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uid 540

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This species has a counterpart in the theoretical database.

Transitions

νk
[cm-1]
λ
[μm]
int
[km/mol]
2315 4.32 308
2136 4.682 516
2069 4.833 112
2008 4.98 59.6
1937 5.163 103
1791 5.583 430
1732 5.774 476
1689 5.921 852
1663 6.013 266
1648 6.068 553
1526 6.553 131
1500 6.667 84.1
1443 6.93 119
1377 7.262 134
1338 7.474 266
1274 7.849 366
1258 7.949 126
1239 8.071 526
1152 8.681 123
911 10.98 50.7
885 11.3 228
839 11.92 136
782 12.79 138
764 13.09 284
734 13.62 352
720 13.89 604
717 13.95 488
698 14.33 23.8
692 14.45 13.2
675 14.81 6.03
665 15.04 3.49
651 15.36 28.8
626 15.97 68.9
613 16.31 77.8
588 17.01 530
578 17.3 94.6
574 17.42 129
540 18.52 92.5
535 18.69 102
526 19.01 38.5
522 19.16 30.1

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)