Fermi energy in semiconductors

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SUMMARY

The discussion centers on the concept of Fermi energy in intrinsic semiconductors, particularly at absolute zero temperature (T=0). It establishes that the Fermi energy, or chemical potential, is not equal to the conduction band minimum (E_c) or the valence band maximum (E_v) but is positioned in the middle of the band gap. The conversation highlights complications arising from adding electrons at T=0, which introduces configurational entropy and challenges the third law of thermodynamics, asserting that entropy (S) must equal zero at absolute zero. The dialogue also touches on the degeneracy of the conduction band minimum, indicating that it is not always degenerate.

PREREQUISITES
  • Understanding of thermodynamics, specifically the equation dU=Tds-Pdv+μdN.
  • Familiarity with semiconductor physics, including concepts of conduction and valence bands.
  • Knowledge of Fermi energy and its significance in solid-state physics.
  • Awareness of the third law of thermodynamics and its implications at absolute zero.
NEXT STEPS
  • Research the implications of Fermi energy in various semiconductor materials.
  • Explore the role of configurational entropy in solid-state physics.
  • Study the effects of temperature on semiconductor behavior, particularly near absolute zero.
  • Investigate the concept of degeneracy in conduction band minima across different semiconductor types.
USEFUL FOR

Physicists, materials scientists, and electrical engineers interested in semiconductor theory, thermodynamics, and the behavior of materials at low temperatures.

hokhani
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From thermodynamics we have dU=Tds-Pdv+\mu dN. So the chemical potential is the energy change due to adding an extra particle when S and V are constant. Now consider an intrinsic semiconductor at T=0 in which the valence band is all-occupied and conduction band is empty. If we add an extra electron to the lowest point of conduction band (an specified point in the conduction band) the energy change would be E_c and so the Fermi energy (chemical potential).

Then, why the Fermi energy is in the middle of band gap and is not E_c?
 
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Why not E_v, as you can as well remove an electron?
Besides that, this is quite an academic discussion as T=0 cannot be reached. For finite temperatures mu is well defined. Hence you can take the limit T to 0.
 
Let's complicate things a little bit since you chose to discuss the T=0 case. If you add an electron to the semiconductor, then this will lead to a finite configurational entropy due to the degenerate states in which you can add the electron. But this would violate the third law of thermodynamics that is S=0 at T=0.

Discussing imperfections at 0K would always lead to complications. But it still fun to think about them!
 
Useful nucleus said:
Let's complicate things a little bit since you chose to discuss the T=0 case. If you add an electron to the semiconductor, then this will lead to a finite configurational entropy due to the degenerate states in which you can add the electron. But this would violate the third law of thermodynamics that is S=0 at T=0.

Discussing imperfections at 0K would always lead to complications. But it still fun to think about them!

I don't see why. The minimum of the conduction band is usually not degenerate.
 
DrDu, I agree with you if the minimum of the conduction band is non-degenerate, but that this is always the case, is something new to me.
 

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