Page 80 - High Power Laser Handbook
P. 80

50    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     51


                                                         HF          DF
                       ω      vibrational level linear term  4138.73  3000.358
                       X      first anharmonicity correction   –90.05  –47.34
                       B J    rotational constant          20.96       11.00
                       B 1J   rotational constant first    –0.7958     –0.2936
                              correction
                      Table 3.2  HF and DF Energy Level Parameters. All Values are in
                      Wavenumbers
                         The first term in Eq. (3.5) corresponds to the behavior of a simple
                      harmonic oscillator with quantum number v. Allowable values for
                      v are 0, 1, 2, . . . . The second term corresponds to a first-order anhar-
                      monic  correction  illustrating  deviation  from  ideal  harmonic
                      behavior. The third term is associated with the rotational quantum
                      number J and the associated rigid-rotor rotational energy. Allow-
                      able values for J are 0, 1, 2, . . . . The fourth term is the Coriolis
                      effect  correction  to  the  rotational  energy.  More  sophisticated
                      expressions,  including  16  terms  or  more,  are  also  available.  The
                      interested reader can find a more detailed discussion of diatomic
                                                                               8
                      energy  levels  and  spectroscopy  in  Spectra  of  Diatomic  Molecules,
                      which  also  provides  general  information  on  diatomic  molecule
                      energy-level notation.
                         It should be noted that diatomic molecules containing hydrogen
                      are atypical as compared with most single-bond diatomics. The for-
                      mer  have  rather  large  vibrational  level  separations,  substantial
                      amounts of anharmonicity, and very large rotational constants. This
                      last feature is a major advantage from a laser standpoint.
                         The allowed molecular transitions for HF and DF are:

                                             ∆ν = +/–1                     (3.6a)

                                             ∆  J = +/–1                   (3.6b)

                      Moreover, the degeneracy of the E(v, J) level is 2J + 1.
                         In terms of energy levels, the primary allowed transitions are:

                          E(ν, J – 1) → E[(ν – 1), J], which is denoted as a P branch.
                          E(ν, J + 1) → E[(ν – 1), J], which is denoted as an R branch.

                      The P branch is the dominant lasing transition due to higher gain (see
                      Sec. 3.3.2). Figure 3.4 shows energy-level diagrams appropriate for
                      HF and DF lasers (note that vibrational levels are denoted by V as
                      opposed to ν).
   75   76   77   78   79   80   81   82   83   84   85