while operating within the limiting ratio is more challenging. In such cases, a
higher coefficient of thermal expansion difference and, hence, higher birefrin-
gence can be achieved by adjusting the composition of stress members so they are
similar to those used for gyroscope fibers. Indeed a broad range of ytterbium-
doped LMA DCFs, whose characteristics are optimized for various output
powers, are now commercially available [33]. An optical image showing the
cross-section of such a fiber, with a 20-mm core and 400-mm inner-cladding
diameter and a birefringence exceeding 3:5 10
4
, is presented in Fig. 22.2.
22.5 FIBER LASERS: STATE OF THE ART
LMA fibers with core diameters of 20–30 mm and NAs of around 0.06 have
become the industry standard for