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Chapter 3 & 4 Beam Optics + Fourier Optics 1
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Comments 第二章的延续 非平面波 主要沿 z 方向传播 在横截面( xy )里,电磁场为非均匀分布
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3.1 THE GAUSSIAN BEAM
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Under paraxial Helmholtz equation
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Properties W 0 ~ z 0 1/2 束缚越强,扩散越大!
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Gouy Phase
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Divergence and Gouy Phase Dispersion Relation k x 2 +k y 2 +k z 2 =k 0 2 Isotropic media
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Divergence and Gouy Phase Confinement in x-y w(z) Broadening in k x -k y 1/w(z) Divergence and Gouy Phase
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Gouy Phase k x 2 + k y 2 + k z 2 = k 2 OL 26, 485 (2001) 源于量子受限效应
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Problems Broadening in wavevector? Could explain the divergence! Wrong for Gouy phase Weights of different Fourier components do not vary with distance z! Why? Paraxial Approximation A dilemma exists! 也许值得探讨
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3.2 TRANSMISSION THROUGH OPTICAL COMPONENTS
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光路设计上 很重要
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3.4 LAGUERRE-GAUSSIAN AND BESSEL BEAMS
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伴随着 l ,存在环状能流, 在光学蜗旋上、光镊里起 到关键作用!
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Vortex
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Generation
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Applications
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Bessel Beams < k, Gouy Phase Non-integrable
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FOURIER OPTICS
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based on harmonic analysis (the Fourier transform) linear systems
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Expansion Methods Fourier Optics Expansion based on the solutions of wave equation -- plane waves Paraxial Optics? LG waves HG waves Expansion based on the orthogonal and complete sets
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4.1 PROPAGATION OF LIGHT IN FREE SPACE
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算法实现 周期边界性条件 取样区域的尺寸大小 A 为周期 Fourier Transformation 中, k=n2π/A, 取分立值 可调用 Fast Fourier Transformation (FFT) 命 令
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4.2 OPTICAL FOURIER TRANSFORM
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4.3 DIFFRACTION OF LIGHT
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WHY? x kx Sharp edge high spatial frequency
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Problem? We must utilize the components with higher wavevectors kx, ky>k kz become pure imaginary! Evanescent waves & surface waves Bigger k smaller wavelength 电镜, x-ray
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SNOM
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Perfect lense / superlense Phys. Rev. Lett. 85, 3966–3969 (2000), cited by 4500 times 用左手材料 / 负折射率( left-handed materials or negative refractive media )材料可以实现超聚焦
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science_308_534 (2005)
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END
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Homework Plot the curves of Eqs. (3.1-8) to (3.1-10) versus z, and explain what they means EXERCISE 3.1-3 EXERCISE 3.1-2
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Homework EXERCISE 4.1-1 What is Fresnel Approximation and Fraunhofer approximation? Explain their difference EXERCISE 4.2-2 EXERCISE 4.3-3
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