Acta Physica Sinica, Volume. 69, Issue 6, 064206-1(2020)
Figures & Tables(9)
Fig. 1. Schematic illustration of smoothing by dynamic interference structures of beamlets.
Fig. 2. The contrast of focal spots with different phase modulation.
Fig. 3. Dynamic interference structures with different kinds of phase modulation: (a) Tilted phase; (b) cylinder phase; (c) ellipsoid phase; (d) spiral phase.
Fig. 4. (a) Variation of contrast with integral time and (b) FOAPI curves with different phase plate array.
Fig. 5. Variation of contrast with integral time with different PV.
Fig. 6. Variation of contrast with integral time of different Δ
Fig. 7. Focused intensity distributions with different smoothing scheme: (a) CPP only; (b) 2D-SSD + CPP; (c) smoothing by dynamic interference structures of beamlets + CPP; (d) smoothing by dynamic interference structures of beamlets+2D-SSD + CPP.
Fig. 8. (a) Variation of contrast with integral time and (b) FOPAI curves with different smoothing scheme.
Table 1.
2D-Fourier transform of different phase distribution.
不同相位分布的二维傅里叶变换表达式
View tableView in ArticleTable 1.
2D-Fourier transform of different phase distribution.
不同相位分布的二维傅里叶变换表达式
$ {\varphi }_{1}(x_{f}, y_{f}) $ $ B_{1}(x_{f}, y_{f}) $ $ b_{1}(x_{f}, y_{f}) $ x $ {\delta }[x_{f}/({\lambda f})+1/(2\text{π} )]{\delta }[y_{f}/({\lambda f})] $ 0 –x2 $ \text{π} ^{1/2}\delta [y_{f}/(\lambda f) ]$ $ \text{π} ^{2}x_{f}^{2}/({\lambda }^{2}f^{2})-3\text{π} /4 $ $ -[h_{1}{ }(x/w)^{2}+ h_{2}(y/w)^{2}] $ $ w^{2}\text{π} (h_{1}h_{2})^{-1/2} $ $ \text{π} ^{2}x_{f}^{2}/(h_{1}{\lambda }^{2}f^{2}w^{2})+\text{π} ^{2}y_{f}^{2}/(h_{2}{\lambda }^{2}f^{2}w^{2})-3\text{π} /2 $ $ \arctan(y/x) $ $ [-{\lambda f}/(2\text{π} )]\{ {\delta }[x_{f}/({\lambda f})]{\rm d}{\delta }[y_{f}/({\lambda f})]/{\rm d}y_{f }- {\rm i}{\delta }[y_{f}/({\lambda f})]{\rm d}\delta [x_{f}/({\lambda f})]/{\rm d}x_{f}\} $
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Hao Xiong, Zhe-Qiang Zhong, Bin Zhang, Zhan Sui, Xiao-Min Zhang.
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Received: Jun. 20, 2019
Accepted: --
Published Online: Nov. 19, 2020
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