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Rotation of methyl radicals in a solid argon matrix

机译:固体氩气基质中甲基的旋转

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Electron spin resonance (ESR) measurements were carried out to study the rotation of methyl radicals (CH3) in a solid argon matrix at 14-35 K temperatures. The radicals were produced by dissociating methane by plasma bursts generated either by a focused 193 nm laser radiation or a radio frequency discharge device during the gas condensation on the substrate. The ESR spectrum exhibits axial symmetry at the lowest temperature and is ascribed to ground state molecules with symmetric total nuclear spin function I=3/2. The hyperfine anisotropy (A(parallel to)-A(perpendicular to)) was found to be -0.01 mT, whereas that of the g value was 2.5x10(-5). The anisotropy is observed for the first time in Ar and is manifested by the splitting of the low-field transition. Elevation of temperature leads reversibly to the appearance of excited state contribution having antisymmetric I=1/2. As a function of the sample temperature, the relative intensities of symmetric and antisymmetric spin states corresponding to ground and excited rotor states, respectively, proton hyperfine and electron g-tensor components, and spin-lattice relaxation rates were determined by a numerical fitting procedure. The experimental observations were interpreted in terms of a free rotation about the C-3 axis and a thermal activation of the C-2-type rotations above 15 K. The ground and excited rotational state energy levels were found to be separated by 11.2 cm(-1) and to exhibit significantly different spin-lattice coupling. A crystal field model has been applied to evaluate the energy levels of the hindered rotor in the matrix, and crystal field parameter epsilon(4)=-200 cm(-1), corresponding to a 60 cm(-1) effective potential barrier for rotation of the C-3 axis, was obtained. (c) 2007 American Institute of Physics.
机译:进行电子自旋共振(ESR)测量以研究在14-35 K温度下固体氩气基质中甲基(CH3)的旋转。自由基是通过在基板上的气体凝结过程中,通过聚焦193 nm激光辐射或射频放电设备产生的等离子体脉冲分解甲烷而产生的。 ESR光谱在最低温度下表现出轴向对称性,并归因于具有对称总核自旋函数I = 3/2的基态分子。发现超细各向异性(A(平行于)-A(垂直于))为-0.01 mT,而g值为2.5x10(-5)。各向异性是在Ar中首次观察到的,并通过低场跃迁的分裂得以体现。温度的升高可逆地导致出现具有反对称I = 1/2的激发态贡献。作为样品温度的函数,分别通过数值拟合程序确定分别对应于基态和受激转子态,质子超细和电子g张量分量的对称和反对称自旋态的相对强度,以及自旋晶格弛豫率。根据绕C-3轴的自由旋转和高于15 K的C-2-型旋转的热激活来解释实验观察结果。发现基态和激发态的能级相隔11.2 cm( -1)并表现出显着不同的自旋-晶格耦合。晶体场模型已应用于评估矩阵中受阻转子的能级,并且晶体场参数epsilon(4)=-200 cm(-1),对应于60 cm(-1)的有效势垒获得了C-3轴的旋转角。 (c)2007年美国物理研究所。

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