The effect of ethynyl substitution and cyclopenta fusion on the ultraviolet absorption spectra of polycyclic aromatic hydrocarbons

Author(s):  
Nathan D Marsh ◽  
Celina J Mikolajczak ◽  
Mary J Wornat
2018 ◽  
Vol 610 ◽  
pp. A65 ◽  
Author(s):  
Elena Maltseva ◽  
Cameron J. Mackie ◽  
Alessandra Candian ◽  
Annemieke Petrignani ◽  
Xinchuan Huang ◽  
...  

Aim. We aim to elucidate the spectral changes in the 3 μm region that result from chemical changes in the molecular periphery of polycyclic aromatic hydrocarbons (PAHs) with extra hydrogens (H-PAHs) and methyl groups (Me-PAHs). Methods. Advanced laser spectroscopic techniques combined with mass spectrometry were applied on supersonically cooled 1,2,3,4-tetrahydronaphthalene, 9,10-dihydroanthracene, 9,10-dihydrophenanthrene, 1,2,3,6,7,8-hexahydropyrene, 9-methylanthracene, and 9,10-dimethylanthracene, allowing us to record mass-selective and conformationally selective absorption spectra of the aromatic, aliphatic, and alkyl CH-stretches in the 3.175 − 3.636 µm region with laser-limited resolution. We compared the experimental absorption spectra with standard harmonic calculations and with second-order vibrational perturbation theory anharmonic calculations that use the SPECTRO program for treating resonances. Results. We show that anharmonicity plays an important if not dominant role, affecting not only aromatic, but also aliphatic and alkyl CH-stretch vibrations. The experimental high-resolution data lead to the conclusion that the variation in Me- and H-PAHs composition might well account for the observed variations in the 3 μm emission spectra of carbon-rich and star-forming regions. Our laboratory studies also suggest that heavily hydrogenated PAHs form a significant fraction of the carriers of IR emission in regions in which an anomalously strong 3 μm plateau is observed.


2019 ◽  
Vol 21 (37) ◽  
pp. 21094-21103 ◽  
Author(s):  
Isaac Benkyi ◽  
Enrico Tapavicza ◽  
Heike Fliegl ◽  
Dage Sundholm

Absorption spectra of polycyclic aromatic hydrocarbons have been simulated by using a real-time generating function method that combines adiabatic electronic excitation energies with vibrational energies of the excited states.


Sign in / Sign up

Export Citation Format

Share Document