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arXiv physics/0508051physics.opticsphysics.chem-ph
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双光子吸收截面色散的基本极限

Fundamental Limits of the Dispersion of the Two-Photon Absorption Cross-Section

Javier Pérez Moreno, Mark G. Kuzyk

摘要:

我们严格地将求和规则应用到态求和表达式中,计算了双光子吸收截面色散的基本极限。理论与数据的比较表明,三能级模型中的截断和规则给出了合理的基本限制。通过严格的解析计算,证明了双光子吸收截面在极限附近只有三个主态,共振项随态的增加而减小.我们还发现,在分析具有多个激发态的实际分子时,即使在共振附近,非显共振项的贡献也不能忽略。然而,令人费解的是,外推的非共振的结果,共振只使用三能级模型的共振项被证明是与准确的结果是一致的。此外,非共振近似示出的规模与完整的三能级模型相比,在几何学上。这种缩放可用于简化测量结果的分析。我们发现现有的分子离基本极限还很远,因此还有改进的空间。但是,达到基本极限需要精确控制能级间距,而不依赖于跃迁偶极矩--使用今天的合成方法似乎不可能完成这项任务。因此,我们提出的替代方法,仍然可以导致实质性的改进,只需要控制的过渡时刻的第一激发态。虽然它是最好的标准化测量的双光子吸收截面的基本限制时,比较分子,我们表明,简单地除以每个分子的电子数的平方产生一个很好的度量比较。

英文摘要:

We rigorously apply the sum rules to the sum-over-states expression to calculate the fundamental limits of the dispersion of the two-photon absorption cross-section. A comparison of the theory with the data suggests that the truncated sum rules in the three-level model give a reasonable fundamental limit. Our ansatz that the two photon absorption cross-section near the limit must have only three dominant statesis is supported by a rigorous analytical calculation that the resonant term gets smaller as more states are added. We also find that the contributions of the non-explicitly resonant terms can not be neglected when analyzing real molecules with many excited states, even near resonance. However, puzzling as it may be, extrapolating an off-resonant result to resonance using only the resonant term of the three-level model is shown to be consistent with the exact result. In addition, the off-resonant approximation is shown to scale logarithmically when compared with the full three-level model. This scaling can be used to simplify the analysis of measurements. We find that existing molecules are still far from the fundamental limit; so, there is room for improvement. But, reaching the fundamental limit would require precise control of the energy-level spacing, independently of the transition dipole moments -- a task that does not appear possible using today's synthetic approaches. So, we present alternative methods that can still lead to substantial improvements which only require the control of the transition moment to the first excited state. While it is best to normalize measured two photon absorption cross-sections to the fundamental limits when comparing molecules, we show that simply dividing by the square of the number of electrons per molecule yields a good metric for comparison.

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