Esposito Vincent J, Ferrari Piero, Palmer C Zachary, Boersma Christiaan, Candian Alessandra, Fortenberry Ryan C, Buma Wybren Jan, Tielens Alexander G G M
NASA Ames Research Center, Astrophysics Branch, Moffett Field, California 94035, United States.
Radboud University, Institute for Molecules and Materials, FELIX Laboratory, Nijmegen 6525 XZ, The Netherlands.
J Phys Chem Lett. 2025 Feb 6;16(5):1296-1304. doi: 10.1021/acs.jpclett.4c03396. Epub 2025 Jan 27.
The CN stretch frequency of neutral, gas-phase 9-cyanoanthracene is 2207 cm (4.531 μm) based on high-resolution infrared absorption experiments coupled with a new hybrid anharmonic quantum chemical methodology. A broad band (full-width at half-maximum of 47 cm) is observed and assigned to multiple transitions, including the CN stretch fundamental and various combination bands that gather intensity from strong anharmonic coupling with the bright CN stretch. The new hybrid computational approach utilizes the harmonic force constants from the double-hybrid rev-DSDPBEP86 functional that includes MP2 electron correlation, and the cubic and quartic force constants from the B3LYP density functional. In combination, this method computes a band center of 2207 cm for 9-cyanoanthracene, a direct match with experiment. Further, the hybrid method produces a difference of less than 1 cm for the two isomers of cyanonaphthalene and cyanobenzene. As shown from comparison with CCSD(T)-F12b anharmonic frequency computations of cyanobenzene, inclusion of electron correlation is required to properly characterize the electronic structure of the highly electron withdrawing CN group on polycyclic aromatic hydrocarbons. In agreement with earlier studies, computation of the CN stretch of 14 small CN-PAHs produces a narrow (∼20 cm) band from 2207-2229 cm (4.53-4.48 μm). The remainder of the spectrum below 2000 cm and from 3000-3120 cm shows good agreement between experiment and the hybrid theory with a mean absolute error of 16 and 14 cm, respectively.
基于高分辨率红外吸收实验以及一种新的混合非谐量子化学方法,中性气相9-氰基蒽的C≡N伸缩频率为2207 cm⁻¹(4.531 μm)。观察到一个宽带(半高宽为47 cm),并将其归因于多个跃迁,包括C≡N伸缩基频以及各种因与明亮的C≡N伸缩产生强非谐耦合而聚集强度的组合带。这种新的混合计算方法利用了包含MP2电子相关的双杂化rev-DSDPBEP86泛函的谐性力常数,以及B3LYP密度泛函的三次和四次力常数。综合起来,该方法计算出9-氰基蒽的带中心为2207 cm⁻¹,与实验结果直接匹配。此外,该混合方法对氰基萘和氰基苯的两种异构体计算得到的差值小于1 cm。与苯甲腈的CCSD(T)-F12b非谐频率计算结果相比表明,需要考虑电子相关才能正确表征多环芳烃上强吸电子C≡N基团的电子结构。与早期研究一致,对14种小的CN-PAHs的C≡N伸缩计算在2207 - 2229 cm⁻¹(4.53 - 4.48 μm)范围内产生一个窄带(约20 cm)。在2000 cm⁻¹以下以及3000 - 3120 cm⁻¹范围内的其余光谱,实验与混合理论之间显示出良好的一致性,平均绝对误差分别为16 cm和14 cm。