Page 39 - Fiber Bragg Gratings
P. 39

20         Chapter 2 Photosensitivity and Photosensitization of Optical Fibers

        both indirectly, e.g., by etching glass exposed to radiation or using second-
        harmonic generation [9,26,27] as a probe, and directly, e.g., by measure-
        ment of photocurrent in germania-doped planar waveguides [28] and
        across thin films of bulk glass [29].
            It has been concluded that the photocurrent is influenced by the
        fluence of the exciting UV radiation; the photocurrent (probably by tunnel-
        ing [29]) is a linear function of the power density for CW excitation [28],
        while for pulsed, high-intensity radiation, it takes on a two-photon excita-
        tion characteristic [29].
            The paramagnetic defects of the Ge(/i) type including the E' center
        are detected by ESR. The GeE' has an associated optical absorption at
        4.6 eV [30].



        2.4 Photosensitization techniques

        A question often asked is: Which is the best fiber to use for the fabrication
        of most gratings? Undoubtedly, the preferred answer to this question
        should be standard telecommunications fiber. Although techniques have
        been found to write strong gratings in this type of fiber, there are several
        reasons why standard fiber is not the best choice for a number of applica-
        tions. Ideally, a compatibility with standard fiber is desirable, but the
        design of different devices requires a variety of fibers. This does open the
        possibility of exploiting various techniques for fabrication and sensitiza-
        tion. Here we look in some detail at the behavior of commonly used species
        in optical fiber and present their properties, which may influence the type
        of application. For example, the time or intensity of UV exposure required
        for the writing of gratings affects the transmission and reliability proper-
        ties. This results in either damage (Type II gratings) [31] or the formation
        of Type I, at low fluence, and Type IIA gratings [32], each of which have
        different characteristics (see Section 2.4.1).
            The use of boron and tin as a codopant in germanosilicate fibers, hot
        hydrogenation and cold, high-pressure hydrogenation, and flame-assisted
        low-pressure hydrogenation ("flame-brushing") are well-established pho-
        tosensitization methods. The type of the fiber often dictates what type of
        grating may be fabricated, since the outcome depends on the dopants.
            The literature available on the subjects of photosensitivity, the com-
        plex nature of defects, and the dynamics of growth of gratings is vast
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