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uid 543

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This species has a counterpart in the theoretical database.

Transitions

νk
[cm-1]
λ
[μm]
int
[km/mol]
4859 2.058 1.32e+4
3253 3.074 56.7
3074 3.253 302
3028 3.303 67.6
2917 3.428 9.12
2900 3.448 98.2
2852 3.506 105
2738 3.653 147
2634 3.796 110
2592 3.857 51
2533 3.948 54.5
2492 4.013 101
1587 6.302 325
1572 6.363 5.14
1544 6.479 289
1456 6.868 279
1449 6.901 57.5
1430 6.994 207
1409 7.096 292
1397 7.16 72.1
1393 7.178 41.9
1390 7.197 55.8
1348 7.417 1.64e+3
1326 7.539 246
1274 7.849 116
1258 7.95 209
1247 8.019 87.1
1208 8.282 47.8
1170 8.551 109
1142 8.753 55
1109 9.019 37.8
1096 9.127 7.62
991.5 10.09 36.1
823 12.15 39.6
816.2 12.25 52.2
786.2 12.72 20.8
738.3 13.54 24.7
732.6 13.65 9.41
715.7 13.97 161
693.1 14.43 19.3
645.8 15.48 22.1
623.2 16.05 69.2
615.2 16.25 25.1
586.4 17.05 58.4

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