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顺式-顺式和反式-垂直HOONO:作用光谱学与异构化动力学

Cis-cis and trans-perp HOONO: action spectroscopy and isomerization kinetics.

作者信息

Fry Juliane L, Nizkorodov Sergey A, Okumura Mitchio, Roehl Coleen M, Francisco Joseph S, Wennberg Paul O

机构信息

Arthur Amos Noyes Laboratory of Chemical Physics, California Institute of Technology, Pasadena, California 91125, USA.

出版信息

J Chem Phys. 2004 Jul 15;121(3):1432-48. doi: 10.1063/1.1760714.

DOI:10.1063/1.1760714
PMID:15260688
Abstract

The weakly bound HOONO product of the OH+NO2+M reaction is studied using the vibrational predissociation that follows excitation of the first OH overtone (2nu1). We observe formation of both cis-cis and trans-perp conformers of HOONO. The trans-perp HOONO 2nu1 band is observed under thermal (223-238 K) conditions at 6971 cm(-1). We assign the previously published (warmer temperature) HOONO spectrum to the 2nu1 band at 6365 cm(-1) and 2nu1-containing combination bands of the cis-cis conformer of HOONO. The band shape of the trans-perp HOONO spectrum is in excellent agreement with the predicted rotational contour based on previous experimental and theoretical results, but the apparent origin of the cis-cis HOONO spectrum at 6365 cm(-1) is featureless and significantly broader, suggesting more rapid intramolecular vibrational redistribution or predissociation in the latter isomer. The thermally less stable trans-perp HOONO isomerizes rapidly to cis-cis HOONO with an experimentally determined lifetime of 39 ms at 233 K at 13 hPa (in a buffer gas of predominantly Ar). The temperature dependence of the trans-perp HOONO lifetime in the range 223-238 K yields an isomerization barrier of 33+/-12 kJ/mol. New ab initio calculations of the structure and vibrational mode frequencies of the transition state perp-perp HOONO are performed using the coupled cluster singles and doubles with perturbative triples [CCSD(T)] model, using a correlation consistent polarized triple zeta basis set (cc-pVTZ). The energetics of cis-cis, trans-perp, and perp-perp HOONO are also calculated at this level [CCSD(T)/cc-pVTZ] and with a quadruple zeta basis set using the structure determined at the triple zeta basis set [CCSD(T)/cc-pVQZ//CCSD(T)/cc-pVTZ]. These calculations predict that the anti form of perp-perp HOONO has an energy of DeltaE0=42.4 kJ/mol above trans-perp HOONO, corresponding to an activation enthalpy of DeltaH298 (double dagger 0)=41.1 kJ/mol. These results are in good agreement with statistical simulations based on a model developed by Golden, Barker, and Lohr. The simulated isomerization rates match the observed decay rates when modeled with a trans-perp to cis-cis HOONO isomerization barrier of 40.8 kJ/mol and a strong collision model. The quantum yield of cis-cis HOONO dissociation to OH and NO2 is also calculated as a function of photon excitation energy in the range 3500-7500 cm(-1), assuming D0=83 kJ/mol. The quantum yield is predicted to vary from 0.15 to 1 over the observed spectrum at 298 K, leading to band intensities in the action spectrum that are highly temperature dependent; however, the observed relative band strengths in the cis-cis HOONO spectrum do not change substantially with temperature over the range 193-273 K. Semiempirical calculations of the oscillator strengths for 2nu1(cis-cis HOONO) and 2nu1(trans-perp HOONO) are performed using (1) a one-dimensional anharmonic model and (2) a Morse oscillator model for the OH stretch, and ab initio dipole moment functions calculated using Becke, Lee, Yang, and Parr density functional theory (B3LYP), Møller-Plesset pertubation theory truncated at the second and third order (MP2 and MP3), and quadratic configuration interaction theory using single and double excitations (QCISD). The QCISD level calculated ratio of 2nu1 oscillator strengths of trans-perp to cis-cis HOONO is 3.7:1. The observed intensities indicate that the concentration of trans-perp HOONO early in the OH+NO2 reaction is significantly greater than predicted by a Boltzmann distribution, consistent with statistical predictions of high initial yields of trans-perp HOONO from the OH+NO2+M reaction. In the atmosphere, trans-perp HOONO will isomerize nearly instantaneously to cis-cis HOONO. Loss of HOONO via photodissociation in the near-IR limits the lifetime of cis-cis HOONO during daylight to less than 45 h, other loss mechanisms will reduce the lifetime further.

摘要

利用在激发第一个OH泛频(2ν1)后发生的振动预解离,对OH + NO2 + M反应中弱束缚的HOONO产物进行了研究。我们观察到了HOONO的顺 - 顺式和反 - 垂直式构象体的形成。在热(223 - 238 K)条件下,在6971 cm⁻¹处观察到反 - 垂直式HOONO的2ν1带。我们将先前发表的(较高温度下)HOONO光谱归属于6365 cm⁻¹处的2ν1带以及HOONO顺 - 顺式构象体中包含2ν1的组合带。反 - 垂直式HOONO光谱的带形与基于先前实验和理论结果预测的转动轮廓非常吻合,但6365 cm⁻¹处顺 - 顺式HOONO光谱的表观起源没有特征且明显更宽,这表明后一种异构体中分子内振动重新分布或预解离更快。热稳定性较差的反 - 垂直式HOONO在13 hPa(主要是Ar缓冲气体)、233 K时迅速异构化为顺 - 顺式HOONO,实验测定的寿命为39 ms。在223 - 238 K范围内反 - 垂直式HOONO寿命的温度依赖性得出异构化势垒为33±12 kJ/mol。使用耦合簇单双激发并微扰三重激发[CCSD(T)]模型,采用相关一致极化三重ζ基组(cc - pVTZ),对过渡态反 - 反式HOONO的结构和振动模式频率进行了新的从头算计算。在此水平[CCSD(T)/cc - pVTZ]以及使用四重ζ基组并基于在三重ζ基组确定的结构[CCSD(T)/cc - pVQZ//CCSD(T)/cc - pVTZ],还计算了顺 - 顺式、反 - 垂直式和反 - 反式HOONO的能量。这些计算预测反 - 反式HOONO的反式形式比反 - 垂直式HOONO的能量高ΔE0 = 42.4 kJ/mol,对应于活化焓ΔH298(双 dagger 0)= 41.1 kJ/mol。这些结果与基于Golden、Barker和Lohr开发的模型的统计模拟结果非常吻合。当用40.8 kJ/mol的反 - 垂直式到顺 - 顺式HOONO异构化势垒和强碰撞模型进行模拟时,模拟的异构化速率与观察到的衰减速率相匹配。假设D0 = 83 kJ/mol,还计算了顺 - 顺式HOONO解离为OH和NO2的量子产率作为3500 - 7500 cm⁻¹范围内光子激发能量 的函数。预测在298 K下观察到 的光谱范围内量子产率从0.15变化到1,导致作用光谱中的带强度高度依赖于温度;然而,在193 - 273 K范围内顺 - 顺式HOONO光谱中观察到的相对带强度随温度变化不大。使用(1)一维非谐模型和(2)OH伸缩振动的莫尔斯振子模型,以及使用Becke、Lee、Yang和Parr密度泛函理论(B3LYP)、在二阶和三阶截断的Møller - Plesset微扰理论(MP2和MP3)以及使用单激发和双激发的二次组态相互作用理论(QCISD)计算的从头算偶极矩函数,对2ν1(顺 - 顺式HOONO)和2ν1(反 - 垂直式HOONO)的振子强度进行了半经验计算。QCISD水平计算的反 - 垂直式与顺 - 顺式HOONO的2ν1振子强度之比为3.7:1。观察到的强度表明,在OH + NO2反应早期反 - 垂直式HOONO的浓度明显大于玻尔兹曼分布预测的值,这与OH + NO2 + M反应中反 - 垂直式HOONO高初始产率的统计预测一致。在大气中,反 - 垂直式HOONO将几乎瞬间异构化为顺 - 顺式HOONO。近红外光解离导致的HOONO损失限制了顺 - 顺式HOONO在白天的寿命小于45小时,其他损失机制将进一步缩短其寿命。

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