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激光诱导 2-溴-2-硝基丙烷的紫外光解:OH 和 Br 形成的动力学。

Laser-induced UV photodissociation of 2-bromo-2-nitropropane: dynamics of OH and Br formation.

机构信息

Radiation and Photochemistry Division, Bhabha Atomic Research Centre, Trombay, Mumbai 400 085, India.

出版信息

J Chem Phys. 2011 Jan 28;134(4):044316. doi: 10.1063/1.3532085.

Abstract

Photoexcitation of 2-bromo-2-nitropropane (BNP) at 248 and 193 nm generates OH, Br, and NO(2) among other products. The OH fragment is detected by laser-induced fluorescence spectroscopy, and its translational and internal state distributions (vibration, rotation, spin-orbit, and Λ-doubling components) are probed. At both 248 and 193 nm, the OH fragment is produced translationally hot with the energy of 10.8 and 17.2 kcal∕mol, respectively. It is produced vibrationally cold (v" = 0) at 248 nm, and excited (v" = 1) at 193 nm with a vibrational temperature of 1870 ± 150 K. It is also generated with rotational excitation, rotational populations of OH(v" = 0) being characterized by a temperature of 550 ± 50 and 925 ± 100 K at 248 and 193 nm excitation of BNP, respectively. The spin-orbit components of OH(X(2)Π) are not in equilibrium on excitation at 193 nm, but the Λ-doublets are almost in equilibrium, implying no preference for its π lobe with respect to the plane of rotation. The NO(2) product is produced electronically excited, as detected by measuring UV-visible fluorescence, at 193 nm and mostly in the ground electronic state at 248 nm. The Br product is detected employing resonance-enhanced multiphoton ionization with time-of-flight mass spectrometer for better understanding of the dynamics of dissociation. The forward convolution analysis of the experimental data has provided translational energy distributions and anisotropy parameters for both Br((2)P(3∕2)) and Br∗((2)P(1∕2)). The average translational energies for the Br and Br∗ channels are 5.0 ± 1.0 and 6.0 ± 1.5 kcal∕mol. No recoil anisotropies were observed for these products. Most plausible mechanisms of OH and Br formation are discussed based on both the experimental and the theoretical results. Results suggest that the electronically excited BNP molecules at 248 and 234 nm relax to the ground state, and subsequently dissociate to produce OH and Br through different channels. The mechanism of OH formation from BNP on excitation at 193 nm is also discussed.

摘要

2-溴-2-硝基丙烷(BNP)在 248nm 和 193nm 光激发下生成 OH、Br 和 NO2 等产物。通过激光诱导荧光光谱检测 OH 碎片,并探测其平动和内部分布(振动、旋转、自旋轨道和Λ-双重分量)。在 248nm 和 193nm 激发时,OH 碎片分别以 10.8 和 17.2kcal/mol 的能量产生热平动。在 248nm 时,它以振动冷(v"=0)的状态产生,而在 193nm 时则以振动激发(v"=1)的状态产生,振动温度为 1870±150K。OH 也具有旋转激发,BNP 在 248nm 和 193nm 激发时,OH(v"=0)的转动布居分别由温度 550±50 和 925±100K 来表征。在 193nm 激发时,OH(X2Π)的自旋轨道分量没有达到平衡,但 Λ-双重态几乎处于平衡状态,这意味着 OH 相对于旋转平面没有对其π叶瓣的偏好。通过测量 UV-可见荧光检测到,在 193nm 激发时,NO2 产物处于电子激发态,而在 248nm 激发时主要处于基态电子态。通过共振增强多光子电离与飞行时间质谱联用检测 Br 产物,以更好地了解离解动力学。对实验数据的正向卷积分析为 Br((2)P(3∕2))和 Br*((2)P(1∕2))提供了平动能分布和各向异性参数。Br 和 Br*通道的平均平动能分别为 5.0±1.0 和 6.0±1.5kcal/mol。这些产物没有观察到反冲各向异性。基于实验和理论结果,讨论了 OH 和 Br 形成的最合理机制。结果表明,248nm 和 234nm 激发的电子激发 BNP 分子弛豫到基态,随后通过不同的通道解离生成 OH 和 Br。还讨论了 193nm 激发时 BNP 生成 OH 的机制。

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