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Dive into the research topics where J. H. Leach is active.

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Featured researches published by J. H. Leach.


Applied Physics Letters | 2007

High electron mobility in nearly lattice-matched AlInN∕AlN∕GaN heterostructure field effect transistors

J. Xie; X. Ni; M. Wu; J. H. Leach; Ü. Özgür; Hadis Morkoç

High electron mobility was achieved in Al1−xInxN∕AlN∕GaN (x=0.20–0.12) heterostructure field effect transistors (HFETs) grown by metal-organic chemical vapor deposition. Reduction of In composition from 20% to 12% increased the room temperature equivalent two-dimensional-electron-gas density from 0.90×1013to1.64×1013cm−2 with corresponding electron mobilities of 1600 and 1410cm2∕Vs, respectively. The 10K mobility reached 17600cm2∕Vs for the nearly lattice-matched Al0.82In0.18N∕AlN∕GaN heterostructure with a sheet carrier density of 9.6×1012cm−2. For comparison, the AlInN∕GaN heterostructure without the AlN spacer exhibited a high sheet carrier density (2.42×1013cm−2) with low mobility (120cm2∕Vs) at room temperature. The high mobility in our samples is in part attributed to ∼1nm AlN spacer which significantly reduces the alloy scattering as well as provides a smooth interface. The HFETs having gate dimensions of 1.5×40μm2 and a 5μm source-drain separation exhibited a maximum transconductance of ∼200mS∕mm ...


Scientific Reports | 2013

Universal phonon mean free path spectra in crystalline semiconductors at high temperature

Justin P. Freedman; J. H. Leach; Edward A. Preble; Zlatko Sitar; Robert F. Davis; Jonathan A. Malen

Thermal conductivity in non-metallic crystalline materials results from cumulative contributions of phonons that have a broad range of mean free paths. Here we use high frequency surface temperature modulation that generates non-diffusive phonon transport to probe the phonon mean free path spectra of GaAs, GaN, AlN, and 4H-SiC at temperatures near 80 K, 150 K, 300 K, and 400 K. We find that phonons with MFPs greater than 230 ± 120 nm, 1000 ± 200 nm, 2500 ± 800 nm, and 4200 ± 850 nm contribute 50% of the bulk thermal conductivity of GaAs, GaN, AlN, and 4H-SiC near room temperature. By non-dimensionalizing the data based on Umklapp scattering rates of phonons, we identified a universal phonon mean free path spectrum in small unit cell crystalline semiconductors at high temperature.


Applied Physics Letters | 2009

Degradation in InAlN/GaN-based heterostructure field effect transistors: Role of hot phonons

J. H. Leach; Congyong Zhu; M. Wu; X. Ni; X. Li; J. Xie; Ü. Özgür; Hadis Morkoç; J. Liberis; E. Šermukšnis; A. Matulionis; H. Cheng; Cagliyan Kurdak

We report on high electric field stress measurements at room temperature on InAlN/AlN/GaN heterostructure field effect transistor structures. The degradation rate as a function of the average electron density in the GaN channel (as determined by gated Hall bar measurements for the particular gate biases used), has a minimum for electron densities around 1×1013 cm−2, and tends to follow the hot phonon lifetime dependence on electron density. The observations are consistent with the buildup of hot longitudinal optical phonons and their ultrafast decay at about the same electron density in the GaN channel. In part because they have negligible group velocity, the build up of these hot phonons causes local heating, unless they decay rapidly to longitudinal acoustic phonons, and this is likely to cause defect generation which is expected to be aggravated by existing defects. These findings call for modified approaches in modeling device degradation.


Semiconductor Science and Technology | 2008

Hot-electron energy relaxation time in AlInN/AlN/GaN 2DEG channels

A. Matulionis; J. Liberis; E. Šermukšnis; J. Xie; J. H. Leach; M. Wu; Hadis Morkoç

A microwave noise technique has been used for experimental investigation, at room temperature, of power dissipation in the voltage-biased two-dimensional electron gas channel located in the GaN layer of a lattice-matched Al0.82In0.18N/AlN/GaN heterostructure. No saturation of the relaxation time is found in the investigated electron temperature range up to ~2800 K: the hot-electron energy relaxation time decreases from ~6 ps at near equilibrium to 75 ± 20 fs at ~200 nW/electron. The electron drift velocity reaches ~1.8 × 107 cm s−1 at 65 kV cm−1 electric field. The hot-phonon effect on power dissipation is discussed.


Proceedings of the IEEE | 2010

Small Signal Equivalent Circuit Modeling for AlGaN/GaN HFET: Hybrid Extraction Method for Determining Circuit Elements of AlGaN/GaN HFET

Q. Fan; J. H. Leach; Hadis Morkoç

The developments in AlGaN/GaN heterojunction field effect transistors (HFETs) are beginning to allow harnessing of the great potential of this technology in high-power radio-frequency (RF) applications. However, the integration of HFET into a circuit environment requires accurate small and large signal modeling of the device operating under various biasing conditions. The conventional small signal equivalent circuit modeling methods consist of “cold” measurements for extracting parasitic elements, and on-bias measurements in determining the intrinsic device circuit elements. Also, the optimization routines are often explored directly using the “hot” measurement data to minimize errors. In this paper, an 18-element small signal equivalent circuit model for AlGaN/GaN HFET is proposed and implemented, and contrasted to various de-embedding methods. Among the methods treated, the hot-FET optimization extraction based on the parasitic capacitances obtained from cold measurements leads to the smallest error between the simulated S-parameters and the measured ones at all bias points employed, with an average error of about 5%. This hybrid extraction algorithm is strengthened by imposing constraints to avoid any nonphysical convergence. We note that the extrinsic parasitics determined by this method differ considerably from the values obtained by cold-FET measurements, which implies that the assumption on the bias independency for extrinsic parameters in the latter method might be questionable for AlGaN/GaN HFET.


Applied Physics Letters | 2004

The effect of hydrogen etching on 6H-SiC studied by temperature-dependent current-voltage and atomic force microscopy

S. Doğan; D. Johnstone; F. Yun; S. Sabuktagin; J. H. Leach; A. A. Baski; Hadis Morkoç; G. Li; Biswa N. Ganguly

6H–SiC was etched with hydrogen at temperatures between 1000 and 1450°C. The etched Si-terminated face for the 6H‐SiC wafer was investigated by atomic force microscopy and temperature-dependent current–voltage (I–V–T) measurements. Mechanical polishing damage was effectively removed by hydrogen etching at temperatures above 1250°C. Atomic force microscopy images revealed that very good surface morphology, atomic layer flatness, and large and large step width were achieved. Schottky diode characteristics were investigated in detail by current–voltage and temperature-dependent current–voltage measurements, and the results showed a transition from defect assisted tunneling to thermionic emission as the annealing temperature was increased from 1250 to 1450°C.6H–SiC was etched with hydrogen at temperatures between 1000 and 1450°C. The etched Si-terminated face for the 6H‐SiC wafer was investigated by atomic force microscopy and temperature-dependent current–voltage (I–V–T) measurements. Mechanical polishing damage was effectively removed by hydrogen etching at temperatures above 1250°C. Atomic force microscopy images revealed that very good surface morphology, atomic layer flatness, and large and large step width were achieved. Schottky diode characteristics were investigated in detail by current–voltage and temperature-dependent current–voltage measurements, and the results showed a transition from defect assisted tunneling to thermionic emission as the annealing temperature was increased from 1250 to 1450°C.


Proceedings of the IEEE | 2010

Status of Reliability of GaN-Based Heterojunction Field Effect Transistors

J. H. Leach; Hadis Morkoç

GaN-based heterojunction field effect transistors (HFETs) will play major roles in the high-power, high-frequency military and commercial arenas for microwave and millimeter wave transmitters and receivers used in communications and radar devices. In fact, devices operative in the X-band (7-12.5 GHz) and beyond are already at market and boast quite impressive performances. Having improved the crystal quality now to levels where the reliability [expressed as mean time to failure (MTTF)] is claimed to exceed ten million hours, the work now needs to focus on which of the physical mechanisms responsible for degradation are the most important, and how the existing degradation accelerates subsequent degradation, ultimately resulting in device failure. Available data show that not all devices from the same wafer show similar longevity and the wide spread of activation energies reported for three-temperature extrapolation-based predictions of the lifetime are troubling. If we hope to make consistent, reliable predictions of device lifetimes, particularly when the devices are being pushed in radio-frequency (RF) operation to near their limits, more work will need to be done in characterizing the long term stability of the devices, and new physical models for the failure mechanisms will have to be developed.


Applied Physics Letters | 2007

Electron mobility in InGaN channel heterostructure field effect transistor structures with different barriers

J. Xie; J. H. Leach; X. Ni; M. Wu; Ryoko Shimada; Ü. Özgür; Hadis Morkoç

InGaN possesses higher electron mobility and velocity than GaN, and therefore is expected to lead to relatively better performances for heterostructure field effect transistors (HFETs). However, the reported mobilities for AlGaN∕InGaN HFETs are lower than GaN channel HFETs. To address this issue, we studied the effect of different barriers on the Hall mobility for InGaN channel HFETs grown by metal organic chemical vapor deposition. Unlike the conventional AlGaN barrier, the AlInN barrier can be grown at the same temperature as the InGaN channel layer, alleviating some of the technological roadblocks. Specifically, this avoids possible degradation of the thin InGaN channel during AlGaN growth at high temperatures; and paves the way for better interfaces. An undoped In0.18Al0.82N∕AlN∕In0.04Ga0.96N HFET structure exhibited a μH=820cm2∕Vs, with a ns=2.12×1013cm−2 at room temperature. Moreover, with an In-doped AlGaN barrier, namely, Al0.24In0.01Ga0.75N, grown at 900°C, the μH increased to 1230cm2∕Vs with a n...


Applied Physics Letters | 2009

Plasmon-enhanced heat dissipation in GaN-based two-dimensional channels

A. Matulionis; J. Liberis; I. Matulionienė; M. Ramonas; E. Šermukšnis; J. H. Leach; M. Wu; X. Ni; X. Li; Hadis Morkoç

Decay of nonequilibrium longitudinal optical (LO) phonons is investigated at room temperature in two-dimensional electron gas channels confined in nearly lattice-matched InAlN/AlN/GaN structures. A nonmonotonous dependence of the LO-phonon lifetime on the supplied electric power is reported for the first time and explained in terms of plasmon–LO-phonon resonance tuned by applied bias at a fixed sheet density (8×1012 cm−2). The shortest lifetime of 30±15 fs is found at the power of 20±10 nW/electron.


Journal of Applied Physics | 2009

Electron drift velocity in lattice-matched AlInN/AlN/GaN channel at high electric fields

L. Ardaravičius; M. Ramonas; J. Liberis; O. Kiprijanovič; A. Matulionis; J. Xie; M. Wu; J. H. Leach; Hadis Morkoç

Hot-electron transport was probed by nanosecond-pulsed measurements for a nominally undoped two-dimensional channel confined in a nearly lattice-matched Al0.82In0.18N/AlN/GaN structure at room temperature. The electric field was applied parallel to the interface, the pulsed technique enabled minimization of Joule heating. No current saturation was reached at fields up to 180 kV/cm. The effect of the channel length on the current is considered. The electron drift velocity is deduced under the assumption of uniform electric field and field-independent electron density. The highest estimated drift velocity reaches ∼3.2×107 cm/s when the AlN spacer thickness is 1 nm. At high fields, a weak (if any) dependence of the drift velocity on the spacer thickness is found in the range from 1 to 2 nm. The measured drift velocity is low for heterostructures with thinner spacers (0.3 nm).

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Hadis Morkoç

Virginia Commonwealth University

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Ü. Özgür

Virginia Commonwealth University

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M. Wu

Virginia Commonwealth University

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X. Ni

Virginia Commonwealth University

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X. Li

Virginia Commonwealth University

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J. Xie

Virginia Commonwealth University

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K. R. Evans

Wright-Patterson Air Force Base

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Edward A. Preble

North Carolina State University

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V. Avrutin

Virginia Commonwealth University

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D. Johnstone

Virginia Commonwealth University

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