Page 160 - Optical Communications Essentials
P. 160

Passive Optical Components



          150  Chapter Nine


                        MZI Equation To have input signals at wavelengths λ 1 and λ 2 that enter ports 1 and 2,
                        respectively, emerge from only one output port, the length difference in the interfer-
                        ometer arms should be

                                                     1  1    −1  c
                                           ∆L =  2 n eff    −     =                   (9.7)
                                                     λ 1  λ     2 n eff  ∆ν
                                                           2
                        where n eff is the effective refractive index of the MZI material and ∆ν is the frequency
                        separation of the two wavelengths.

                        Example Assume that the input wavelengths of a 2   2 silicon MZI are separated by
                        100GHz (or equivalently, 0.75nm at 1550nm). With n eff   1.5 in a silicon waveguide,
                        we know from Eq. (9.7) that the waveguide length difference must be

                                                         8
                                                    3    10 m/s
                                              ∆L =             = 1 mm
                                                           11
                                                   21 5  ( .  )  10 /s
                                                                                            n
                      By using basic 2   2 MZI modules, any size N   N multiplexers (with N   2 )
                      can be constructed.

          9.2. Isolators and Circulators
                      In a number of applications it is desirable to have a passive optical device that
                      is nonreciprocal; that is, it works differently when its inputs and outputs are
                      reversed. Two examples of such a device are isolators and circulators. To under-
                      stand the operation of these devices, we need to recall some facts about polar-
                      ization and polarization-sensitive components from Chap. 3.

                      ■ Light can be represented as a combination of a parallel vibration and a per-
                       pendicular vibration, which are called the two orthogonal plane polarization
                       states of a light wave.
                      ■ A polarizer is a material or device that transmits only one polarization com-
                       ponent and blocks the other.
                      ■ A Faraday rotator is a device that rotates the state of polarization (SOP) of
                       light passing through it by a specific angular amount.
                      ■ A device made from birefringent materials (called a walk-off polarizer) splits
                       the light signal entering it into two orthogonally (perpendicularly) polarized
                       beams, which then follow different paths through the material.
                      ■ A half-wave plate rotates the SOP of a lightwave by 90°; for example, it converts
                       right circularly polarized light to left circularly polarized light.


          9.2.1. Optical isolators
                      Optical isolators are devices that allow light to pass through them in only one
                      direction. This is important in a number of instances to prevent scattered or


                 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.
   155   156   157   158   159   160   161   162   163   164   165