Page 82 - High Power Laser Handbook
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52    G a s , C h e m i c a l , a n d F r e e - E l e c t r o n L a s e r s                                                          Chemical Lasers     53


                         28
                         24
                         20
                        Amplitude (a.u.)  16                            v = 1 --> 0

                                                                        v = 2 --> 1
                         12

                          4 8
                          0
                           2.5    2.6   2.7    2.8   2.9    3.0    3.1
                                          Wavelength (µm)
                      Figure 3.5  Typical lasing spectrum of HF continuous wave (CW) lasers.




                         20
                         18
                         16
                        Amplitude (a.u.)  12 8                          v = 1 --> 0
                         14
                         10
                                                                        v = 2 --> 1
                                                                        v = 3 --> 2
                          4 6
                          2
                          0
                           3.5    3.6   3.7    3.8    3.9   4.0    4.1
                                          Wavelength (µm)
                      Figure 3.6  Typical lasing spectrum of DF CW lasers.



                             g  = upper-level degeneracy factor
                              U
                              g = lower-level degeneracy factor
                               L
                              λ   = laser wavelength
                           t    = upper-state spontaneous lifetime
                            spont
                            g(ν) = normalized line shape
                      Limiting the discussion specifically to HF, we first consider the term
                      in brackets and the transition (v + 1, J – 1) → (v, J). N  can be expressed
                                                                U
                      as the product of the total HF number density N and the fraction of
                      these molecules in the v + 1 and J – 1 states.
                         One assumption that is frequently satisfied in the absence of las-
                      ing, and that is approximately satisfied during lasing, is that the rota-
                      tional levels are in thermal equilibrium with an absolute temperature T
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