Page 165 - Tunable Lasers Handbook
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144     Charles Freed

                   1 1.  SMALL-SIGNAL GAIN AND SATURATION INTENSITY OF  REGULAR
                   BAND LASING TRANSITIONS  IN SEALED-OFF CO, ISOTOPE LASERS

                       The stability and most other operational characteristics of rare CO,  isotope
                   lasers are generally similar to the commonly used  12C160,  lasers. However, the
                   small-signal gain coefficient a.  and saturation intensity I, of the rare CO,  lasing
                   transitions can be significantly different from corresponding lines of  1Xi60,.  It
                   can be shown that the power output of a laser may be approximated [I211 by


                                        6 =21,Ar, ( __- 1) ,
                                                  I, + t,.
                   where I, is the internal cavity loss per pass, l, is the transmittance of the output
                   mirror, and L  and A  are the length and effective cross-section area of  the gain
                   medium,  respectively. Equation  ( 19) clearly  shows  that  the  small-signal  gain
                   coefficient a.  and  saturation  intensity I,  are  the  two  salient parameters  to  be
                   measured in order to optimize a laser design for a desired output power Po.
                       The  measured  values  of  small-signal  gain  coefficient  a.  and  saturation
                   intensity I, will, to  a very  large degree, depend on  a number  of  experimental
                   parameters,  such  as  excitation  currents,  gas  pressures,  mixtures  and  mixing
                   ratios,  wall temperatures.  and discharge tube diameters. CO,  dissociation  and
                   recombination rates and impurity buildup will also critically affect both an and
                   Z,,  and thus  output  power  and  CO,  laser  lifetime.  Recirculating  gas  flow  can
                   lead to very large increases of  the small-signal gain coefficient and saturation
                   intensity  by  a  complex  combination  of  effects  involving not  only  convective
                   cooling,  but  also  better  control  of  CO,  dissociation  and  recombination  rates
                   and  impurity  cleanup  by  means  of  appropriately  chosen  catalytic  converters.
                   Clearly. any meaningful measurement of small-signal gain and saturation inten-
                   sity in a CO,  amplifier should be accompanied by a detailed description of the
                   experimental  method  and  associated  parameters.  Note  that  the  gas-discharge
                   scaling laws and other results described by Abrams and Bridges  [122] may be
                   of great value in extrapolation from a given set of data.
                       Effects due to Fermi resonance play  a major role in determining the very
                   significant variations in gain for the I and I1 bands in the various CO,  isotopes.
                   This was both theoretically and experimentally demonstrated for the first time by
                   Silver et al. E1231  in  1970. To show the effect of  Fermi resonance on the laser
                   gain, it is only necessary to form the gain ratio of  the transitions. Silver et al.
                   used  the  gains measured  for  the  WlgO,,  QC1602, and  13C1602 I and 11 band
                   P(20) transitions to obtain their results. The ratios of gain and absorption coeffi-
                   cients depend directly on the matrix element ratio. which they calculated from
                   the vibrational state wave functions. Thus, the ratio of  gain was given [123] as
                   g(OOOl-I)/g(OOO1-II)  = K(OOO1-I)  /K(OOOl-11)  where K denoted the J-indepen-
                   dent portion  of  the matrix  element ratio  inferred from gain and loss measure-
                   ments. The final result obtained for the matrix element ratio was [ 1231:
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