Optical process in semiconductors

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SUMMARY

The discussion focuses on the optical absorption process in both indirect and direct bandgap semiconductors, specifically addressing the relationship between the wave vectors of electrons and photons. It establishes that the condition \hbar\vec{q} << \hbar\vec{k} holds true due to the significant difference in wavelengths, with typical optical photons having a wavelength of approximately 500nm compared to the picometer range of electrons' DeBroglie wavelength. This disparity in scale directly influences the energy and momentum changes experienced by electrons upon photon absorption.

PREREQUISITES
  • Understanding of solid-state physics concepts
  • Familiarity with bandgap types: direct and indirect
  • Knowledge of wave vector notation and calculations
  • Basic principles of optical absorption in semiconductors
NEXT STEPS
  • Study the mathematical models of optical absorption in semiconductors
  • Learn about the DeBroglie wavelength and its implications in quantum mechanics
  • Explore the differences between direct and indirect bandgap semiconductors
  • Investigate the role of momentum conservation in photon-electron interactions
USEFUL FOR

Students and professionals in solid-state physics, semiconductor researchers, and anyone studying the optical properties of materials will benefit from this discussion.

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Homework Statement


I'm trying to understand this part of my notes where the optical absorption in both indirect and direct bandgap semiconductors. This part specifically mathematically describes the change in energy and momentum of an electron in a semiconductor after it has absorbed energy from incident photon.

Qn: Why is \hbar\vec{q} &lt;&lt; \hbar\vec{k}?


Homework Equations



http://img222.imageshack.us/img222/9665/qnmj5.th.jpg

This is the part I am referring to.

The Attempt at a Solution

 
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Hmm, I am currently taking Solid State myself and am currently learning this material, but I'll try to offer some insight.

I would think that \hbar\vec{q} &lt;&lt; \hbar\vec{k} would have to be true when you consider the wavelengths of typical electrons and photons.

Remember that the magnitude of the wave vector for either electron or photon is:

k=\frac{2\pi}{\lambda}

Where, for electrons, lambda is the DeBroglie Wavelength.

An average optical photon has a wavelength of ~500nm, while the DeBroglie wavelength of an electron is in the picometer range, much, much smaller. So, how does this effect the relative values of k and q and thus, the values of \hbar k and \hbar q?
 
Last edited:
Oh yeah, you're right. That should be the explanation. Thanks.
 

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