Kevin H. Smith
Harris Corporation
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Featured researches published by Kevin H. Smith.
IEEE Photonics Technology Letters | 2005
Tyson L. Lowder; Kevin H. Smith; Benjamin L. Ipson; Aaron R. Hawkins; Richard H. Selfridge; Stephen M. Schultz
We present a new type of fiber Bragg grating (FBG) that can be used in high-temperature sensing applications. We use the flat side of a D-shaped optical fiber as a platform to etch the grating into the surface of the fiber. Because the grating becomes a physical feature of the fiber, it is not erased at high temperatures as are standard FBGs. These surface relief fiber Bragg gratings will operate up to high temperatures. We provide a brief explanation of the fabrication process and present our results for operation up to 1100/spl deg/C.
Applied Optics | 2003
Douglas J. Markos; Benjamin L. Ipson; Kevin H. Smith; Stephen M. Schultz; Richard H. Selfridge; Thomas D. Monte; Richard Dyott; Gregory Miller
The partial removal of a section of the core from a continuous D-shaped optical fiber is presented. In the core removal process, selective chemical etching is used with hydrofluoric (HF) acid. A 25% HF acid solution removes the cladding material above the core, and a 5% HF acid solution removes the core. A red laser with a wavelength of 670 nm is transmitted through the optical fiber during the etching. The power transmitted through the optical fiber is correlated to the etch depth by scanning electron microscope imaging. The developed process provides a repeatable method to produce an optical fiber with a specific etch depth.
Applied Optics | 2004
Kevin H. Smith; Doug J. Markos; Benjamin L. Ipson; Stephen M. Schultz; Richard H. Selfridge; John P. Barber; Kevin J. Campbell; Thomas D. Monte; Richard Dyott
We present a method for fabricating an in-fiber electro-optic polymer waveguide within a D-shaped optical fiber. A combined process of selective chemical etching and spin coating creates a 2-cm in-fiber poly(methyl methacrylate)-DR1 dye polymer waveguide section with an overall insertion loss of micro 1.6 dB at 1550 nm. Numerical simulations show that, for in-fiber polymer waveguides to have low loss, the polymer layers thickness must be kept below a certain value so that it will not support slab waveguide modes. Long transition regions between the unetched fiber and the polymer waveguide section also reduce loss. We analyze the efficiency of an in-fiber polymer waveguide by simulating its theoretical performance as an electro-optic modulator.
Applied Optics | 2007
Damien Weidmann; Kevin H. Smith; Brian N. Ellison
An experimental investigation of high-frequency noise, i.e., up to 3 GHz, exhibited by a 9.7 μm quantum cascade laser, is described. Noise characteristics and measurements of a liquid-nitrogen-cooled continuous-wave distributed-feedback laser are presented. Well defined sets of narrow and intense resonance peaks have been observed in the 10-300 MHz range. Measurements of relative intensity noise have been performed. It is also shown that quantum-cascade lasers are sensitive to optical feedback. The excess noise generated by the feedback has been investigated under well defined conditions. A description of the experimental phenomenon is presented along with methods of minimizing optical feedback.
Optics Express | 2004
Kevin H. Smith; Richard H. Selfridge; Stephen M. Schultz; Douglas J. Markos; Benjamin L. Ipson
This paper presents the analysis of a 2 cm long in-fiber polymer waveguide formed on the platform of a D-shaped optical fiber. Numerical simulations provide an understanding of the major loss mechanisms for feasible in-fiber polymer waveguide geometries. The primary loss mechanism is determined to be excitation of slab modes on the flat surface of the fiber with transition geometry being the next major contribution to loss.
Proceedings of SPIE | 2011
Peter A. Wasilousky; Kevin H. Smith; Ryan Glasser; Geoffrey L. Burdge; Lee M. Burberry; Bill Deibner; Michael Silver; Robert Peach; Christopher Visone; Prem Kumar; Oo Kaw Lim; Gideon Alon; Chao Hsiang Chen; Amar R. Bhagwat; Paritosh Manurkar; Michael Vasilyev; Muthiah Annamalai; Nikolai Stelmakh; Zachary Dutton; Saikat Guha; Cesar A. Santivanez; Jian Chen; Marcus P. da Silva; Will Kelly; Jeffrey H. Shapiro; Ranjith Nair; Brent J. Yen; Franco N. C. Wong
We demonstrate a balanced-homodyne LADAR receiver employing a phase-sensitive amplifier (PSA) to raise the effective photon detection efficiency (PDE) to nearly 100%. Since typical LADAR receivers suffer from losses in the receive optical train that routinely limit overall PDE to less than 50% thus degrading SNR, PSA can provide significant improvement through amplification with noise figure near 0 dB. Receiver inefficiencies arise from sub-unity quantum efficiency, array fill factors, signal-local oscillator mixing efficiency (in coherent receivers), etc. The quantum-enhanced LADAR receiver described herein is employed in target discrimination scenarios as well as in imaging applications. We present results showing the improvement in detection performance achieved with a PSA, and discuss the performance advantage when compared to the use of a phase-insensitive amplifier, which cannot amplify noiselessly.
Applied Optics | 2007
Tyson L. Lowder; Brian R. Tebbs; Richard H. Selfridge; Stephen M. Schultz; Kevin H. Smith; Thomas D. Monte
Surface-relief fiber Bragg gratings exhibit substantially more polarization dependence than standard fiber Bragg gratings. Using D-fiber with different core orientations, surface-relief gratings are analyzed and fabricated to determine the polarization dependence. We show that the largest Bragg reflection occurs for the polarization state with a dominant TE field component parallel to the flat surface of the fiber. The polarization dependence is adjusted by changing the index of refraction of the surrounding media and by fabricating the surface relief grating using rotated core D-fiber.
Applied Optics | 2005
Kevin H. Smith; Benjamin L. Ipson; Richard H. Selfridge; Stephen M. Schultz
We present a method of replacing a section of the core of a D-shaped optical fiber with sensing materials as a platform for various extrinsic fiber sensors. In this configuration light guides within the sensing material allow for strong interaction between the sensing material and the optical field. Initial experimental results indicate that replacing the fiber core with polymer enhances its temperature sensitivity by at least a factor of 5. The new technique is promising as a means for incorporating various sensing materials into the path of a beam traveling in an optical fiber.
Smart Structures and Materials 2005: Smart Sensor Technology and Measurement Systems | 2005
Kevin H. Smith; Benjamin L. Ipson; Tyson L. Lowder; Aaron R. Hawkins; Richard H. Selfridge; Stephen M. Schultz
We present a new type of fiber Bragg grating (FBG) in which we etch the grating into the flat surface of a D-shaped optical fiber. Instead of being written in the core of the fiber, as are standard FBGs, these surface relief fiber Bragg gratings (SR-FBGs) are placed in the cladding above the core. These gratings are a viable alternative to standard FBGs for sensing applications. In this work we describe the fabrication process for etching Bragg gratings into the surface of D-fibers and demonstrate their performance as temperature sensors. We show that SR-FBGs resist much higher temperatures than standard FBGs by demonstrating their operation up to 1100 degrees Celsius.
Frontiers in Optics | 2003
Kevin H. Smith; Stephen M. Schultz; Richard H. Selfridge; Richard Dyott
This presentation introduces a technique for replacing the core of an optical with a nonlinear polymeric material. This creates a platform that allows for interaction between light guided by an optical fiber and external influences, including electric fields and other controlled or sensed environmental changes.