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uid 548

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This species has a counterpart in the theoretical library

Transitions

Frequency
[wavenumbers]
Wavelength
[microns]
Integrated cross-section
[km/mol]
3777 2.648 49.59
3757 2.662 63.11
3712 2.694 78.89
3574 2.798 15.78
3090 3.236 306.6
3072 3.255 299.8
3026 3.305 22.54
1926 5.192 22.54
1856 5.388 20.29
1692 5.91 31.56
1624 6.158 54.1
1608 6.219 65.37
1554 6.435 115
1546 6.468 31.56
1532 6.527 302
1505 6.645 128.5
1489 6.716 72.13
1472 6.793 38.32
1444 6.925 277.2
1438 6.954 126.2
1405 7.117 112.7
1364 7.331 60.86
1351 7.402 288.5
1335 7.491 160
1305 7.663 193.8
1273 7.855 78.89
1260 7.937 81.14
1247 8.019 299.8
1233 8.11 72.13
1166 8.576 63.11
1120 8.929 27.05
877 11.4 90.16
831 12.03 81.14
800 12.5 160
794 12.59 63.11
755 13.25 295.3
753 13.28 92.42
705 14.18 81.14
577 17.33 139.8

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)