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Abstract Summary Swept wavelength laser source is currently an essential element for many biomedical and sensing applications especially for Optical Coherence Tomography (OCT). Swept Source OCT (SS-OCT) is fast becoming one of the most successful optical technologies, in the field of disease diagnostics and biomedical imaging. For such applications, the main interest is to have a wide wavelength-tuning range, high speed, miniaturized dimensions and low cost. Miniaturization opens the door to integrate the system on a handheld unit, which may initiate a wide variety of new applications. Various configurations have been proposed for SSOCT utilizing external optical components, which are bulky, expensive and difficult to align. To overcome these challenges, swept sources based on MEMS technology have recently attracted a great attention. The technology provides miniaturized dimensions, low cost and batch processing. In-plane MEMS components suitable for building a complete integrated SS-OCT head have been reported. The main drawback of swept source based on in-plane MEMS filter is the small tuning range (20 nm - 35 nm), which is not suitable for many OCT applications. In this thesis, we present an SOI-MEMS tunable Fabry-Perot filter with 125 nm tuning range and a free-spectral range (FSR) larger than 130 nm. The SOI-MEMS filter is based on two-silicon-layers Bragg mirrors etched with an 80 μm depth. The SOI-MEMS filter is then used to construct a 100 nm tuning range swept laser source. The tuning of the filter is carried out using a MEMS electrostatic comb-drive actuator attached to the free- Bragg mirror of the filter, in a lithographically self-aligned manner. The presented results represent, to the best of our knowledge, the largest tuning range reported in literature for an in-plane MEMS-based swept laser source. For the swept source applications rapid filter tuning speed that may exceed 100 kHz is required to achieve high image acquisition rate. The swept laser for these high speed applications is usually a multimode laser with average spectral width around 0.1 nm. A narrow swept laser spectral width/linewidth is required to achieve a large penetration depth in the sample that may exceed several millimeters. The spectral width of such sources is affected by the filter scanning speed, its 3dB spectral width, the SOA gain and its wavelengths dependence, the cavity loss and many other parameters. Conventionally the instantaneous spectral width at these high speeds cannot be accessed by direct measurement. Instead indirect estimation for the average spectral width at a certain speed is done using the Fourier transform of a measured coherence function. Few previous trials for modeling the swept source have been proposed based on time domain propagation equations governing the gain dynamics and the complex electric-field envelope to describe the swept laser behavior. This time domain approach did not include the wavelength dependence of the SOA gain. The previous modeling trials did not give much insight on the swept laser instantaneous spectral width with its multi-folded nature. In this thesis we also present a new technique to model the swept source operation and predict the instantaneous spectral width using a multimode rate equation approach. The model successfully estimates the reported spectral width narrowing at static positions with respect to the filter 3dB spectral width and how this effect is reduced as the filter scanning speed is increased. It allows predicting for the first time, to our knowledge, the effect of the gain spectrum on the instantaneous spectral width at different scanning speeds. The effects of filter 3-dB spectral width, the cavity loss, the pumping current and the loop length are also studied. In addition the model allows monitoring the evolution of different modes as the filter is scanned in time domain. 11 The work in this thesis is presented as follows: In Chapter 1, an introduction about swept laser source, the main research topics of the thesis and the thesis outline are presented. Chapter 2, we present a comprehensive overview on swept laser sources, basic configuration, operation principle, its main specifications, configurations and implementation techniques. Chapter 3 presents a novel multimode rate equation numerical model for the swept laser, practical technique for extracting the SOA parameters is provided, Modified multimode rate equation for the swept laser is derived and the different factors affecting the swept laser instantaneous spectral width are studied in detail. Chapter 4 is devoted to the deeply-etched optical MEMS tunable filter for SS-OCT applications where the Bragg mirrors and multilayer filter designs are discussed. An overview on the SOI technology and Deep Reactive Ion Etching (DRIE) is presented, the deeply etched structures fabrication steps are explained in details, the fabricated structures SEM photos are included and process achievements are summarized. The optical characterization of the deeply etched components and MEMS based swept laser is presented. The reflection response of the multilayer mirror is measured and its reflectivity is estimated. The effect of etching error on the reflection response is determined. The MEMS filter is optically characterized showing its tuning range, insertion loss and 3dB bandwidth. Chapter 5 MEMS based swept laser is constructed and characterized demonstrating the large improvement in tuning range and the factors affecting it. Practical technique for SOA parameter extraction is provided and its effect on the MEMS swept laser tuning range is presented. In Chapter 6 the final conclusions of the thesis are stated, a comparison with previous published work is provided and future work is discussed. |