Electron Effective Mass and Effective Mass Theory in Semiconductors

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SUMMARY

The concept of "effective mass" in semiconductors is crucial for understanding electron mobility and the behavior of quasiparticles within the framework of Fermi Liquid Theory. It simplifies complex many-body interactions by allowing electrons to be treated similarly to free electrons in a vacuum, facilitating easier calculations. Effective mass theory is particularly useful for calculating energies associated with shallow defects in semiconductors, although it is not applicable for deep defects due to the limitations of the approximations involved.

PREREQUISITES
  • Understanding of semiconductor physics
  • Familiarity with Fermi Liquid Theory
  • Knowledge of electron mobility concepts
  • Basic principles of defect theory in semiconductors
NEXT STEPS
  • Explore the implications of effective mass on electron mobility in semiconductors
  • Study the mathematical formulation of Fermi Liquid Theory
  • Investigate the differences between shallow and deep defects in semiconductors
  • Learn about the role of orbital overlap in determining effective mass
USEFUL FOR

Researchers, physicists, and engineers working in semiconductor technology, particularly those focused on electronic properties and defect analysis in materials.

mendes
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I would like to ask about the reason why the electron "effective mass" was introduced in semiconductors. What is its' usefulness ?

And also about the so-called "effective mass theory" used to calculate energies for the shallow defects in semiconducors. What are mean pecularities and approximations of this theory and why we can't use it to calculate deep defects.

Thanks.
 
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mendes said:
I would like to ask about the reason why the electron "effective mass" was introduced in semiconductors. What is its' usefulness ?

Er.. there are many properties that depends on the effective mass. The mobility is one example. So that's one reason why such a concept was introduced.

Another reason is that, within the Fermi Liquid Theory, we can lump all the many-body interactions into this "renormalized" mass (effective mass), creating a "quasiparticle", rather than a bare electron. This allows us to go from a many-body problem (difficult), to many one-body problem (easier).

Zz.
 
Simply because you can behave electrons in semiconductors like in electrons in vacuum with effective mass.
 
in simple metals, the effective mass can be related to the orbital overlap. strongly overlapping orbitals give states with free electron like character, whereas a reduced overlap increases the effective mass..
 

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