Page 166 - An Introduction to Microelectromechanical Systems Engineering
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Fiber-Optic Communication Devices                                             145

                               Partially
                               reflective   Nonreflective
                               facet        facet            Reflective mirror
                    Auxiliary output  Laser diode  Collimating lens
                    (front facet)  (gain medium)
                                                              First diffractive order
                                                                             Output (back facet)
                                                                   θ
                                                     Incident beam
                                  Thermoelectric
                                 cooler
                                                                    Grating
                                   Pivot point          (a)












                                                       θ 1
                                                         θ 2





                                                        (b)
                  Figure 5.8  (a) Illustration of the Littman-Metcalf external cavity laser configuration. Light from
                  the laser diode is collimated and diffracted by a grating acting as a wavelength filter. Lasing occurs
                  only at one wavelength, whose diffraction order is reflected by the mirror back into the cavity. (b)
                  Rotating the mirror around a virtual pivot point changes the wavelength and tunes the laser.




                  collimating lens, then diffracts on the grating. The mirror reflects back into the cav-
                  ity and the gain medium only one wavelength whose diffracted beam is exactly per-
                  pendicular to the mirror. This wavelength (and corresponding diffraction angle θ)
                  depends strictly on the grating pitch as well as the relative angle of the mirror with
                  the diffraction grating. In actuality, because the diffraction grating has finite disper-
                  sion [16], the linewidth of the reflected wavelength is broadened to a few picome-
                  ters. The output of the laser is typically the main (undiffracted) order reflecting from
                  the grating, but an auxiliary output can be taken from the partially reflective facet of
                  the laser diode.
                      The Littman-Metcalf configuration utilizes a fixed grating but rotates the reflec-
                  tive mirror to tune the laser to a different wavelength [Figure 5.8(b)]. It is the rota-
                  tion of the mirror that achieves both tuning operations simultaneously: it selects a
                  different diffracted wavelength from the grating, and it modulates the physical
                  length of the cavity. By appropriately selecting a virtual pivot point [17], the dimen-
                  sional change of the cavity length can be such that an integral number of new half
                  wavelengths can fit within the cavity—note that a rotation about a virtual pivot
                  point is geometrically equivalent to a rotation about a real pivot point and a linear
                  translation. A poor choice of pivot point or misalignment can cause serious
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