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uid 546

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This species has a counterpart in the theoretical database.

Transitions

νk
[cm-1]
λ
[μm]
int
[km/mol]
2520 3.968 504
2350 4.255 146
2251 4.442 159
2026 4.936 53.9
1863 5.368 192
1840 5.435 459
1775 5.634 296
1670 5.988 94.3
1540 6.494 134
1530 6.536 135
1521 6.575 198
1436 6.964 197
1354 7.386 60.8
1289 7.758 232
1265 7.905 17.5
1184 8.446 75.3
1174 8.518 128
1084 9.225 34.9
920 10.87 24.9
915 10.93 23.9
901 11.1 22.4
894 11.19 72.3
881 11.35 1.05e+3
842 11.88 270
831 12.03 125
815 12.27 227
804 12.44 113
794 12.59 64.8
779 12.84 394
762 13.12 291
755 13.25 59.8
747 13.39 424
717 13.95 167
705 14.18 59.8
695 14.39 101
656 15.24 24.4
618 16.18 32.4
612 16.34 74.8
610 16.39 95.8

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)