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Dive into the research topics where G. L. Olson is active.

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Featured researches published by G. L. Olson.


Applied Physics Letters | 1990

Kinetics of solid phase epitaxy in thick amorphous Si layers formed by MeV ion implantation

J.A. Roth; G. L. Olson; D. C. Jacobson; J. M. Poate

The kinetics of solid phase epitaxy (SPE) have been measured in MeV ion‐implanted amorphous Si layers up to 5 μm thick. Epitaxial crystallization in these layers occurs at a constant rate throughout the entire film, without loss of interface planarity or competition from random nucleation or twin formation. The activation energy for SPE in thick layers is found to be 2.70 eV, in excellent agreement with the value determined previously in much thinner films. The SPE kinetics are shown not to depend on the implant dose for doses up to 1000 times the threshold for amorphization. The presence of water vapor in the annealing ambient during SPE results in the indiffusion of hydrogen and a concomitant reduction of the SPE growth rate at distances as great as 2 μm from the surface. This effect may have important implications for the development of a microscopic model of the SPE process in silicon.


Thin Solid Films | 1998

Real-time monitoring and control of epitaxial semiconductor growth in a production environment by in situ spectroscopic ellipsometry

B Johs; C.M Herzinger; J.H Dinan; A Cornfeld; J.D Benson; D. Doctor; G. L. Olson; I Ferguson; M Pelczynski; P Chow; C.H Kuo; S. Johnson

To manufacture the next generation of epitaxially grown semiconductor device structures, real-time monitoring and control of the growth is considered a necessity to achieve acceptable yields. In situ spectroscopic ellipsometry (SE) has demonstrated sensitivity to important growth parameters, such as substrate temperature, layer thickness and composition; the literature also contains some examples of growth control by in situ SE. However, applying this characterization technique in a production environment presents a number of challenges. This article discusses these challenges and solutions which have been implemented on production-ready growth chambers. Real-time in situ SE composition monitoring results which were obtained on such chambers are in excellent agreement with ex situ characterization techniques. Preliminary composition control experiments, using in situ SE as the feedback sensor, are also presented.


Applied Physics Letters | 1988

Excimer laser‐assisted metalorganic vapor phase epitaxy of CdTe on GaAs

J. J. Zinck; Peter D. Brewer; John E. Jensen; G. L. Olson; L. W. Tutt

We have successfully grown CdTe (111) on GaAs (100) at 165 °C using a 248 nm excimer laser to photodissociate dimethylcadmium and diethyltellurium in the gas phase. Good crystalline quality of the layers is confirmed by x‐ray diffractometry. Growth rates up to 2 μm/h have been recorded in real time using time‐resolved reflectivity. Auger analysis reveals that the films are stoichiometric throughout the thickness of the layer, and that carbon and oxygen contaminants are below the level of detectability. We have used laser‐induced fluorescence spectroscopy to examine the photodissociation mechanism of diethyltellurium and have observed a linear dependence of Te atom production on excimer laser power.


Applied Physics Letters | 1990

Reversible modification of CdTe surface composition by excimer laser irradiation

Peter D. Brewer; J. J. Zinck; G. L. Olson

KrF excimer laser irradiation of CdTe at fluences below the melt threshold (≤75 mJ/cm2) removes surface layers and produces reversible changes in the surface composition that depend upon the laser fluence and number of laser pulses delivered to the surface. At fluences above ∼40 mJ/cm2 a Te‐rich layer is obtained. A stoichiometric composition can be restored by irradiation at reduced laser fluence. The primary desorption products are Cd and Te2, and the velocities of these species are well described by a Maxwellian distribution. The fluence‐dependent changes in CdTe surface composition are consistent with a photothermal mechanism based on the competition between formation and desorption of Te2 and desorption of Cd atoms from the laser‐irradiated surface.


Journal of Crystal Growth | 1999

Mbe growth of HgCdTe avalanche photodiode structures for low-noise 1.55 μm photodetection

T. J. de Lyon; Bonnie A. Baumgratz; George R. Chapman; Eli E. Gordon; Andrew T. Hunter; Mike D. Jack; J. E. Jensen; W. Johnson; B Johs; K. Kosai; W. Larsen; G. L. Olson; M. Sen; Bobby Walker; O. K. Wu

Molecular-beam epitaxy (MBE) has been utilized to fabricate HgCdTe heterostructure separate absorption and multiplication avalanche photodiodes (SAM-APD) sensitive to infrared radiation in the 1.1-1.6 μm spectral range, as an alternative technology to existing III-V APD detectors. Device structures were grown on CdZnTe(211)B substrates using CdTe, Te, and Hg sources with in situ In and As doping. The composition of the HgCdTe alloy layers was adjusted to achieve both efficient absorption of IR radiation in the 1.1-1.6 μm spectral range and low excess-noise avalanche multiplication. The Hg 1-x Cd x Te alloy composition in the gain region of the device, = 0.73, was selected to achieve equality between the bandgap energy and spin-orbit splitting to resonantly enhance the impact ionization of holes in the split-off valence band. The appropriate value of this alloy composition was determined from analysis of the 300 K bandgap and spin-orbit splitting energies of a set of calibration layers, using a combination of IR transmission and spectroscopic ellipsometry measurements. MBE-grown APD epitaxial wafers were processed into passivated mesa-type discrete device structures and diode mini-arrays using conventional HgCdTe process technology. Device spectral response, dark current density, and avalanche gain measurements were performed on the processed wafers. Avalanche gains in the range of 30-40 at reverse bias of 85-90 V and array-median dark current density below 2 x 10 -4 A/cm 2 at 40 V reverse bias have been demonstrated.


MRS Proceedings | 1990

The Effect of Hydrogen on the Kinetics of Solid Phase Epitaxy in Amorphous Silicon

J. A. Roth; G. L. Olson; D. C. Jacobson; J. M. Poate; C. Kirschbaum

This paper discusses the intrusion of H into a-Si layers during solid phase epitaxy and the effect of this H on the growth kinetics. We show that during annealing in the presence of water vapor, H is continuously generated at the oxidizing a-Si surface and diffuses into the amorphous layer, where it causes a reduction in the epitaxial growth rate. The measured variation of growth rate with the depth of the amorphous/crystal interface is correlated with the concentration of H at the interface. The diffusion coefficient for H in a-Si is determined by comparing measured depth profiles with calculated values. Hydrogen intrusion is observed even in layers annealed in vacuum and in inert gas ambients. Thin (


Journal of Crystal Growth | 2000

Status of HgCdTe-MBE technology for producing dual-band infrared detectors

Rajesh D. Rajavel; Peter D. Brewer; D. M. Jamba; J. E. Jensen; C LeBeau; G. L. Olson; J. A. Roth; W.S Williamson; James Bangs; P. Goetz; J.L. Johnson; E. A. Patten; Jerry A. Wilson

Progress on achieving reproducible growth of high performance, dual-band IR detector structures in HgCdTe grown by molecular beam epitaxy (MBE) is described. The reproducibility achieved in the MBE growth of n-p-n device structures comprising HgCdTe epitaxial layers with different composition and doping characteristics was evaluated from the run-to-run precision in the alloy composition, dopant concentration and dislocation density. For a series of 25 growth runs, the standard deviation of the alloy composition in the n-type absorbing layer was 0.002; the yield for the in situ n- and p-type doping process was > 95%; and the average dislocation density was < 5 x 10 5 cm -2 . In situ optical diagnostics, including spectroscopic ellipsometry and an optical absorption flux monitor were used for the real-time determination of the alloy composition and Cd flux during MBE growth of the two-color device structures. Focal plane arrays with 128 x 128 elements were fabricated for the simultaneous detection of two sub-bands in the MWIR spectrum. Average R o A values exceeding 1 x 10 6 and 2 x 10 5 Ω cm 2 were measured at 77 K for diodes operating at 4.0 and 4.5 μm, respectively, and the quantum efficiency was greater than 70% in each band. These results on MBE growth and device performance demonstrate that HgCdTe MBE technology is poised for the modest-scale production of advanced IR devices.


Optoelectronics '99 - Integrated Optoelectronic Devices | 1999

Epitaxial growth of HgCdTe 1.55-μm avalanche photodiodes by molecular beam epitaxy

Terence J. de Lyon; Bonnie A. Baumgratz; George R. Chapman; Eli E. Gordon; Andrew T. Hunter; Michael D. Jack; John E. Jensen; W. Johnson; Blaine D. Johs; K. Kosai; W. Larsen; G. L. Olson; M. Sen; Burt Walker

Separate absorption and multiplication avalanche photodiode (SAM-APD) device structures, operating in the 1.1 - 1.6 micrometer spectral range, have been fabricated in the HgCdTe material system by molecular-beam epitaxy. These HgCdTe device structures, which offer an alternative technology to existing III-V APD detectors, were grown on CdZnTe(211)B substrates using CdTe, Te, and Hg sources with in situ In and As doping. The alloy composition of the HgCdTe layers was adjusted to achieve both efficient absorption of IR radiation in the 1.1 - 1.6 micrometer spectral range and low excess-noise avalanche multiplication. To achieve resonant enhancement of hole impact ionization from the split-off valence band, the Hg1-xCdxTe alloy composition in the gain region of the device, x equals 0.73, was chosen to achieve equality between the bandgap energy and spin-orbit splitting. The appropriate value of this alloy composition was determined from analysis of the 300 K bandgap and spin-orbit splitting energies of a set of calibration layers, using a combination of IR transmission and spectroscopic ellipsometry measurements. MBE-grown APD epitaxial wafers were processed into passivated mesa-type discrete device structures and diode mini-arrays using conventional HgCdTe process technology. Device spectral response, dark current density, and avalanche gain measurements were performed on discrete diodes and diode mini- arrays on the processed wafers. Avalanche gains in the range of 30 - 40 at reverse bias of 85 - 90 V and array-median dark current density below 2 X 10-4 A/cm2 at 40 V reverse bias have been demonstrated.


MRS Proceedings | 1986

Excimer Laser-Assisted Deposition of GaAs, AlAs, and (Al,Ga)as from Lewis Acid-Base Adducts.

J. J. Zinck; Peter D. Brewer; J. E. Jensen; G. L. Olson; L. W. Tutt

Abstract : Laser-assisted deposition of GaAs, AL,As and (AL,Ga)As thin films on Ge100 substrates from trimethylgallium-trimethylarsenic and trimethylaluminum-trimethylarsenic Lewis acid-base adduct source materials is reported. A parametric study has been performed in which reactive gas pressure, substrate temperature, laser fluence, laser wavelength (248 nm or 193 nm), and orientation of the laser beam with respect to the substrate have been varied. In the case of irradiation parallel to the substrate, stoichiometric films of GaAs and (AL,Ga)As have been obtained. The data suggest that for irradiation perpendicular to the substrate a competition exists between desorption and photodeposition, which adversely affects film stoichiometry under the conditions studied.


International Symposium on Optical Science and Technology | 2001

Advances in HgCdTe-based infrared detector materials: the role of molecular-beam epitaxy

Terence J. de Lyon; Rajesh D. Rajavel; J. A. Roth; John E. Jensen; G. L. Olson; Peter D. Brewer; Andrew T. Hunter; Tod S. Williamson; Steven L. Bailey; James Bangs; A. A. Buell; George R. Chapman; Alex C. Childs; Eli E. Gordon; Michael D. Jack; S. M. Johnson; K. Kosai; Kevin D. Maranowski; E. A. Patten; J. M. Peterson; L. T. Pham; W. A. Radford; Valerie Randall; J. B. Varesi; Jerry A. Wilson

Since its initial synthesis and investigation more than 40 years ago, the HgCdTe alloy semiconductor system has evolved into one of the primary infrared detector materials for high-performance infrared focal-plane arrays (FPA) designed to operate in the 3-5 mm and 8-12 mm spectral ranges of importance for thermal imaging systems. Over the course of the past decade, significant advances have been made in the development of thin-film epitaxial growth techniques, such as molecular-beam epitaxy (MBE), which have enabled the synthesis of IR detector device structures with complex doping and composition profiles. The central role played by in situ sensors for monitoring and control of the MBE growth process are reviewed. The development of MBE HgCdTe growth technology is discussed in three particular device applications: avalanche photodiodes for 1.55 +m photodetection, megapixel FPAs on Si substrates, and multispectral IR detectors.

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