Explaining Surface Plasmon Excitation by Light

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SUMMARY

Surface plasmon excitation by light requires that the incident light possesses a component normal to the surface, a condition fulfilled by p-polarized light. This necessity arises from the conservation of momentum and the distinct boundary conditions dictated by Maxwell's equations. The electric field parallel to the surface diminishes due to high charge mobility, while the normal component can build up stronger fields outside the metal, facilitating plasmon generation. Understanding these principles is crucial for manipulating surface plasmons effectively.

PREREQUISITES
  • Understanding of surface plasmon resonance (SPR)
  • Familiarity with p-polarized light and its properties
  • Basic knowledge of Maxwell's equations
  • Concept of electric displacement field (D) and its relationship to electric field (E)
NEXT STEPS
  • Research the principles of surface plasmon resonance (SPR) in detail
  • Study the behavior of p-polarized light in optical applications
  • Explore the implications of Maxwell's equations in electromagnetic theory
  • Investigate the role of electric displacement fields in plasmonics
USEFUL FOR

Physicists, optical engineers, and researchers in nanotechnology focusing on surface plasmon applications and light-matter interactions.

geo_alchemist
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Surface Plasmons ?

Well, to begin with, I am not a physicist and therefore please don't redirect me to some physics tutorials.
now the question:
Why is it necessary for surface plasmon exitation by light that the incident light must have component normal to the surface?
I know that this condition can be fulfilled only in case of p-polarized light. but my questioin is about necessity of normal component.
Pls, if anyone can explain this to me, I would be much obliged.
 
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Isn't it just conservation of momentum?
If you want plasmons to be generated to the left of a surface then the light coming in from the right must reflect to the right.
 


Sorry, I can't follow the point.
may be for you it looks as A, B, C, but for me it's far more complex.
can you tell me in more details, what you mean by "If you want plasmons to be generated to the left of a surface then the light coming in from the right must reflect to the right"?
 


Inside the metal, all electric fields are very small, as conductivity is high. Now from the Maxwell equations there arise two different boundary conditions for the electric field parallel and normal to the surface. The electric field component parallel to the surface has to be continuous, while normal to the surface, D has to be continuous. Now even if E normal to the surface inside the metal is small, D=E*epsilon is much larger as the absolute value of epsilon is high (roughly equal to the conductivity of the metal).
Roughly speaking, the electric field parallel to the surface approximately vanishes due to the high mobility of the charges parallel to the surface. In direction normal to the surface, the mobility of the charges is hindered (by the surface) so that higher fields can build up, at least outside the metal.
 

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