2014
DOI: 10.1063/1.4901290
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Gate-control efficiency and interface state density evaluated from capacitance-frequency-temperature mapping for GaN-based metal-insulator-semiconductor devices

Abstract: Articles you may be interested inModeling small-signal response of GaN-based metal-insulator-semiconductor high electron mobility transistor gate stack in spill-over regime: Effect of barrier resistance and interface states Interface trap characterization of atomic layer deposition Al2O3/GaN metal-insulator-semiconductor capacitors using optically and thermally based deep level spectroscopies Analysis of AlN/AlGaN/GaN metal-insulator-semiconductor structure by using capacitance-frequencytemperature mapping App… Show more

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Cited by 11 publications
(4 citation statements)
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“…The energy level depth of the interface states ( E C – E T ) can be derived from trapped electron emitting time constant τ e by the Shockley–Read–Hall (SRH) statistics: τe=1υthσnNCexptrue(ECETkTtrue), where υ th is thermal electron velocity, σ n is electron capture cross section, and N C is the effective density of states in conduction band in GaN. By frequency‐dependent C–V method , D it can be estimated from the following equation: Dit(E=EAVG)=1q(ΔVΔECSiNCSiNq) =CSiN (V2V1)qkT ln (f2/f1)CSiNq2, where V 1 and V 2 are the on‐set voltages for f 1 and f 2 ( f 1 < f 2 ), respectively. E AVG is the average energy between trap energy depth E 1 and E 2 .…”
Section: Resultsmentioning
confidence: 99%
“…The energy level depth of the interface states ( E C – E T ) can be derived from trapped electron emitting time constant τ e by the Shockley–Read–Hall (SRH) statistics: τe=1υthσnNCexptrue(ECETkTtrue), where υ th is thermal electron velocity, σ n is electron capture cross section, and N C is the effective density of states in conduction band in GaN. By frequency‐dependent C–V method , D it can be estimated from the following equation: Dit(E=EAVG)=1q(ΔVΔECSiNCSiNq) =CSiN (V2V1)qkT ln (f2/f1)CSiNq2, where V 1 and V 2 are the on‐set voltages for f 1 and f 2 ( f 1 < f 2 ), respectively. E AVG is the average energy between trap energy depth E 1 and E 2 .…”
Section: Resultsmentioning
confidence: 99%
“…6 On the other hand, in the case of the MIS devices, V th is affected by the insulator-semiconductor conduction band offset w and the fixed charge density σ int of the insulator-semiconductor interface. Various insulators such as oxides Al 2 O 3 , 7 HfO 2 , 8,9 TiO 2 , 10 AlSiO, 11,12 AlTiO, [13][14][15][16][17][18][19] oxynitrides TaON, 20 AlON, 21 and nitrides BN, 22,23 AlN [24][25][26][27][28] have been employed as a gate insulator for GaN-based devices, where V th can be modulated by both w and σ int . Similarly to f S , w is not uniquely determined by the electron affinity difference between the insulator and the semiconductor, and is affected by insulator-semiconductor interface treatments.…”
Section: Introductionmentioning
confidence: 99%
“…For high-speed and high-power applications, GaN-based metal-insulator-semiconductor field-effect transistors (MIS-FETs) have been extensively investigated using various gate insulators, such as high-dielectric-constant (high-k) oxides Al 2 O 3 [1], HfO 2 [2,3], TiO 2 [4], AlSiO [5,6], AlTiO [7][8][9][10][11][12], high-k oxynitrides TaON [13], AlON [14], and high-k nitrides BN [15,16], AlN [17][18][19][20][21]. In particular, Al x Ti y O (AlTiO), an alloy of Al 2 O 3 and TiO 2 , is an important insulator, because it can be applied to dielectric constant engineering, energy gap engineering, and interface charge engineering [11].…”
Section: Introductionmentioning
confidence: 99%