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uid 542

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This species has a counterpart in the theoretical database.

Transitions

νk
[cm-1]
λ
[μm]
int
[km/mol]
4903 2.04 8.85e+3
3165 3.159 62.1
2950 3.389 166
2814 3.554 100
2798 3.574 144
2777 3.601 199
2678 3.734 140
2666 3.752 103
2639 3.789 13.8
2615 3.824 120
2577 3.88 38
2567 3.895 44
1585 6.31 56.9
1571 6.367 74.3
1556 6.429 292
1530 6.536 49.1
1508 6.63 369
1466 6.821 316
1415 7.067 252
1402 7.135 24.3
1383 7.23 26.7
1370 7.298 545
1365 7.325 909
1357 7.37 898
1330 7.52 677
1309 7.639 3.03e+3
1198 8.347 31.2
1193 8.384 52.4
1183 8.454 622
1164 8.59 15.8
1036 9.649 92.4
997.1 10.03 13.2
923.4 10.83 40.1
879.5 11.37 21.9
820.7 12.18 18.2
797.3 12.54 63.7
765.8 13.06 34.8
760.8 13.14 24
751.3 13.31 39.1
705.6 14.17 38.1
575.5 17.38 148
508.5 19.67 23.2

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 3.00 of the experimental database (Apr 16, 2020)