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Dive into the research topics where Andrew A. Allerman is active.

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Featured researches published by Andrew A. Allerman.


Applied Physics Letters | 2000

Minority carrier diffusion, defects, and localization in InGaAsN, with 2% nitrogen

S. R. Kurtz; Andrew A. Allerman; C. H. Seager; R. M. Sieg; E. D. Jones

Electron and hole transport in compensated, InGaAsN ({approx} 2% N) are examined through Hall mobility, photoconductivity, and solar cell photoresponse measurements. Short minority carrier diffusion lengths, photoconductive-response spectra, and doping dependent, thermally activated Hall mobilities reveal a broad distribution of localized states. At this stage of development, lateral carrier transport appears to be limited by large scale (>> mean free path) material inhomogeneities, not a random alloy-induced mobility edge.


Optics Letters | 1999

Intracavity Frequency Doubling of a Diode-Pumped, External Cavity, Surface Emitting Semiconductor Laser

Thomas D. Raymond; William J. Alford; Mary H. Crawford; Andrew A. Allerman

We present a compact, robust, solid-state blue-light (490-nm) source capable of greater than 5 mW of output in a TEM(00) mode. This device is an optically pumped, vertical external-cavity surface-emitting laser with an intracavity frequency-doubling crystal.


Journal of Applied Physics | 2009

Strain relaxation in AlGaN multilayer structures by inclined dislocations

D. M. Follstaedt; Stephen R. Lee; Andrew A. Allerman; Jerrold A. Floro

To examine further the strain relaxation produced by inclined threading dislocations in AlGaN, a heterostructure with three AlGaN layers having successively increasing Ga contents and compressive strains was grown on an AlN template layer by metalorganic vapor-phase epitaxy. The strain state of the layers was determined by x-ray diffraction (XRD) and the dislocation microstructure was characterized with transmission electron microscopy (TEM). As the GaN mole fraction of the heterostructure increased from 0.15 to 0.48, the increased epitaxial strain produced inclined dislocations with successively greater bend angles. Using the observed bend angles, which ranged from 6.7° to 17.8°, the measured strain relaxation within each layer was modeled and found to be accounted for by threading-dislocation densities of 6–7×109/cm2, in reasonable agreement with densities determined by TEM and XRD. In addition to the influence of lattice-mismatch strain on the average bend angle, we found evidence that local strain inh...


Applied Physics Letters | 1999

Deep Levels in p-Type InGaAsN Lattice Matched to GaAs

D. Kwon; R. J. Kaplar; S. A. Ringel; Andrew A. Allerman; S. R. Kurtz; E. D. Jones

Deep level transient spectroscopy (DLTS) measurements were utilized to investigate deep level defects in metal-organic chemical deposition (MOCVD)-grown unintentionally doped p-type InGaAsN films lattice matched to GaAs. The as-grown material displayed a high concentration of deep levels distributed within the bandgap, with a dominant hole trap at E{sub v} + 0.10 eV. Post-growth annealing simplified the deep level spectra, enabling the identification of three distinct hole traps at 0.10 eV, 0.23 eV, and 0.48 eV above the valence band edge, with concentrations of 3.5 x 10{sup 14} cm{sup {minus}3}, 3.8 x 10{sup 14} cm{sup {minus}3}, and 8.2 x 10{sup 14} cm{sup {minus}3}, respectively. A direct comparison between the as-grown and annealed spectra revealed the presence of an additional midgap hole trap, with a concentration of 4 x 10{sup 14} cm{sup {minus}3} in the as-grown material. The concentration of this trap is sharply reduced by annealing, which correlates with improved material quality and minority carrier properties after annealing. Of the four hole traps detected, only the 0.48 eV level is not influenced by annealing, suggesting this level may be important for processed InGaAsN devices in the future.


Japanese Journal of Applied Physics | 2005

Junction Temperature in Ultraviolet Light-Emitting Diodes

Y. Xi; Thomas Gessmann; J.-Q. Xi; Jong Kyu Kim; Jay M. Shah; E. Fred Schubert; Arthur J. Fischer; Mary H. Crawford; Katherine H. A. Bogart; Andrew A. Allerman

The junction temperature and thermal resistance of AlGaN and GaInN ultraviolet (UV) light-emitting diodes (LEDs) emitting at 295 and 375 nm, respectively, are measured using the temperature coefficient of diode-forward voltage. An analysis of the experimental method reveals that the diode-forward voltage has a high accuracy of ±3°C. A comprehensive theoretical model for the dependence of diode-forward voltage (Vf) on junction temperature (Tj) is developed taking into account the temperature dependence of the energy gap and the temperature coefficient of diode resistance. The difference between the junction voltage temperature coefficient (dVj/dT) and the forward voltage temperature coefficient (dVf/dT) is shown to be caused by diode series resistance. The data indicate that the n-type neutral regions are the dominant resistive element in deep-UV devices. A linear relationship between junction temperature and current is found. Junction temperature is also measured by the emission-peak-shift method. The high-energy slope of the spectrum is explored in the measurement of carrier temperature.


Nature Communications | 2013

Strong coupling in the sub-wavelength limit using metamaterial nanocavities

Alexander Benz; Salvatore Campione; Sheng Liu; Ines Montano; J. F. Klem; Andrew A. Allerman; Wendt; Michael B. Sinclair; Filippo Capolino; Igal Brener

The interaction between cavity modes and optical transitions leads to new coupled light-matter states in which the energy is periodically exchanged between the matter states and the optical mode. Here we present experimental evidence of optical strong coupling between modes of individual sub-wavelength metamaterial nanocavities and engineered optical transitions in semiconductor heterostructures. We show that this behaviour is generic by extending the results from the mid-infrared (~10 μm) to the near-infrared (~1.5 μm). Using mid-infrared structures, we demonstrate that the light-matter coupling occurs at the single resonator level and with extremely small interaction volumes. We calculate a mode volume of 4.9 × 10−4 (λ/n)3 from which we infer that only ~2,400 electrons per resonator participate in this energy exchange process.


Journal of Vacuum Science & Technology B | 2004

High field transport in GaN/AlGaN heterostructures

J.M. Barker; D. K. Ferry; Stephen M. Goodnick; D.D. Koleske; Andrew A. Allerman; R. J. Shul

Experimental as well as theoretical studies have been performed on the velocity-field characteristics of AlGaN/GaN heterostructures. A comparison of these studies shows that the experimental velocities are comparable to those expected from previously published simulations based upon Monte Carlo techniques. Several possible mechanisms for the low value of the velocity previously found are discussed, including nonequilibrium phonons and local inhomogeneities in the field.


Applied Physics Letters | 2002

Deep-level defects in InGaAsN grown by molecular-beam epitaxy

R. J. Kaplar; S. A. Ringel; S. R. Kurtz; J. F. Klem; Andrew A. Allerman

Deep-level transient spectroscopy (DLTS) studies on both p-type unintentionally doped and n-type (Si-doped), 1.05 eV band gap InGaAsN grown by molecular-beam epitaxy are reported. Two majority-carrier hole traps were observed in p-type material, H3′ (0.38 eV) and H4′ (0.51 eV), and no evidence was found for the presence of minority-carrier electron traps. In n-type material, we observed a shallow distribution of electron levels, E1′, as well as a deep electron trap E4′ (0.56 eV) and a deep hole trap H5′ (0.71 eV). All DLTS peaks observed were broad and are thus consistent with continuous defect distributions and/or groups of closely spaced discrete energy levels in the band gap. Comparison of the spectra to previously reported spectra of metalorganic chemical vapor deposition-grown InGaAsN of the same composition revealed some similarities and some differences, suggesting that some of the observed deep levels are due to intrinsic physical sources, whereas others are specific to the growth technique used.


Journal of Applied Physics | 2011

Electrical characterization of n-type Al0.30Ga0.70N Schottky diodes

A. R. Arehart; Andrew A. Allerman; S. A. Ringel

The carrier trapping properties and current transport behavior of Ni/n-Al0.30Ga0.70N Schottky diodes were quantitatively characterized by a combination of deep level optical spectroscopy (DLOS), thermally based deep level transient spectroscopy (DLTS), current-voltage-temperature (I-V-T), and internal photoemission (IPE) measurements. High quality Schottky diode behavior was observed with an IPE-determined barrier height of 1.66 eV and the observed temperature-independent reverse leakage current behavior was found to be consistent with field emission in reverse bias and thermionic-field emission in forward bias as the dominant transport mechanisms. The trap spectroscopy measurements revealed the presence of several bandgap states located at EC–0.9 eV (seen by both DLOS and DLTS), EC–1.5, EC–3.11, and EC–3.93 eV—all via DLOS. The EC–3.10 level, which is present in very high concentration, is found to correlate with the energy position expected for the cation vacancy in AlGaN, based on the vacuum referred b...


Applied Physics Letters | 1999

Origin of the Time-Dependence of Wet Oxidation of AlGaAs

Carol I. H. Ashby; Monica M. Bridges; Andrew A. Allerman; B. E. Hammons; H. Q. Hou

The time dependence of the wet oxidation of high-Al-content AlGaAs can be either linear, indicating reaction-rate limitation, or parabolic, indicating diffusion-limited rates. The transition from linear to parabolic time dependence can be explained by the increased rate of the formation of intermediate As2O3 versus its reduction to elemental As. A steadily increasing thickness of the As2O3-containing region at the oxidation front will shift the process from the linear to the parabolic regime. This shift from reaction-rate limited (linear) to diffusion-limited (parabolic) time dependence is favored by increasing temperature or increasing Al mole fraction.

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Andrew Armstrong

Sandia National Laboratories

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Mary H. Crawford

Sandia National Laboratories

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S. R. Kurtz

Sandia National Laboratories

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Albert G. Baca

Sandia National Laboratories

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E. D. Jones

Sandia National Laboratories

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Robert Kaplar

Sandia National Laboratories

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Arthur J. Fischer

Sandia National Laboratories

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Michael W. Moseley

Sandia National Laboratories

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Jonathan J. Wierer

Sandia National Laboratories

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Daniel D. Koleske

Sandia National Laboratories

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