Page 115 - Tunable Lasers Handbook
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96      Charles Freed

                   numbers for 12C1607, W16O 2’  12C180,,  W18O 2’  W160180, 14C1607. and 14C180,
                   were simultaneousl;  computed from 390 beat frequency measurements between
                   pairs  of  adjacent (0001)-[  1000, 0200],~,, band  C02 laser transitions.  The input
                   data included the 56 beat frequencies measured between  adjacent 12C1601 rota-
                   tional lines by Petersen et a/. [93], and the absolute frequencies of the 10.18ym I-
                   R(30) and 9.33-ym 11-R(10) 12C160, transitions determined by Evenson et al. [94]
                   relative to the primary cesium standard. These initial results for the seven CO,  iso-
                   topic species listed were published by Freed et al. in 1980 [36].
                       In  1983 Petersen et al. published  [99] improved vibrational-rotational con-
                   stants and absolute frequency tables for the regular bands of  12C160,.  These new
                   results obtained at the NBS in Boulder, Colorado, were based on new  beat fre-
                   quency  measurements,  including  high-J  and  across-the-band  center  measure-
                   ments,  and  yielded  about  a  factor  of  10 better  frequency  tables.  In  addition,
                   some specific 13C1602 lines were also measured with reduced uncertainties. The
                   new results of Petersen et a/. [99] yielded a more precise determination of  the
                   absolute frequency  (relative to the primary  cesium standard) of  the  12C160,  I-
                   R(30) line, with an absolute uncertainty of 3.1 kHz. This uncertainty of 3.1 kHz
                   became the principal limit for the uncertainties in  the frequency tables for the
                   absolute  frequencies  of  regular  band  lasing  transitions  in  nine  C02 isotopic
                   species, published by Bradley et al. in 1986 [37]. The data and results published
                   in this paper represented the final phase and outcome of the isotopic CO,  laser
                   frequency-calibration work that had begun at MIT Lincoln Laboratory more than
                   a decade earlier. This final CO,  isotope frequency calibration work represented
                   significant improvement over previous results for the following reasons:

                       1.  We  have  included  in  our  database  the  most  recent  measurements  on
                   13C160,  regular band transitions that Petersen et al. published  [99]; their more
                   precise-measurement  of  the  I-R(30) line  absolute frequency, and the beat  fre-
                   quencies of their widely spaced lines [99] was included in our database as shown
                   in Table 1.
                       2.  We have extended our previous measurements, particularly of  lC1601 to
                   higher  J  values,  and  have  made  the  first  measurements  of  12C170, -  &d
                   13C160180.
                       3.  We have improved our instrumentation and measurement techniques. and
                   thus have been able to measure pressure  shifts in  CO,  laser lines with a more
                   sophisticated  two-channel  line-center-stabilized  calibration  system  (which  is
                   described in the next section).
                       4.  We  have  recognized  deficiencies in  our  earlier  weighting  of  measure-
                   ments, and have become familiar with the use of resistant statistical procedures
                   for minimizing the effects of “outliers.”
                   As a result of the preceding changes, the number of beat frequency measurements
                   has increased to 915, the number of  isotopic species has increased to nine, and
                   the precision of predicted frequencies has increased by an order of magnitude.
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