By Adarsh Deepak
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Spectrosc. 278-310 (1975). 55, CALCULATION OF VIBRATION-ROTATION ENERGY LEVELS 23 5. , Mol. Phys. 32, 499-521 (1976). 6. , J. 33, 741-747 (1972). Phys. 7. , Spectrochim. 1711-1715 (1973). 29Ά, 8. , J. Mol. Spectrosc. 65, 219-228 (1977). 9. , and Toth, R. , J. Mol. Spectrosc. 67, 117-131 (1977). 10. Toth, R. , J. Mol. Spectrosc. 67, 185-205 (1977). 11. , and Toth, R. , J. Mol. Spectrosc. 70, 361-373 (1978). 12. S. O. 11443 (1975). 13. , Mol. Phys. 33, 1641-1650 (1977). 14. Toth, R. , J. Mol. Spectrosc.
1 cm"1 and strengths accurate to 15%. 1 cm -1 , that would be considered very satisfactory. Such applications include radiance transfer calculations, broad-band transmission, and wideband remote sounding. As a general matter, however, the results of Flaud and Camy-Peyret are not only impressive, they are essential. For laser propagation, hot through cold calculations, accurate intensities associated with interacting levels and so on, it is imperative that we have the eigenvalues, eigenvectors, and transition moments in order to properly proceed with the study of water.
6). 1! + 760 mm N„ T - 296. -io-sV-sV-iff-Jo'-lff-lo'-l·* è WPVENUMBER i ΆΆΆΆΆΆΆ 1 (CH-ll FIGURE 11. Attenuation coefficient vapor including modified continuum (Eq. for air-broadened 49). water FREQUENCY (GHZ) -2,40 Q HRVENUMBER 24£ (CM-1 ) FIGURE 12. Attenuation coefficient divided by term for air-broadened water vapor including modified (Eg. 49) . radiation continuum S. A. CLOUGH ET AL 46 2. Huber, D. L. , and Van Vleck, J. , Rev. 187 (1966). 3. , Phys. 4. Futrelle, R. , Phys. Rev. 5. , J. (1970).
Atmospheric Water Vapor by Adarsh Deepak