Non-equilibrium conduction electrons

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Discussion Overview

The discussion revolves around the behavior of non-equilibrium conduction electrons in semiconductors following excitation from the valence band to the conduction band, particularly focusing on the implications of long recombination times and the definitions of chemical potential and Fermi distribution in this context.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants question the behavior of non-equilibrium electrons in the conduction band during long recombination times, specifically whether they relax to the band minima and how they are distributed.
  • One participant suggests that in a semiconductor at room temperature with a small band gap, there may already be established knowledge about the behavior of conduction band electrons.
  • Another participant asserts that non-equilibrium electrons will relax to the band minima through electron-phonon interactions and that they do not follow the Fermi-Dirac distribution, which applies only to thermally excited electrons.
  • In contrast, a different participant argues that intraband scattering processes can lead to a quasi-equilibrium state where the distribution of electrons aligns with the Fermi function, introducing the concept of a quasi-Fermi level.
  • A later reply acknowledges the argument about quasi-equilibrium and agrees that the Fermi distribution applies only for short timescales between excitation and recombination.

Areas of Agreement / Disagreement

Participants express disagreement regarding the applicability of the Fermi distribution to non-equilibrium electrons, with some asserting that it does not apply while others argue that a quasi-equilibrium can be reached. The discussion remains unresolved on the exact nature of the chemical potential in this context.

Contextual Notes

The discussion highlights the dependence on timescales for various processes, such as interband and intraband scattering, which may influence the thermalization and distribution of conduction electrons.

BeauGeste
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Here's the issue I'm trying to wade through:

1. If you excite electrons from valence band to conduction band (with a laser say), you are out of thermodynamic equilibrium. In some recombination time, the system will go back to equilibrium. All well in good.

2. Now let us consider a very long recombination time. What are the non-equilibrium electrons in the conduction band doing? Do they relax to the band minima? Are they distributed according to the Fermi function? What is the chemical potential doing? Is it possible to even define a chemical potential here?

Any help with these questions would be appreciated.

Thanks.
 
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BeauGeste said:
Here's the issue I'm trying to wade through:

1. If you excite electrons from valence band to conduction band (with a laser say), you are out of thermodynamic equilibrium. In some recombination time, the system will go back to equilibrium. All well in good.

2. Now let us consider a very long recombination time. What are the non-equilibrium electrons in the conduction band doing? Do they relax to the band minima? Are they distributed according to the Fermi function? What is the chemical potential doing? Is it possible to even define a chemical potential here?

Any help with these questions would be appreciated.

Thanks.

Er.. something with a "long recombination time" would be a semiconductor at room temperature with the band gap small enough to sustain a population of charge career in the conduction band. Isn't this the same thing? If it is, then don't we know a lot already about the behavior of the electrons in the conduction band?

Zz.
 
BeauGeste,

Do they relax to the band minima?

Sure. As long as the band minimum isn't populated then these electrons will relax to the band minimum through electron-phonon interaction. The conduction electron will emit a photon when it relaxes back to the valence band.

Are they distributed according to the Fermi function?

Absolutely not! The Fermi-Dirac distribution function applies only to electrons that are thermally excited.

What is the chemical potential doing? Is it possible to even define a chemical potential here?

The chemical potential doesn't change. It is strictly a function of temperature and not on the level of electron-photon excitement.

Best Regards

modey3
 
I'm afraid that I have to disagree with Modey, because it's all a matter of timescale. In most semiconductors, the interband lifetime is relatively long, on the order of microseconds. However, intraband scattering processes are usually short, having lifetimes on the order of 100 fs or even less. These intraband processes will thermalize the distribution within the band rather quickly, and so you're actually right: they'll reach a quasi-equilibrium distributed according to the Fermi function. In semiconductor lasers, we call this a quasi-Fermi level.
 
I stand corrected. For very long recombination times that makes sense and as you said the Fermi distribution can only apply for small time scales between the excitement and recombination of electrons.

modey3
 

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