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uid 548

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This species has a counterpart in the theoretical database.

Transitions

νk
[cm-1]
λ
[μm]
int
[km/mol]
3777 2.648 49.6
3757 2.662 63.1
3712 2.694 78.9
3574 2.798 15.8
3090 3.236 307
3072 3.255 300
3026 3.305 22.5
1926 5.192 22.5
1856 5.388 20.3
1692 5.91 31.6
1624 6.158 54.1
1608 6.219 65.4
1554 6.435 115
1546 6.468 31.6
1532 6.527 302
1505 6.645 128
1489 6.716 72.1
1472 6.793 38.3
1444 6.925 277
1438 6.954 126
1405 7.117 113
1364 7.331 60.9
1351 7.402 289
1335 7.491 160
1305 7.663 194
1273 7.855 78.9
1260 7.937 81.1
1247 8.019 300
1233 8.11 72.1
1166 8.576 63.1
1120 8.929 27
877 11.4 90.2
831 12.03 81.1
800 12.5 160
794 12.59 63.1
755 13.25 295
753 13.28 92.4
705 14.18 81.1
577 17.33 140

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)