Snell's law with a complex refractive index

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SUMMARY

This discussion focuses on the application of Snell's Law in the context of complex refractive indices, specifically addressing the extinction coefficient (k) and its impact on the refractive angle (B). The participants clarify that while Snell's Law, expressed as N sin(A) = N' sin(B), remains valid, the angle B can be a complex number when absorption is present. The conversation highlights the need for careful consideration of boundary conditions and the complexities introduced by polarized light at media interfaces, particularly with examples like air and silicon, where N values are 1 and 4.4-0.8i, respectively.

PREREQUISITES
  • Understanding of Snell's Law and its mathematical formulation
  • Familiarity with complex refractive indices, specifically the form N = n - ik
  • Knowledge of wave propagation in different media, including plane waves
  • Basic principles of polarization and boundary conditions in optics
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  • Research the derivation of Snell's Law for complex refractive indices
  • Explore the implications of absorption on light propagation in materials
  • Study the effects of polarized light at media interfaces
  • Examine experimental methods to measure complex angles of refraction
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Optics researchers, physicists, and engineering professionals interested in advanced light-matter interactions and the behavior of light in complex media.

zhanghe
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hello everyone

Consider extinction coefficient k, n becomes N=n-ik.
the textbook says NsinA=N'sinB still holds itself.

But the sinB,for exmple, may be a complex number, i want to know
how to get B?
how to understand this situation, which is the refractive angle?
the B's real part?
 
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The electric field in a plane wave E~exp[i(kx-wt)], where k=w N/c.
If N=n-ia, then E~exp[i(nw/c)x-wt)exp[-ax].
This means n is still used by Snell.
k is usually the wave number, so I used a for I am N.
 
thank you
and you mean that the refrective angle only depends on Re N--n
and has nothing to do with I am N--a(using your signal), right?
 
pam said:
The electric field in a plane wave E~exp[i(kx-wt)], where k=w N/c.
If N=n-ia, then E~exp[i(nw/c)x-wt)exp[-ax].
This means n is still used by Snell.
k is usually the wave number, so I used a for I am N.

Why you write exp{i[(nw/c)x-wt]}*exp(-ax) and not exp{i[(nw/c)x-wt]}*exp(axw/c) ?
 
Last edited:
Sorry. That was a misprint. It should be axw/c.

"and you mean that the refrective angle only depends on Re N--n"
I'm afraid I oversimplified. The boundary conditions have to be applied at the interface, and the derivation done from scratch. It gets quite complicated.
 
these days ,i thought further that maybe it's only a kind of appearance to describe the polirized light phase shift at the interface of different media.
but i wonder which is the refractive angle if k ,ie absorption exist.
for example. air/silicon,whose N is 1 and 4.4-0.8i, respectively.
to Snell, 1*sin(AOI)=(4.4-0.8i)*sin(AOR),
AOR will be a complex number, how to get the real AOR in experiments?
 

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