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228    Cha pte r  Ni ne


                     1.0









                   Bulk absorption coefficient (cm –1 )  0.01
                     0.1




















                    0.001
                             4 µm           5 µm      6 µm   7 µm
                          2500           2000           1500     1200
                                                   –1
                                      Wave number (cm )
              FIGURE 9.12  Infrared absorption coeffi cient for AMI vacuum fl oat zoned
              silicon as a function of wavelength.


              laser emitting at 2.94 µm. No measurable absorption for the 12-cm
              crystal was observed. No damage resulted from the intense radiation
                                    2
              estimated to be 4 MW/cm  after 10 min of irradiation. Results show
              high-purity single-crystal silicon was suitable for use with high-
              intensity NIR lasers pulsed or CW.


        9.6  Single-Crystal Silicon Fibers
              There was great interest in developing flexible infrared fibers to be
              used with these high-intensity lasers. Silica fibers were extremely
              low in absorption in the visible region, but because of water absorp-
              tion cut off before 2 µm. Attention shifted to fluoride glasses with
              some success. Polycrystalline materials were extruded but suf-
              fered from light scatter and breakage at grain boundaries when bent.
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