1 / 37

ENE 451

ENE 451. Fundamental of Optical Engineering Lecture 8. Example of polarizations. A linearly polarized plane wave with Ē vector described by

neylan
Download Presentation

ENE 451

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. ENE 451 Fundamental of Optical Engineering Lecture 8

  2. Example of polarizations • A linearly polarized plane wave with Ē vector described by is incident on an optical element under test. Describe the state of polarization of the output wave (linear, elliptrical, or circular) if the optical element is:

  3. Example of polarizations • (a) A linear polarizer oriented to transmit light polarized in the ex direction.

  4. Example of polarizations • (b) A half-wave plate with birefringence axes oriented to coincide with ex and ey.

  5. Example of polarizations • (c) A half-wave plate with birefringence axes oriented at 45º relative to ex and ey .

  6. Example of polarizations • (d) A quarter-wave plate with birefringence axes oriented to coincide with ex and ey .

  7. Example of polarizations • (e) A quarter-wave plate with birefringence axes oriented at 45º relative to ex and ey .

  8. Example of polarizations • (f) A half-wave plate with birefringence axes oriented at 25º relative to ex and ey .

  9. Example of polarizations • (g) A quarter-wave plate with birefringence axes oriented at 25º relative to ex and ey .

  10. Example of polarizations • A linearly polarized light propagating in the z-direction with polarization vector in the x-direction is incident on a birefringent crystal. What is the state of polarization of the light after passing through the crystal if: (a) the crystal is a quarter-wave plate with optic axis in the xy plane oriented at 30º relative to the y-axis?

  11. Example of polarizations • (b) the crystal is a half-wave plate with optic axis in the y-direction?

  12. Example of polarizations • (c) the crystal is a half-wave plate with optic axis in the xy plane oriented at 11º relative to the x-axis?

  13. Example of polarizations • (d) the crystal is a quarter-wave plate with optic axis in the xy plane oriented at 45º relative to the y-axis?

  14. Example of polarizations • (e) the crystal is a quarter-wave plate with optic axis in the z-direction?

  15. Example of birefringence • For a birefringent median with n0 = 1.654 and nE = 1.485 as shown in the figure. Find the length L that makes it be (a) a full wave plate (b) a half wave plate (c) a ¼ -wave plate if the wavelength is 656 nm.

  16. Example of birefringence

  17. Electrooptic modulator • This makes use of electrooptic effect (applied electric fields used to change the optical properties). • There are 2 kinds of electrooptic effect: linear and quadratic.

  18. Pockels effect • The linear electrooptic effect is called “Pockels effect”. • This refers to the change in the indices of the ordinary and extranordinary rays proportional to applied electric field. • This effect exists only in crystals without an inversion symmetry such as LiNbO3.

  19. Kerr effect • For a crystal with an inversion symmetry, the linear electrooptic effect can not exist, while the quadratic electrooptic effect known as “Kerr effect” is observed. • This is where the induced index change is proportional to the square of applied electric field.

  20. Optical modulator

  21. Optical modulator • V (pi-voltage) or half-wave voltage is the applied voltage that makes the relative phase shift be  in a cube of material. • In general, = refractive index changes produced by applied voltage.

  22. Optical modulator • It is preferable to design L >> h to have a low applied voltage V. • After applying a voltage, indices are changed as

  23. Example • V for the material is 2,700 V, L = 2 cm, and h = 0.5 mm. Find applied voltage V to have Δ =  (complete extinction).

  24. Example • An electrooptic crystal has dimensions of 2x2x3 along the x,y, and z axes with nE = 1.487 and nO = 1.536. An input wave propagating in the z-direction at λ = 0.63 μm is linearly polarized at a 45º angle relative to the x- and y- axes. A voltage V applied across the crystal in the x-direction. The voltage is increased from V = 0 until, when V = 245 V, the output polarization from the crystal is the same as that observed for V = 0. Assume that optic axis is along the y-axis. • (a) What is the total phase retardation, in rad, for V = 0? • (b) What is pi-voltage for the material? • (c) What is the refractive index change Δnx produced by the applied voltage of 245 V, assuming Δny =0?

  25. Interference in thin films • Recall: interference eq.

  26. Interference in thin films • Assume that

  27. Interference in thin films • Reflectance • We can consider R into 3 cases: • n1 = n3. • n1 < n2, n2>n3 , n1≠ n3. • n1 < n2 < n3.

  28. Interference in thin films • Case 1: n1 = n3 • From a definition: Aij = Aji

  29. Interference in thin films • Max in R for • Min in R for

  30. Example • n1 = 1.5, n2 = 1.6, and λ = 0.63 μm. Find t2 for Rmax and Rmin.

  31. Interference in thin films • Case 2: n1 < n2, n2>n3 , n1≠ n3.

  32. Interference in thin films • Max in R for • Min in R for

  33. Example • n1 = 1.5, n2 = 1.6, n3 = 1.4, λ = 0.63 μm. Find t2 for Rmax and Rmin.

  34. Interference in thin films • Case 3: n1 < n2 < n3

  35. Interference in thin films • Max in R for • Min in R for

  36. Example • n1 = 1.5, n2 = 1.6, n3 = 1.7, λ = 0.63 μm. Find t2 for Rmax and Rmin.

More Related