Konen Ian M, Li Eunice X J, Lester Marsha I, Vázquez Juana, Stanton John F
Department of Chemistry, University of Pennsylvania, Philadelphia, Pennsylvania 19104-6323, USA.
J Chem Phys. 2006 Aug 21;125(7):074310. doi: 10.1063/1.2234772.
High resolution infrared spectra of nitric acid have been recorded in the first OH overtone region under jet-cooled conditions using a sequential IR-UV excitation method. Vibrational bands observed at 6933.39(3), 6938.75(4), and 6951.985(3) cm(-1) (origins) with relative intensities of 0.42(1), 0.38(1), and 0.20(1) are attributed to strongly mixed states involved in a Fermi resonance. A vibrational deperturbation analysis suggests that the optically bright OH overtone stretch (2nu1) at 6939.2(1) cm(-1) is coupled directly to the nu1 + 2nu2 state at 6946.4(1) cm(-1) and indirectly to the 3nu2 + nu3 + nu7 state at 6938.5(1) cm(-1). Both the identity of the zero-order states and the indirect coupling scheme are deduced from complementary CCSD(T) calculations in conjunction with second-order vibrational perturbation theory. The deperturbation analysis also yields the experimental coupling between 2nu1 and nu1 + 2nu2 of -6.9(1) cm(-1), and that between the two dark states of +5.0(1) cm(-1). The calculated vibrational energies and couplings are in near quantitative agreement with experimentally derived values except for a predicted twofold stronger coupling of 2nu1 to nu1 + 2nu2. Weaker coupling of the strongly mixed states to a dense background of vibrational states via intramolecular vibrational energy redistribution is evident from the experimental linewidths of 0.08 and 0.25 cm(-1) for the higher energy and two overlapping lower energy bands, respectively. A comprehensive rotational analysis of the higher energy band yields spectroscopic parameters and the direction of the OH overtone transition dipole moment.
利用顺序红外 - 紫外激发方法,在喷射冷却条件下记录了硝酸在首个OH泛频区域的高分辨率红外光谱。在6933.39(3)、6938.75(4)和6951.985(3) cm⁻¹(谱带起源)处观测到的振动谱带,其相对强度分别为0.42(1)、0.38(1)和0.20(1),归因于参与费米共振的强混合态。振动去微扰分析表明,在6939.2(1) cm⁻¹处光学明亮的OH泛频伸缩振动(2ν₁)直接与在6946.4(1) cm⁻¹处的ν₁ + 2ν₂态耦合,并间接与在6938.5(1) cm⁻¹处的3ν₂ + ν₃ + ν₇态耦合。零阶态的身份和间接耦合方案均通过结合二阶振动微扰理论的互补CCSD(T)计算推导得出。去微扰分析还得出2ν₁与ν₁ + 2ν₂之间的实验耦合为 -6.9(1) cm⁻¹,以及两个暗态之间的耦合为 +5.0(1) cm⁻¹。计算得到的振动能量和耦合与实验推导值几乎在数量上一致,只是预测的2ν₁与ν₁ + 2ν₂的耦合强度要强两倍。从较高能量谱带和两个重叠的较低能量谱带的实验线宽分别为0.08和0.25 cm⁻¹可以明显看出,强混合态通过分子内振动能量重新分布与密集的振动态背景的耦合较弱。对较高能量谱带进行的全面转动分析得出了光谱参数以及OH泛频跃迁偶极矩的方向。