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Featured researches published by R. Bhat.


Applied Physics Letters | 1987

Extreme selectivity in the lift‐off of epitaxial GaAs films

Eli Yablonovitch; Thomas J. Gmitter; J. P. Harbison; R. Bhat

We have discovered conditions for the selective lift‐off of large area epitaxial AlxGa1−xAs films from the substrate wafers on which they were grown. A 500‐A‐thick AlAs release layer is selectivity etched away, leaving behind a high‐quality epilayer and a reusable GaAs substrate. We have measured a selectivity of ≳107 between the release layer and Al0.4Ga0.6As. This process relies upon the creation of a favorable geometry for the outdiffusion of dissolved H2 gas from the etching zone.


Applied Physics Letters | 1987

Dramatic enhancement in the gain of a GaAs/AlGaAs heterostructure bipolar transistor by surface chemical passivation

C. J. Sandroff; R.N. Nottenburg; J.‐C. Bischoff; R. Bhat

With a simple chemical treatment we have passivated nonradiative recombination centers at the periphery of a GaAs/AlGaAs heterostructurebipolar transistor, resulting in a 60‐fold increase in the current gain of the device at low collector currents. This large enhancement in gain was achieved by spin coatingthin films of Na2S9H2O onto the devices after their fabrication. We briefly discuss the passivation mechanism and the implications for other III‐V optoelectronic devices.


Journal of Applied Physics | 1986

Optical properties of AlxGa1−x As

D. E. Aspnes; S. M. Kelso; R. A. Logan; R. Bhat

We report pseudodielectric function 〈e〉 data for AlxGa1−xAs alloys of target compositions x=0.00–0.80 in steps of 0.10 grown by liquid‐phase epitaxy and measured by spectroellipsometry. Cleaning procedures that produce abrupt interfaces between the technologically relevant alloys x≤0.5 and the ambient are described. The 〈e2〉 data are corrected near the fundamental direct absorption edge by a Kramers–Kronig analysis of the 〈e1〉 data to circumvent a limitation of the rotating‐analyzer ellipsometric technique. The results and the associated pseudooptical functions 〈n〉, 〈R〉, and 〈α〉 are listed in tabular form. Accurate values of the E0 and E1 threshold energies are determined from these spectra by Fourier methods. From these values, and from similar values for a GaAs‐capped AlAs sample grown by organometallic chemical vapor deposition, the dependencies of the E0 and E1 interband critical point energies on nominal composition are obtained. Cubic polynomial representations of these dependences are determined to...


Applied Physics Letters | 1987

Nearly ideal electronic properties of sulfide coated GaAs surfaces

Eli Yablonovitch; C. J. Sandroff; R. Bhat; Thomas J. Gmitter

We have discovered that a class of inorganic sulfides [Li2S, (NH4)2S, Na2S⋅9H2O, etc.] imparts excellent electronic properties to GaAs surfaces. The surface recombination velocity at the interface between Na2S⋅9H2O and GaAs begins to approach that of the nearly ideal AlGaAs/GaAs interface. We propose the formation of a robust covalently bonded sulfide layer to explain the favorable electronic quality of such interfaces.


Applied Physics Letters | 1996

Wavelength conversion by difference frequency generation in AlGaAs waveguides with periodic domain inversion achieved by wafer bonding

S. J. B. Yoo; C. Caneau; R. Bhat; M. A. Koza; A. Rajhel; Neo Antoniades

Wavelength conversion by difference‐frequency generation is achieved in a periodically domain reversed AlGaAs waveguide. The AlGaAs waveguide is epitaxially grown on a template substrate where a periodic crystal domain inversion is achieved using wafer bonding, selective etching, and organometallic chemical vapor deposition. Wavelength conversion experiments on a fabricated buried heterowaveguide showed a 90 nm conversion bandwidth, polarization diversified operation, and polarization independent conversion efficiency. The experimental results also showed linearity and spectral inversion, which imply transparency to signal formats including analog and frequency modulation. Simultaneous conversion of multiple input wavelengths with no measurable cross talk is also demonstrated.


Applied Physics Letters | 1989

Single quantum wire semiconductor lasers

E. Kapon; S. Simhony; R. Bhat; D. M. Hwang

Single quantum wire GaAs/AlGaAs injection lasers were fabricated using organometallic chemical vapor deposition on V‐grooved GaAs substrates. The quantum wire active region has a crescent‐shaped cross section ∼100 A thick and less than 1000 A wide. Amplified spontaneous emission and lasing spectra of the quantum wire lasers exhibit effects due to transitions between quasi‐one‐dimensional subbands separated by ∼10 meV. Single quantum wire laser structures with tight optical confinement exhibited threshold currents as low as 3.5 mA for uncoated devices at room temperature.


Journal of Crystal Growth | 1988

Patterned quantum well heterostructures grown by OMCVD on non-planar substrates: Applications to extremely narrow SQW lasers

R. Bhat; E. Kapon; D. M. Hwang; M.A. Koza; C.P. Yun

Abstract We have studied the OMCVD growth of GaAs/AlGaAs quantum well heterostructures on non-planar substrates in the temperature range of 625 to 750°C. The lateral variation in layer thickness and other growth features were found to depend not only on the growth temperature but also on the aluminum content of the layer. An example of the application of this technique of producing lateral thickness variations in quantum well heterostructures to a quantum well semiconductor laser is given. A unique feature of this laser is the formation of a quantum-wire-like crescent shaped active region at the center of a two-dimensional optical waveguide.


Applied Physics Letters | 1991

Monolithic InP/InGaAsP/InP Grating Spectrometer for the 1.48-1.56 μm Wavelength Range

J.B.D. Soole; Axel Scherer; H. P. LeBlanc; N.C. Andreadakis; R. Bhat; M. A. Koza

We report a two‐dimensional grating spectrometer implemented in an InP/InGaAsP/InP planar waveguide for use in the low‐loss 1.5 μm wavelength fiber band. The spectrometer uses a single vertical‐walled focusing reflection grating to disperse 78 channels, spaced at 1 nm intervals, with diffraction‐limited resolution (∼0.3 nm) and a high channel isolation (≳19 dB). The spectrometer may be used such that it is insensitive to the state of the input polarization.


Applied Physics Letters | 1995

QUASI-PHASE-MATCHED SECOND-HARMONIC GENERATION IN ALGAAS WAVEGUIDES WITH PERIODIC DOMAIN INVERSION ACHIEVED BY WAFER-BONDING

S. J. B. Yoo; R. Bhat; C. Caneau; M. A. Koza

Quasi‐phase‐matched second‐harmonic generation is observed in an AlGaAs waveguide. The AlGaAs waveguide is epitaxially grown on a template substrate where a periodic crystal domain inversion is achieved using wafer bonding and organometallic chemical vapor deposition. A scanning electron micrograph of the waveguide cross section reveals a distinct propagation of the crystal domain boundaries in the epitaxial growth direction. Second‐harmonic generation measurements on a fabricated rib‐loaded waveguide show a clear quadratic dependence of the second‐harmonic power to the input fundamental power. The peak conversion efficiency is 4.9%/W whereas the theoretical value is 124%/W for an ideal waveguide with no loss and with equal domain dimensions. A significant increase in the conversion efficiency is expected with reduced scattering losses realized by improved epitaxial growth and fabrication processes.


Applied Physics Express | 2009

500-nm Optical Gain Anisotropy of Semipolar (1122) InGaN Quantum Wells

Dmitry Sizov; R. Bhat; Jerome Napierala; Chad S. Gallinat; Kechang Song; Chung-En Zah

We studied the effect of carrier population on light emission polarization of green InGaN quantum wells (QWs) on the semipolar (1122) plane. The 3 nm thick QWs emitting light at about 540 nm at low pumping power have electrical field (E) component E∥[1123] stronger than that E∥[1100]. However, we found that increasing the pumping power changed the sign of the polarization ratio. Using the varied stripe length (VSL) method, we measured the optical gain for light propagating ∥[1123] direction to be ~2 times that of light propagating ∥[1100] direction. We explain this behavior by inhomogeneous QW state filling.

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M. A. Koza

Telcordia Technologies

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M.A. Koza

Telcordia Technologies

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D. M. Hwang

Telcordia Technologies

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E. Kapon

École Polytechnique Fédérale de Lausanne

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C.E. Zah

Telcordia Technologies

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