Page 222 - High Power Laser Handbook
P. 222

190   So l i d - S t at e   La s e r s                   Zigzag Slab Lasers    191


                                  t/2       Parameter    Factor Change
                                            Thickness, t      1          1/2
                      t
                                            Height, h         1          2
                                            Heat density, Q   1          1
                  h             2h          ∆T                1          1/4
                                            Index change, ∆n    1        1/4
                                            Focal length      1           1
                                            Stress, σ         1          1/4
                                            Gain, g  0        1          1
                 Figure 8.5  The table highlights the advantages of aspect-ratio scaling of a slab.




                      offers two degrees of freedom when it comes to slab sizing. By mak-
                      ing a slab taller and thinner, its center-to-edge temperature difference
                      ∆T and the stresses can be reduced, enabling the slab to scale to higher
                      powers. Figure 8.5 shows a comparison of two slabs with the same
                      area  and  overall  output  power.  The  first  one  has  a  cross-sectional
                      aspect ratio of 2:1, while the second one is a factor of 2 thinner and
                      taller with an aspect ratio of 8:1. According to equations in Figs. 8.3
                      and 8.4, both ∆T and the stress decrease by a factor of 4, enabling a
                      factor of 4 scaling in power.
                         Aspect-ratio  scaling  also  has  limitations.  For  traditional  side-
                      pumped slabs, as the slab becomes taller and thinner, pump absorp-
                      tion efficiency begins to suffer. In addition, losses due to diffraction
                      within the slab become a factor that limits the length of the slab, and
                      maintaining  fabrication  tolerances  on  TIR  surface  figures  becomes
                      increasingly more difficult. Finally, for crystalline slabs, there may be
                      growth limits on the height of the slab. A brief discussion for each of
                      these limitations follows.

                      Pump Absorption
                      Pump  absorption  efficiency  for  traditional  side-pumped  thin
                      slabs is an issue primarily for Nd:YAG, because the Nd-doping
                      concentrations are limited to ~1 percent. Higher concentrations of
                      Nd in YAG result in low-optical-quality crystals and a rapid deg-
                      radation in the fluorescence lifetime. For diode arrays centered
                      on the 807-nm absorption band of Nd:YAG with a bandwidth of
                      ~4 nm, the required slab thickness for greater than 80 percent absorp-
                      tion efficiency is ~6 mm. This efficiency follows Beer’s law and
                      degrades for thinner slabs. To overcome this problem, alternate
                      edge-pumping  and  end-pumping  techniques  have  been  devel-
                      oped  (discussed  later  in  this  section)  that  provide  much  longer
                      absorption distances.
   217   218   219   220   221   222   223   224   225   226   227