chapter 3 & 4

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Chapter 3 & 4 Beam Optics + Fourier Optics 1

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Chapter 3 & 4. Beam Optics + Fourier Optics. 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. 3.1 THE GAUSSIAN BEAM. Under paraxial Helmholtz equation. Properties. W 0 ~ z 0 1/2. 束缚越强,扩散越大!. Gouy Phase. Divergence and Gouy Phase. Dispersion Relation - PowerPoint PPT Presentation

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Page 1: Chapter 3 & 4

1

Chapter 3 & 4Beam Optics + Fourier Optics

Page 2: Chapter 3 & 4

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

Page 3: Chapter 3 & 4

3.1 THE GAUSSIAN BEAM

Page 4: Chapter 3 & 4

Under paraxial Helmholtz equation

Page 5: Chapter 3 & 4
Page 6: Chapter 3 & 4

Properties

W0 ~ z01/2

束缚越强,扩散越大!

Page 7: Chapter 3 & 4

Gouy Phase

Page 8: Chapter 3 & 4

Divergence and Gouy Phase

Dispersion Relation kx

2+ky2+kz

2=k02

Isotropic media

Page 9: Chapter 3 & 4

Divergence and Gouy Phase

Confinement in x-y w(z)

Broadening in kx-ky

1/w(z)

Divergence and Gouy Phase

Page 10: Chapter 3 & 4

Gouy Phasekx

2 + ky2 + kz

2 = k2

OL 26, 485 (2001)

源于量子受限效应

Page 11: Chapter 3 & 4

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

Page 12: Chapter 3 & 4
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3.2 TRANSMISSION THROUGH OPTICAL COMPONENTS

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光路设计上很重要

Page 16: Chapter 3 & 4

3.4 LAGUERRE-GAUSSIAN AND BESSEL BEAMS

Page 17: Chapter 3 & 4

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!

Page 18: Chapter 3 & 4

Vortex

Page 19: Chapter 3 & 4

Generation

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Applications

Page 21: Chapter 3 & 4

Bessel Beams

< k, Gouy Phase

Non-integrable

Page 22: Chapter 3 & 4

FOURIER OPTICS

Page 23: Chapter 3 & 4

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

Page 25: Chapter 3 & 4

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

Page 29: Chapter 3 & 4

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

Page 38: Chapter 3 & 4
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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

Page 40: Chapter 3 & 4

SNOM

Page 41: Chapter 3 & 4

Perfect lense / superlensePhys. 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

Page 42: Chapter 3 & 4

science_308_534 (2005)

Page 43: Chapter 3 & 4

END

Page 44: Chapter 3 & 4

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

Page 45: Chapter 3 & 4

Homework EXERCISE 4.1-1

What is Fresnel Approximation and Fraunhofer approximation? Explain their difference

EXERCISE 4.2-2

EXERCISE 4.3-3