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Peacock dogbane beetle opal Thin Film Interference.

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Presentation on theme: "Peacock dogbane beetle opal Thin Film Interference."— Presentation transcript:

1 peacock dogbane beetle opal Thin Film Interference

2 k1k1 k2k2 y Maxima at: if then

3 Reflection from a dielectric slab: n IoIo Reflectance: IRIR (near normal incidence) R = 0.04 for glass.96 1.04.0384.0369 To consider interference between the front and back reflection, assume they have the same amplitude: 0.04 I o ( n = relative index)

4 Dielectric Films n Assume near normal incidence: What is  ? Physical path difference: 2 t t Optical path difference:

5 Wait!! Reflections can cause phase shifts! First reflection:  phase shift Second reflection: no phase shift “Reflection” path difference: Total phase difference: ConstructiveDestructive How does this lead to color?

6 white n t o (nm) R t = 400 nm, n = 1.515,  = 0

7 For varying angle of incidence: normal and 45 degrees 045

8

9 4% per interface adds up!

10 Goal: R = 0, T = 1 (Impedance Matching) E k n g n o Can only adjust n

11 nfnf nono E k ngng Antireflection coating

12 Antireflection coating: two requirements n f = x t n s = 1.5 n o = 1.0 1. Destructive interference:

13 1. Equal amplitudes:

14

15 Reflections from the front and back surfaces of a dielectric slab result in two plane waves with an optical path difference and therefore exhibit interference. The interference effects can be engineered to minimize reflectance or produce pretty colors.


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