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Assuming two degenerate photons that are linearly polarized, the TPA cross section (σ$_{TPA}$) can be calculated using the imaginary part of the third-order response property as | Assuming two degenerate photons that are linearly polarized, the TPA cross section (σ$_{TPA}$) can be calculated using the imaginary part of the third-order response property as | ||
- | {{ :adf:12300b2e-e2fe-40ec-98fb-33cda0f9407e.png?500 }} | + | {{ :adf:5ab2e60d-6c93-49b0-8b5e-8f6ee1ac5411.png?350 }} |
- | * 精细结构常数α$_f$=e$^2$/ | + | * 精细结构常数α=e$^2$/ |
* σ$_{TPA}$单位为Göppert-Mayer (1 GM = 10$^{−50}$ cm$^4$ s photon$^{−1}$) | * σ$_{TPA}$单位为Göppert-Mayer (1 GM = 10$^{−50}$ cm$^4$ s photon$^{−1}$) | ||
* 整数N取决于实验设置 | * 整数N取决于实验设置 | ||
- | * γ二阶超极化率,在ADF软件中,超极化率选项选择γ TPA,即可计算γ(-ω, | + | * γ约化形式的二阶超极化率γ(-ω, |
* ω频率 | * ω频率 | ||
- | * Im表示取虚部 | + | * Im[]表示取虚部 |