Normal incidence on 2 dielectric boundaries

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SUMMARY

The discussion focuses on calculating the total reflected intensity of light at two dielectric boundaries when light is normally incident. The problem involves a medium with impedance Z1, a layer of thickness L and impedance Z2, and a third medium with impedance Z3. Key equations include the continuity of tangential electric (E) and magnetic (H) fields across boundaries, and the reflection coefficient for a single boundary, r = (Z2 - Z1)/(Z1 + Z2). The challenge lies in accounting for multiple reflections within the second medium, which can be addressed using matrix methods as referenced in standard thin film optics literature.

PREREQUISITES
  • Understanding of impedance in wave propagation (Z1, Z2, Z3)
  • Familiarity with the continuity conditions for electromagnetic fields
  • Knowledge of thin film optics and multiple reflection phenomena
  • Ability to work with matrix representations of wave equations
NEXT STEPS
  • Study the derivation of the reflection and transmission coefficients in thin films
  • Learn about matrix methods in optics for handling multiple reflections
  • Explore the implications of varying thickness on interference patterns in thin films
  • Review the texts "Optics of Thin Films" by Knittel and "Optics" by Vasicek for detailed examples
USEFUL FOR

Students and professionals in optics, particularly those dealing with thin film interference, as well as researchers in photonics and materials science looking to deepen their understanding of light behavior at dielectric interfaces.

Robsta
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Homework Statement


I've not been able to do this question for years so I'd really appreciate some help.

Light is normaly incident from a medium 1 with impedance Z1 through a layer of medium 2 of thickness L and impedance Z2 into medium 3 of impedance Z3. Obtain an expression for the total reflected intensity of light when the thickness corresponds to:
a) λ2/4
b) λ2/2

where λ2 is the wavelength of the light in medium 2.

Homework Equations


I know that the tangential components of the E and B fields are continuous over the boundaries so at each interface:

E1f + E1b = E2f +E2b = E3f
H1f + H1b = H2f +H2b = H3f

where f and b signify forward and backward going waves

Also, E1f/H1f = Z1
And E1b/H1b = -Z1

I know how to do this for the one boundary problem where you get r = (Z2 - Z1)/(Z1+Z2) and t = 2Z2/(Z2+Z1) But I can't apply it to the first boundary as now there's a wave coming the other way being reflected from the second boundary. It all seems intractably complicated but I know this is a fairly standard problem, so I'm finding it really frustrating.

3. The Attempt at a Solution


I don't really even know how to start. The wave in the middle material will bounce back and forwards seemingly infinitely and I don't know how to deal with that. I've just said in the middle there's the sum of a forward going and a backward going wave. I don't really know if the equations above are right for the middle section.
 
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You find the answer in any book about thin film optics. Vasicek, Heavens fro example. Or Knittel https://archive.org/details/OpticsOfThinFilms.
If you have still problems, I write about it later.
All the multiple reflected waves add up to a wave traveling forward and an other, traveling backward. You can set up the relation between the waves in front of an interface and behind that interface, and also at the two boundaries of a medium. All these relationship can be written in matrix from.
 

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