition of a Pt/Ti/Pt/Au metal stack. The gates were sunk nm through the InP etch-stop and into the AlInAs barrier at 250 • C as per [10] and passivated with a 15-nm Al 2 O 3 layer by atomic layer deposition (ALD). Careful measurements using focused ion-beam (FIB) cross sections on all structures confirmed a 50-nm gate footprint, as shown in Fig.…”
Section: Device Fabricationmentioning
confidence: 99%
“…InAs insets in indium-rich GaInAs channels evolved toward larger conduction band offsets and better carrier confinement [6]. Combined refinements in low-parasitics process architectures and layer epitaxy enabled record transconductances and short-circuited current-gain cutoff frequencies ( f T ) [7]- [9], as the two quantities are linked according to the following equation [10]:…”
Section: Introductionmentioning
confidence: 99%
“…Low noise microwave amplifiers based on high electron mobility transistors (HEMTs) are widely used in scientific applications ranging from radio astronomy [1] to quantum computing [2,3]. Decades of progress in device fabrication have yielded significant advances in figures of merit such as transconductance [4][5][6], gain [7], unity gain cutoff frequency [8][9][10], maximum oscillation frequency [11], and power consumption [12,13]. The resulting devices exhibit excellent noise performance, with minimum reported noise figures of HEMTs around a factor of 5 above the standard quantum limit in the 1-100 GHz frequency range [7,9,14,15].…”
Section: Introductionmentioning
confidence: 99%