Page 218 - Optical Communications Essentials
P. 218

Wavelength Division Multiplexing



          208  Chapter Twelve


                        L-band 4-THz-wide spectral chunks into the same 40 output fibers. The free spectral
                        range ∆λ FSR is determined from the relationship
                                                                 2
                                                               λ c
                                                FSR   ∆λ FSR                             (12.3)
                                                              ∆Ln eff
                        For example, for the 4-THz frequency range denoted here, the center wavelength λ c is
                        1550.5nm, the free spectral range ∆λ FSR should be at least 32.2nm in order to separate
                        all the wavelengths into distinct fibers, and the effective refractive index n eff is nomin-
                        ally 1.45 in silica. Then the length difference between adjacent array waveguides is
                        ∆L   51.49µm.


                        The passband shape of the AWG filter versus wavelength can be altered by the
                      design of the input and output slab waveguides. Two common passband shapes
                      are shown in Fig. 12.7. On the left is the normal or gaussian passband. This
                      passband shape exhibits the lowest loss at the peak, but the fact that it rolls off
                      quickly on either side of the peak means that it requires a high stabilization of
                      the laser wavelength. Furthermore, for applications where the light passes
                      through several AWGs, the accumulative effect of the filtering function reduces
                      the passband to an extremely small value. An alternative to the gaussian pass-
                      band shape is the flattop or wideband shape, as shown on the right in Fig. 12.7.
                      This wideband device has a uniform insertion loss across the passband and is
                      therefore not as sensitive to laser drift or the sensitivity of cascaded filters as is
                      the gaussian passband. However, the loss in a flattop device is usually 2 to 3dB
                      higher than that in a gaussian AWG. Table 12.3 compares the main operating
                      characteristics of these two designs for a typical 40-channel AWG.


          12.2.4. Diffraction gratings
                      A fourth DWDM technology is based on diffraction gratings. A diffraction grat-
                      ing is a conventional optical device that spatially separates the different wave-
                      lengths contained in a beam of light. The device consists of a set of diffracting


                              Normal or                Flattop or
                             Gaussian AWG            wideband AWG

                                      Rolloff
                       Insertion loss  Passband  Insertion loss  Passband








                             Wavelength                Wavelength
                      Figure 12.7. Two common optical-filter passband shapes: nor-
                      mal or gaussian and flattop or wideband.


                 Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com)
                            Copyright © 2004 The McGraw-Hill Companies. All rights reserved.
                              Any use is subject to the Terms of Use as given at the website.
   213   214   215   216   217   218   219   220   221   222   223