16 research outputs found

    Phase-sensitive amplification of 11 WDM channels across bandwidth of 8 nm in a fibre optic parametric amplifier

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    We experimentally demonstrate phase-sensitive fibre optic parametric amplification with gain >10dB and optical noise figure below 3dB for 11 channels spaced of 100 GHz. We employ all-fibre dispersion management to achieve a wideband phase-matching between signals and their copies

    Phase-sensitive amplification of 11 WDM channels across bandwidth of 8 nm in a fibre optic parametric amplifier

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    We experimentally demonstrate phase-sensitive fibre optic parametric amplification with gain >10dB and optical noise figure below 3dB for 11 channels spaced of 100 GHz. We employ all-fibre dispersion management to achieve a wideband phase-matching between signals and their copies

    Propagation properties of duobinary transmission in optical fibers

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    Thesis (M. Eng.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science; and, Thesis (B.S.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 1998.Includes bibliographical references (leaves 121-126).by Leaf Alden Jiang.B.S.M.Eng

    Advances in Optical Amplifiers

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    Optical amplifiers play a central role in all categories of fibre communications systems and networks. By compensating for the losses exerted by the transmission medium and the components through which the signals pass, they reduce the need for expensive and slow optical-electrical-optical conversion. The photonic gain media, which are normally based on glass- or semiconductor-based waveguides, can amplify many high speed wavelength division multiplexed channels simultaneously. Recent research has also concentrated on wavelength conversion, switching, demultiplexing in the time domain and other enhanced functions. Advances in Optical Amplifiers presents up to date results on amplifier performance, along with explanations of their relevance, from leading researchers in the field. Its chapters cover amplifiers based on rare earth doped fibres and waveguides, stimulated Raman scattering, nonlinear parametric processes and semiconductor media. Wavelength conversion and other enhanced signal processing functions are also considered in depth. This book is targeted at research, development and design engineers from teams in manufacturing industry, academia and telecommunications service operators

    Spectral LADAR: Active Range-Resolved Imaging Spectroscopy

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    Imaging spectroscopy using ambient or thermally generated optical sources is a well developed technique for capturing two dimensional images with high per-pixel spectral resolution. The per-pixel spectral data is often a sufficient sampling of a material's backscatter spectrum to infer chemical properties of the constituent material to aid in substance identification. Separately, conventional LADAR sensors use quasi-monochromatic laser radiation to create three dimensional images of objects at high angular resolution, compared to RADAR. Advances in dispersion engineered photonic crystal fibers in recent years have made high spectral radiance optical supercontinuum sources practical, enabling this study of Spectral LADAR, a continuous polychromatic spectrum augmentation of conventional LADAR. This imaging concept, which combines multi-spectral and 3D sensing at a physical level, is demonstrated with 25 independent and parallel LADAR channels and generates point cloud images with three spatial dimensions and one spectral dimension. The independence of spectral bands is a key characteristic of Spectral LADAR. Each spectral band maintains a separate time waveform record, from which target parameters are estimated. Accordingly, the spectrum computed for each backscatter reflection is independently and unambiguously range unmixed from multiple target reflections that may arise from transmission of a single panchromatic pulse. This dissertation presents the theoretical background of Spectral LADAR, a shortwave infrared laboratory demonstrator system constructed as a proof-of-concept prototype, and the experimental results obtained by the prototype when imaging scenes at stand off ranges of 45 meters. The resultant point cloud voxels are spectrally classified into a number of material categories which enhances object and feature recognition. Experimental results demonstrate the physical level combination of active backscatter spectroscopy and range resolved sensing to produce images with a level of complexity, detail, and accuracy that is not obtainable with data-level registration and fusion of conventional imaging spectroscopy and LADAR. The capabilities of Spectral LADAR are expected to be useful in a range of applications, such as biomedical imaging and agriculture, but particularly when applied as a sensor in unmanned ground vehicle navigation. Applications to autonomous mobile robotics are the principal motivators of this study, and are specifically addressed

    Novel configurations for pulsed optical parametric oscillators and their pump sources

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    The development of all-solid-state, diode-laser pumped neodymium (Nd) lasers and optical parametric oscillators (OPOs) is described, which realise practical sources of coherent radiation with a high degree of frequency agility, are efficient, reliable and potentially compact. A comparison of various neodymium doped host materials reveals yttrium lithium fluoride (YLF) to be an appropriate replacement for the more widely known host yttrium aluminium garnet (YAG) in diode-laser pumped devices. The development of an end-pumped Nd:YLF laser that utilises a 12-mJ, 60W, quasi-CW diode-laser bar is initially described. Multilongitudinal-mode, TEM00 pulse energies of greater than 2 mJ have been observed, with corresponding peak output powers in excess of 118 kW. The incorporation of a novel pre-lase Q-switching technique has realised single-longitudinal-mode peak powers in excess of 90 kW continuing to be achieved. Further, the development of a more powerful end- pumped Nd:YLF laser utilising 2, 3-bar diode-laser arrays, each providing 72-mJ of pump energy is described. In this case, Q-switched, multilongitudinal-mode, TEM00 pulse energies of greater than 11 mJ are reported, with the clear potential for increasing this to greater than 20 mJ, based on measured fixed-Q pulse energies of greater than 30 mJ. Complementing the development of these diode-laser pumped solid-state lasers is the development of optical parametric oscillators based on the nonlinear materials lithium triborate (LBO) and beta-barium borate (?-BBO). Pumped by the frequency up-converted (third harmonic) output of the mid laser, such optical parametric oscillators introduce extensive frequency agility spanning a spectral range from the deep blue (0.4 mum) to the mid-infrared (2.5 mum). Initially, the development of an LBO based device is reported, which in a type I critical phase- match (CPM) geometry has a measured oscillation threshold of 5 mJ, but through the introduction of interferometric, dispersive and injection seeding techniques made to operate on a single axial mode. Near transform limited linewidths are reported in devices which continue to have modest pump thresholds and broad tunability. The parametric generation of broad spectral bandwidths (polychromatic) by the use of suitable phase-matching geometries is also reported. Greater than 100 nm simultaneous bandwidth in the visible spectrum is generated in a collimated signal-wave from a novel, noncollinear phase-matching geometry in a beta-BBO optical parametric oscillator, which is pumped by the collimated output of frequency tripled diode-laser pumped Nd:YAG laser. The device is demonstrated to be efficient, having a similar pump threshold and efficiency to that of the well known collinear phase-matched tunable device, and to continue to encompass a degree of tunability allowing the large simultaneous bandwidth to be tuned across the entire visible spectrum. Dispersive cavity tuning of the optical parametric oscillator by the use of a Littrow-mounted grating or acousto-optic tuning filter, with a static crystal and pump configuration, is also described
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