School of Chemistry, University of Bristol, Bristol BS8 1TS, United Kingdom.
J Chem Phys. 2010 Jun 7;132(21):214307. doi: 10.1063/1.3427544.
This article reports a comprehensive study of the mechanisms of H atom loss in aniline (C(6)H(5)NH(2)) following ultraviolet excitation, using H (Rydberg) atom photofragment translational spectroscopy. N-H bond fission via the low lying (1)pi sigma() electronic state of aniline is experimentally demonstrated. The (1)pi sigma() potential energy surface (PES) of this prototypical aromatic amine is essentially repulsive along the N-H stretch coordinate, but possesses a shallow potential well in the vertical Franck-Condon region, supporting quasibound vibrational levels. Photoexcitation at wavelengths (lambda(phot)) in the range 293.859 nm > or = lambda(phot) > or = 193.3 nm yields H atom loss via a range of mechanisms. With lambda(phot) resonant with the 1(1)pi pi() <-- S(0) origin (293.859 nm), H atom loss proceeds via, predominantly, multiphoton excitation processes, resonantly enhanced at the one photon energy by the first (1)pi pi(*) excited state (the 1(1)pi pi(*) state). Direct excitation to the first few quasibound vibrational levels of the (1)pi sigma(*) state (at wavelengths in the range 269.513 nm > or = lambda(phot) > or = 260 nm) induces N-H bond fission via H atom tunneling through an exit barrier into the repulsive region of the (1)pi sigma() PES, forming anilino (C(6)H(5)NH) radical products in their ground electronic state, and with very limited vibrational excitation; the photo-prepared vibrational mode in the (1)pi sigma() state generally evolves adiabatically into the corresponding mode of the anilino radical upon dissociation. However, as the excitation wavelength is reduced (lambda(phot) < 260 nm), N-H bond fission yields fragments with substantially greater vibrational excitation, rationalized in terms of direct excitation to 1(1)pi pi() levels, followed by coupling to the (1)pi sigma() PES via a 1(1)pi pi()/(1)pi sigma() conical intersection. Changes in product kinetic energy disposal once lambda(phot) approaches approximately 230 nm likely indicate that the photodissociation pathways of aniline proceed via direct excitation to the (higher) 2(1)pi pi() state. Analysis of the anilino fragment vibrational energy disposal-and thus the concomitant dynamics of (1)pi sigma() state mediated photodissociation-provides a particularly interesting study of competing sigma() <-- pi and pi(*) <-- pi absorption processes and develops our appreciation of the photochemistry of aromatic amines. It also allows revealing comparisons with simple amines (such as ammonia and methylamine) as well as the isoelectronic species, phenol. This study yields a value for the N-H bond strength in aniline, D(0)(H-anilino) = 31630+/-40 cm(-1).
本文报道了利用 H(里德堡)原子光碎片翻译光谱学研究苯胺(C(6)H(5)NH(2))中 H 原子损失机制的综合研究。通过苯胺的低能(1)pi sigma()电子态实验证明了 N-H 键的断裂。该典型芳香胺的(1)pi sigma()势能面(PES)沿 N-H 伸缩坐标基本呈排斥性,但在垂直 Franck-Condon 区域具有浅势阱,支持准束缚振动能级。在波长(lambda(phot))为 293.859nm >= lambda(phot)>= 193.3nm 的范围内进行光激发,通过多种机制导致 H 原子损失。当 lambda(phot)与 1(1)pi pi()<--S(0)起源(293.859nm)共振时,H 原子损失主要通过多光子激发过程进行,通过第一(1)pi pi(*)激发态(1(1)pi pi(*)态)在单光子能量处共振增强。直接激发到(1)pi sigma(*)态的前几个准束缚振动能级(在波长范围 269.513nm >= lambda(phot)>= 260nm)诱导 N-H 键断裂,通过 H 原子隧穿通过出口势垒进入(1)pi sigma()PES 的排斥区域,形成苯胺基(C(6)H(5)NH)自由基产物处于其基态,并且振动激发非常有限;(1)pi sigma()态中光制备的振动模式通常在离解时绝热地演变为苯胺基自由基的相应模式。然而,随着激发波长的减小(lambda(phot)<260nm),N-H 键断裂产生的碎片具有更大的振动激发,这可以通过直接激发到 1(1)pi pi()能级来合理地解释,然后通过与(1)pi sigma()PES 耦合通过 1(1)pi pi()/(1)pi sigma()锥形交叉。当 lambda(phot)接近约 230nm 时,产物动能处置的变化可能表明苯胺的光解途径通过直接激发到(更高)2(1)pi pi()态进行。对苯胺片段振动能处置的分析 - 因此对(1)pi sigma()介导的光解的伴随动力学 - 提供了对竞争 sigma()<--pi 和 pi(*)<--pi 吸收过程的特别有趣的研究,并增强了我们对芳香胺光化学的认识。它还允许与简单的胺(如氨和甲胺)以及等电子体苯酚进行比较。这项研究得出了苯胺中 N-H 键强度的值,D(0)(H-苯胺基)= 31630+/-40cm(-1)。