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首页> 外文期刊>The Journal of Chemical Physics >RESONANT X-RAY SCATTERING BEYOND THE BORN-OPPENHEIMER APPROXIMATION - SYMMETRY BREAKING IN THE OXYGEN RESONANT X-RAY EMISSION SPECTRUM OF CARBON DIOXIDE
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RESONANT X-RAY SCATTERING BEYOND THE BORN-OPPENHEIMER APPROXIMATION - SYMMETRY BREAKING IN THE OXYGEN RESONANT X-RAY EMISSION SPECTRUM OF CARBON DIOXIDE

机译:硼-苯甲醚近似之外的共振X射线散射-二氧化碳氧共振X射线发射光谱的对称破裂。

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Although resonant x-ray scattering of molecules fulfills strict electronic symmetry selection rules, as now firmly proven by. spectra of diatomic molecules, the accumulated body of data for polyatomic molecules indicates that an apparent breaking of these rules represents the common situation rather than the exception. The CO2 molecule provides a good example of symmetry breaking, with the. oxygen x-ray emission spectra showing strong intensity for transitions that are forbidden by the parity selection rule. We present time-independent and time-dependent theories for frequency-dependent resonant x-ray scattering beyond, the Born-Oppenheimer approximation in order to explore under what circumstances one can anticipate symmetry breaking in the spectra of polyatomic molecules. The theory starts out from the Kramers-Heisenberg dispersion relation and is generalized for vibrational degrees of freedom and for nonadiabatic coupling of the electronic (vibronic) states, including the frequency dependency of, the scattering cross section. Different Limiting cases and few-level models are considered. The symmetry breaking is proven to be the result of pseudo-Jahn-Teller-Like vibronic coupling between near-degenerate core-excited states. Thus vibromic interaction over the antisymmetric vibrational mode between the ''bright'' 1 sigma(g)(-1)2 pi(u)(-1) and ''dark'' 1 sigma(u)(-1)2 pi(u)(-1) intermediate states of CO2 allows transitions otherwise forbidden. The measurements and theory demonstrate that the symmetry-selective character of the resonant x-ray emission is strongly frequency dependent. The strong intensity of ''dipole-forbidden'' transitions in the pi* oxygen K spectrum at resonance is reduced monotonically with the detuning of the excitation energy from resonance, and the spectra become ''symmetry purified.'' Simulations with full vibronic coupling predict this feature of the x-ray scattering experiment and a few-level model explains the energy dependence of the symmetry selection and the symmetry purification at large detuning energies in the limit of narrowband photon excitation. (C) 1997 American Institute of physics. [References: 36]
机译:尽管分子的共振X射线散射符合严格的电子对称性选择规则,但现在已被可靠地证明。在双原子分子的光谱中,多原子分子数据的累积表明,这些规则的明显破坏代表了普遍的情况,而不是例外。 CO2分子提供了一个很好的对称破坏实例。氧x射线发射光谱显示出奇偶性选择规则所禁止的跃迁的强强度。为了探讨在什么情况下可以预期多原子分子光谱中的对称性破裂,我们提出了与时间无关的和与时间有关的理论,用于频率相关的共振X射线散射,超出了Born-Oppenheimer近似。该理论从Kramers-Heisenberg色散关系开始,并针对振动自由度和电子(振动)态的非绝热耦合(包括散射截面的频率依赖性)进行了概括。考虑了不同的极限情况和少数级别的模型。对称破坏被证明是近简并的核激发态之间的拟Jahn-Teller-Like振动耦合的结果。因此,在``明亮的''1 sigma(g)(-1)2 pi(u)(-1)和``黑暗的''1 sigma(u)(-1)2 pi之间的反对称振动模式下的振动相互作用(u)(-1)的CO2中间状态允许过渡,否则将被禁止。测量和理论表明,共振x射线发射的对称选择性特征与频率密切相关。随着共振能量的失谐,共振中pi *氧K光谱中“偶极禁态”跃迁的强强度随着共振能量的失谐而单调减少,并且光谱变得“对称纯化”。全振动耦合模拟预测了X射线散射实验的这一特征,并建立了一个几级模型来解释在窄带光子激发的极限下,在大失谐能量下对称选择和对称纯化的能量依赖性。 (C)1997年美国物理研究所。 [参考:36]

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