AlGaN/AlN/SiC Metal-Oxide-Semiconductor Heterostructure Field-Effect Transistors with Al 2 O 3 Gate-Oxide and Step-Graded AlGaN Channel
Al 0.75 Ga 0.25 N/n-Al x Ga 1-x N/Al 0.75 Ga 0.25 N/AlN metal-oxide-semiconductor heterostructure field-effect transistors (MOS-HFETs), grown on a SiC substrate, with step-graded Si-doped (n = 3 × 10 18 cm -3 ) widegap Al x Ga 1-x N channel and Al 2 O 3 gate-dielectric are investigated. Increased Al...
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Published in | Meeting abstracts (Electrochemical Society) Vol. MA2021-01; no. 33; p. 1086 |
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Main Authors | , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
30.05.2021
|
Online Access | Get full text |
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Summary: | Al
0.75
Ga
0.25
N/n-Al
x
Ga
1-x
N/Al
0.75
Ga
0.25
N/AlN metal-oxide-semiconductor heterostructure field-effect transistors (MOS-HFETs), grown on a SiC substrate, with step-graded Si-doped (n = 3 × 10
18
cm
-3
) widegap Al
x
Ga
1-x
N channel and Al
2
O
3
gate-dielectric are investigated. Increased Al-compositions with x = 0.25, 0.5, and 0.75 towards the buffer were devised in the composite widegap channel. The high-k Al
2
O
3
dielectric/passivation layer was grown by using a non-vacuum ultrasonic spray pyrolysis deposition (USPD) method. Experimental comparisons were made with respect to a conventional Schottky-gate HFET.
The epitaxial structure of the studied Al
2
O
3
-dielectric Al
0.75
Ga
0.25
N/n-Al
x
Ga
1-x
N/Al
0.75
Ga
0.25
N/AlN MOS-HFET (sample A) and Schottky-gate HFET (sample B). Both devices have the identical epitaxial structure grown on a SiC substrate by using a low-pressure metal-organic chemical vapor deposition (LP-MOCVD) system. The layer structure includes an undoped AlN buffer, a 20-nm undoped Al
0.75
Ga
0.25
N barrier, a 150-nm step-graded Si-doped (n = 3 × 10
18
cm
-3
) Al
x
Ga
1-x
N channel (x = 0.25, 0.5, and 0.75), and a 20-nm undoped Al
0.75
Ga
0.25
N barrier. Standard photolithography and lift-off techniques were used for device processing. For sample B, mesa etching was performed with respect to a 100-nm thick Ni barrier by using an inductively coupled-plasma reactive ion etcher (ICP-RIE). Flow rates were tuned and set at 10 sccm and 20 sccm for the mixed etching gases of BCl
3
and Cl
2
, respectively. The 20-nm undoped Al
0.75
Ga
0.25
N barrier was etched away before deposition of source/drain electrodes. Ti (10 nm)/Al (50 nm)/Ni (10 nm)/Au (50 nm) were evaporated. The source/drain ohmic contacts were formed by annealing the sample for 25 seconds at 900°C by using a rapid thermal annealing (RTA) system (ULVAC MILA-5000). Then, 30-nm thick Al
2
O
3
layer was deposited on the Al
0.75
Ga
0.25
N barrier by using the USPD technique. Finally, gate electrode of Ni (100 nm)/Au (50 nm) was evaporated after gate photolithography. As for sample A, the gate electrode was formed directly on the surface of Al
0.75
Ga
0.25
N barrier without oxide deposition.
Improved device performance of the present MOS-HFET design have been obtained, including maximum drain-source current density (
I
DS, max
) of 130.1 A/mm at
V
GS
= 10 V and
V
DS
= 20 V,
I
DS
at
V
GS
= 0 V (
I
DSS0
) of 83.1 mA/mm, on/off-current ratio (
I
on
/
I
off
) of 1.4 × 10
7
, maximum extrinsic transconductance (
g
m, max
) of 11.8 mS/mm, two-terminal off-state gate-drain breakdown voltage (
BV
GD
) of -404 V, and three-terminal on-state drain-source breakdown voltage (
BV
DS
) of 364 V at 300 K. The present MOS-HFET design has also shown high spectral responsivity (SR) of 737 A/W under 250-nm deep-UV radiation at 300 K. |
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ISSN: | 2151-2043 2151-2035 |
DOI: | 10.1149/MA2021-01331086mtgabs |