Page 409 - Fiber Bragg Gratings
P. 409

386                         Chapter 8 Fiber Grating Lasers and Amplifiers

        well as the management of dispersion. The fiber amplifier has enabled
        undersea transmission over thousands of kilometers. With the increasing
        demand for bandwidth, wavelength division multiplexing (WDM) of opti-
        cal channels is seen to be a viable solution for increasing transmission
        capacity at a given transmission rate, in point-to-point routes [120],
            The important issues in amplified transmission systems for WDM
        applications are the available gain, the gain uniformity across the band-
        width of an amplifier, the robustness to transient switching of WDM
        channels in single and cascaded amplifier chains, and the overall noise
        figure. The gain spectrum and upper-state lifetimes of an erbium-doped
        fiber amplifier vary as a function of the core dopants. High-germanium
        erbium-doped fibers have a highly nonuniform gain with a bandwidth of
        —35 nm from 1530 to 1565 nm, peaking at approximately 1535 nm. The
        use of aluminum reduces the nonuniformity, making the gain spectrum
        flatter, while ytterbium as a codopant with erbium allows an efficient
        transfer of energy from the available high-power diode pumps at 980 nm
        (a wavelength at which erbium suffers from excited-state absorption,
        reducing efficiency) to the required transition in the 1550-nm wavelength
        region for amplification. The latter shifts the gain peak to >1540 nm,
        while narrowing the gain bandwidth. Along with the nonuniformity in
        the gain, the doped fiber amplifier is homogeneously broadened. While
        allowing amplification across the wide gain bandwidth, the gain available
        at any wavelength is dependent on the simultaneous presence or absence
        of other wavelength channels; thus, gain may be depleted from a saturat-
        ing signal from an existing channel as another channel is switched on.
        As the gain in a single amplifier fluctuates, the problem is exacerbated
        with a chain of cascaded amplifiers, leading to severe cross-talk. Nonuni-
        form gain across the bandwidth of the amplifier produces a wavelength-
        dependent low-frequency cross-talk penalty. Apart from the signal degra-
        dation, severe damage to components is a possibility because spiking with
        intermittent interruption and resumption of transmission. The inversion
        and thus the gain is also pump-power dependent, leading to gain changes
        as the pump source ages. For analog transmission systems the problem
        is worse, because the local gain slope leads to harmonic distortion, degrad-
        ing the received signal. Schemes have been developed to stabilize the
        gain of fiber amplifiers as well as flatten the gain variation over a wide
        bandwidth. Fiber gratings offer simple solutions to solve both these prob-
        lems. In the following sections, we look at a specific example of gain
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