1 / 75

Chapter 07&08 & 09 & 10

Chapter 07&08 & 09 & 10. PHOTONIC-CRYSTAL OPTICS. 下几页列出重 要的概 念,需掌握. WaVE Transfer Matrix. Scattering Matrix. Airy's formulas. Fabry -Perot Etalon. Bragg Grating. Bloch Modes. Chapter 8. Comments…why?. Comments…integration circuits. 在小空间里控制光场的传播 , 用 于信息交换及应用!.

mikaia
Télécharger la présentation

Chapter 07&08 & 09 & 10

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Chapter 07&08 & 09 & 10

  2. PHOTONIC-CRYSTAL OPTICS • 下几页列出重要的概念,需掌握

  3. WaVETransfer Matrix

  4. Scattering Matrix

  5. Airy's formulas

  6. Fabry-Perot Etalon

  7. Bragg Grating

  8. Bloch Modes

  9. Chapter 8

  10. Comments…why?...

  11. Comments…integration circuits 在小空间里控制光场的传播,用于信息交换及应用!

  12. Photonic Crystals Metamaterials 尺寸更小,亚波长,<200nm • From a similar consideration

  13. Planar-Mirror Waveguides

  14. Firstly, from ray optics… • Reflection by mirrors • Correct in microwave frequency

  15. Why?... At microwave • Perfect electric conductor (PEC) • ε = ― • n= j • |r|=1 • Phase change: 0 or π (半波损) • 0: 边界场强极大 • π: 边界场强为零

  16. Periodicity  Discrete modes

  17. Propagation Constants

  18. Dispersion Relation 截止频率f0。f <f0 (波长大时)模式消失,无法传播。在截止频率处,群速度为零,即慢光效应。

  19. Group Velocity c.cosθ c 一种特殊的光学延迟线 θπ/2, 越慢

  20. Field Distributions 正交归一本征模式

  21. Multimode Fields

  22. Comments • m=1,2,3… • How about m=0? • Infinite field amplitude, not allowed • Cutoff size: d>dc=/2 But coaxial PEC waveguide supports m=0 TEM mode, which in non-cutoff!

  23. PLANAR DIELECTRIC WAVEGUIDES

  24. Comparing to Section 1 No longer PEC boundary conditions • With field outside the core • With non-zero/pi reflection phase Now Electromagnetic optics

  25. Phase condition

  26. Field Distributions … with EM boundary conditions!

  27. Dispersion Relation

  28. Dispersion…

  29. Group Velocity Goos-Hänchenshift 当相位为常数时,v=c.cosθ

  30. Goos-Hänchen shift • Usually… positive and very small, <0.05λ • Could be negative and with large value in left-handed metamaterials • Backward energy flux • Strong dispersion in LHM

  31. GH shift can make a cavity nature_450_397

  32. Two-Dimensional Waveguides

  33. Boundary Conditions

  34. Applications

  35. Optical Coupling in waveguides

  36. Input Couplers 尽可能大的交叠积分

  37. End-Fire configuration

  38. Prism & Grating Side Couplers To match the wavevectorm…

  39. Fibers 圆柱对称二维光波导,选择性阅读

  40. Vortex modes & Higher-OAM modes

  41. Resonator • From waveguide • Spatial confinement of EM waves • select specific frequencies from a signal • To generate stronger EM field intensity • For applications that need strong EM field • Laser • Quantum Physics • ……

  42. Examples

  43. Planar-Mirror Resonators

  44. Resonator Modes Interference … standing wave …

  45. Similar to 1D waveguides … Smaller d  larger vf (uncertainty principle)

  46. As Traveling waves Multiple interference…

  47. Traveling-Wave Resonator 驻波的缺点:场强分布不均匀,例如E~cos(kz)。 Traveling wave? 场强均匀分布,优点: 例如可以充分利用增益介质等。

More Related