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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]
3757 2.662 147
1624 6.158 167
1587 6.301 196
1508 6.631 121
1456 6.868 101
1430 6.993 110
1409 7.097 332
1394 7.174 924
1370 7.299 147
1365 7.326 294
1357 7.369 440
1352 7.396 206
1348 7.418 889
1334 7.496 137
1326 7.541 231
1309 7.639 1.04e+3
1274 7.849 121
1258 7.949 107
1247 8.019 60.9
1208 8.278 47.1
1183 8.453 255
1170 8.547 84.8
1163 8.598 13.8
1142 8.757 35.3
1109 9.017 17
1036 9.653 23
992 10.08 32.8
885 11.3 68.8
816 12.25 28.4
797 12.55 35.8
786 12.72 72.4
764 13.09 238
751 13.32 154
734 13.62 387
720 13.89 348
717 13.95 365
706 14.16 219
692 14.45 216
646 15.48 11.6
615 16.26 28.7
588 17.01 264
576 17.36 154
508 19.69 31.4

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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75 species present in version 2.00 of the experimental database (Nov 13, 2013)