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uid 343

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This species has a counterpart in the theoretical library

Transitions

Frequency
[wavenumbers]
Wavelength
[microns]
Integrated cross-section
[km/mol]
3060 3.268 120.4
1930 5.18 5.779
1920 5.209 1.926
1789 5.589 4.816
1728 5.786 0.9632
1665 6.005 0.9632
1593 6.277 2.89
1479 6.762 7.826
1444 6.925 18.06
1435 6.97 1.926
1414 7.075 19.26
1321 7.572 6.622
1267 7.893 0.9632
1205 8.299 0.9632
1192 8.391 8.428
1184 8.447 1.926
1152 8.678 1.926
1107 9.034 3.853
1083 9.232 1.926
1038 9.636 3.853
1006 9.938 0.9632
964.6 10.37 0.9632
949.3 10.53 1.926
898.2 11.13 2.89
848.8 11.78 0.9632
842.9 11.86 13.24
830.1 12.05 49.36
771.1 12.97 14.45
748.2 13.37 96.32
711.8 14.05 17.46
645.9 15.48 1.926
570.6 17.53 6.622
554.5 18.03 4.816

Laboratory Spectrum

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This spectrum was measured using the matrix isolation technique. Samples are prepared by co-deposition of the PAH in the gaseous state with an overabundance of argon onto a cold CsI window suspended in a high vacuum chamber (p ~ 10-8 mtorr). The CsI window temperature is held between 10 and 15 K for the duration of the experiment. The infrared spectrum of the cold CsI window is recorded prior to (I0) and immediately after sample deposition (In). The absorbance spectrum for a neutral, matrix isolated PAH is log(In/I0).

By irradiating this matrix with ultraviolet radiation from a microwave powered hydrogen discharge lamp produces ionized PAHs. The infrared spectrum is again measured (Ii), now having absorption bands due to both the neutral and ionized PAH. This absorbance spectrum (log (I/Ii)) is compared with that of the neutral PAH. Most of the new bands produced by ultraviolet irradiation are due to the ionized form of the PAH. See the provided reference for the specific details regarding the data presented here. In some cases a few bands near 1600 cm-1 may be due to H2O.

Note(s):


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84 species present in version 3.10 of the experimental database (Apr 13, 2023)