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Dive into the research topics where T. M. Brennan is active.

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Featured researches published by T. M. Brennan.


IEEE Journal of Quantum Electronics | 1989

Resonant periodic gain surface-emitting semiconductor lasers

M. Y. A. Raja; Steven R. J. Brueck; Marek Osinski; Christian F. Schaus; John G. McInerney; T. M. Brennan; Burrell E. Hammons

A surface-emitting semiconductor laser structure with a vertical cavity, extremely short gain medium length, and enhanced gain at a specific design wavelength is described. The active region consists of a series of quantum wells spaced at one half the wavelength of a particular optical transition in the quantum wells. This special periodicity allows the antinodes of the standing-wave optical field to coincide with the gain elements, enhancing the frequency selectivity, increasing the gain in the vertical direction by a factor of two compared to a uniform medium or a nonresonant multiple quantum well, and substantially reducing amplified spontaneous emission. Optically pumped lasing was achieved in a GaAs/AlGaAs structure grown by molecular-beam epitaxy, with what is believed to be the shortest gain medium (310 nm) ever reported. >


IEEE Transactions on Microwave Theory and Techniques | 1995

Traveling-wave photodetectors for high-power, large-bandwidth applications

Vincent M. Hietala; G. A. Vawter; T. M. Brennan; B. E. Hammons

The traveling-wave photodetectors (TWPD) discussed here offer theoretical quantum efficiencies approaching 100% while maintaining a very large electrical bandwidth. Additionally, they are capable of dissipating the high-power levels required for large dynamic range applications. In this paper, the power dissipation limit of the TWPD is explored. A small-signal steady-state model is developed that includes the effects of electrical propagation losses along the detector. Fabrication details are presented and experimental data shows a 3/spl times/1250 /spl mu/m/sup 2/ detector with a 4.8-GHz bandwidth. >


Applied Physics Letters | 1994

Optical properties of two‐dimensional photonic lattices fabricated as honeycomb nanostructures in compound semiconductors

P. L. Gourley; Joel R. Wendt; G. A. Vawter; T. M. Brennan; B. E. Hammons

We have experimentally studied two‐dimensional photonic lattices, honeycomb nanostructures, fabricated by electron beam lithography with (Al,Ga)As materials. Surface normal optical properties were investigated by measuring reflectance to determine the effective index of refraction and lattice stability against degradation. Also, continuous wave and time‐resolved luminescence spectroscopy was used to assess electron‐hole recombination. Finally, light scattering was employed to study photon coupling and propagation through the lattice. These measurements show that the structures are stable, that nonradiative surface recombination is present, and that resonant coupling of light into/out of the lattice occurs at selected wavelengths satisfying a Bragg condition.


Applied Physics Letters | 1991

Coherent beams from high efficiency two‐dimensional surface‐emitting semiconductor laser arrays

P. L. Gourley; Mial E. Warren; G.R. Hadley; G. A. Vawter; T. M. Brennan; B. E. Hammons

We have fabricated and operated large two‐dimensional (2D) arrays of phase‐locked surface‐emitting semiconductor lasers. The arrays were fabricated by reactive ion beam etching of epitaxial Fabry–Perot resonators comprising GaAs/AlGaAs quantum wells surrounded by AlAs‐AlGaAs quarter‐wave mirrors. Different arrays corresponding to different pixel size (2–5 μm) and spacing (1–2 μm) were produced to investigate evanescent coupling between pixels. The arrays were photopumped so that the array size could be conveniently varied from 1×1, 2×2,... up to 20×20. Except for the 1×1 which emits a circular pattern, all arrays exhibit a well‐defined four‐lobed far‐field pattern in agreement with our theoretical analysis of the optical modes which predicts domination by the 2D out‐of‐phase eigenmode. As a consequence this pattern can be understood with simple Fraunhofer diffraction theory. The angular spread of the lobes, determined by the periodicity of the array elements, is 10° for the array with element size/spacing...


Applied Physics Letters | 1992

On-axis far-field emission from two-dimensional phase-locked vertical cavity surface-emitting laser arrays with an integrated phase-corrector

Mial E. Warren; P. L. Gourley; G.R. Hadley; G. A. Vawter; T. M. Brennan; B. E. Hammons; Kevin L. Lear

We have fabricated large, two‐dimensional (2D) arrays of optically pumped, phase‐locked vertical cavity surface‐emitting lasers that emit more than 50% of their light in a central on‐axis lobe. The emission of the arrays was modified from the usual four‐lobed far‐field of 2D coupled arrays by incorporation of a binary phase‐shift mask on the surface of the array. The array consists of Fabry–Perot resonators comprising GaAs/AlGaAs quantum wells surrounded by AlAs/AlGaAs quarterwave mirrors with a multiple order AlGaAs phase‐delay layer on the top mirror stack. The phase‐shift layer was etched away on alternating elements of the array. The resulting on‐axis emission had an angular width of 2° for an array of approximately 100 elements.


Applied Physics Letters | 1989

High‐efficiency TEM00 continuous‐wave (Al,Ga)As epitaxial surface‐emitting lasers and effect of half‐wave periodic gain

P. L. Gourley; T. M. Brennan; B.E. Hammons; Scott W. Corzine; Randall S. Geels; R. H. Yan; J.W. Scott; Larry A. Coldren

We report room‐temperature, continuous‐wave (cw), photopumped operation of (Al,Ga)As surface‐emitting lasers grown by molecular beam epitaxy. These monolithic semiconductor lasers comprise two multilayer semiconductor mirrors surrounding a layered active region. In the active region, GaAs quantum wells are spaced with half‐wave periodicity to center on standing‐wave maxima of the cavity optical field. By comparing threshold data for different lasers grown with and without half‐wave periodicity, we observe the first experimental evidence for reduced cw lasing threshold (as low as 2×104 W/cm2 ) with periodic gain in an epitaxial surface‐emitting laser. Up to 50 mW with high efficiency (35% total, 80% differential) and narrow spectral linewidth (2 A) have been measured. A very high quality beam with low divergence (2.5°) and circular TEM00 profile has been observed. All of these observations represent significant advances for surface‐emitting laser technology.


Applied Physics Letters | 1988

Reflection mass spectrometry of As incorporation during GaAs molecular beam epitaxy

Jeffrey Y. Tsao; T. M. Brennan; B.E. Hammons

An apertured and cryoshrouded mass spectrometer, which measures line‐of‐sight molecular fluxes from the surface, has been incorporated into a GaAs molecular beam epitaxy system. The spectrometer is simple to implement, yet is a powerful real‐time growth diagnostic. We have used the spectrometer to measure transient and steady‐state As incorporation from As4 during bilayer‐by‐bilayer growth of GaAs. We find, interestingly, that (1) the incorporation coefficient does not oscillate significantly; (2) transient incorporation coefficients depend on surface reconstruction, and may be higher than 0.5 at high Ga fluxes; and (3) in the absence of a Ga flux, excess Ga on the surface need not imply an incorporation coefficient of 0.5.


Applied Physics Letters | 1992

Optical Bloch waves in a semiconductor photonic lattice

P. L. Gourley; Mial E. Warren; G. A. Vawter; T. M. Brennan; B. E. Hammons

We have observed multiple optical Bloch waves in a semiconductor photonic lattice. This photonic lattice comprises epitaxial quarter‐wave periodic layers surrounding a periodic quantum‐well region. After growth, the layers are structured laterally into periodic square unit cells by reactive‐ion‐beam etching. When photoexcited, the lattice emits a complex angular distribution of photons that reflects its periodic structure. Scattered light is distributed according to the Laue conditions in analogy with x‐ray diffraction from a bulk crystal. Optical Bloch waves photostimulated in the lattice are analogous to electron Bloch waves in an atomic lattice. These optical Bloch waves exhibit long‐range translational symmetry and local symmetry due to the shape of the unit cell. Interestingly, the far‐field pattern of stimulated emission gives a direct mapping of the allowed Bloch wave vectors in the Brillouin zone. The mapping exhibits a wave‐vector gap at the Bragg condition and may be associated with a photonic e...


Chaos Solitons & Fractals | 1994

Transverse modes, vortices and vertical-cavity surface-emitting lasers

Francois Brown de Colstoun; G. Khitrova; Alexander V. Fedorov; T. R. Nelson; Curt W. Lowry; T. M. Brennan; B. Gene Hammons; Paul D. Maker

Abstract Injection locking dramatically modifies the phase and transverse output intensity profile of vertical-cavity surface-emitting lasers (VCSELs). Injection can induce a VCSEL to emit a high-order transverse mode. Vortices are generated by three different methods: insertion of a helicoidal phase mask, interference of two Gaussian beams, and injection locking of the TEM01 and TEM10 modes of a VCSEL to form the TEM∗01 donut mode. The first two methods stem from geometrical optics; the third method involves nonlinear mode competition in the laser cavity.


Applied Physics Letters | 1991

Novel reflectance modulator employing an InGaAs/AlGaAs strained‐layer superlattice Fabry–Perot cavity with unstrained InGaAs/InAlAs mirrors

I. J. Fritz; D. R. Myers; G. A. Vawter; T. M. Brennan; B. E. Hammons

We present a novel approach to optoelectronic devices by combining mechanically stable strained and unstrained epitaxial multilayers. We illustrate our approach with an optical reflectance modulator based on an asymmetric Fabry–Perot resonator designed to operate near 1.06 μm. The resonator is grown on a mechanically relaxed buffer of In0.11Ga0.89As deposited on a GaAs substrate. For mirrors, quarter‐wave stacks of In0.11Ga0.89As and In0.1Al0.9As, lattice matched to the buffer, are used. The Fabry–Perot cavity consists of an In0.23Ga0.77As/Al0.35Ga0.65As strained‐layer superlattice whose planar lattice constant also matches the buffer. Our first device operates at 1.04–1.05 μm depending on lateral position across the wafer. The insertion loss at resonance is less than 2 db and a fractional modulation of over 60% has been achieved with a 4 V bias swing.

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B. E. Hammons

Sandia National Laboratories

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D. R. Myers

Sandia National Laboratories

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P. L. Gourley

Sandia National Laboratories

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B.E. Hammons

Sandia National Laboratories

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G. A. Vawter

Sandia National Laboratories

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I. J. Fritz

Sandia National Laboratories

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J. P. Hohimer

Sandia National Laboratories

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J. F. Klem

Sandia National Laboratories

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