Why is Si indirect semiconductor

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Discussion Overview

The discussion centers around the nature of silicon as an indirect bandgap semiconductor, exploring the underlying reasons for its band structure characteristics. Participants examine theoretical aspects, including band structure diagrams, and the implications of electron and hole behavior in silicon compared to other materials.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants explain that the indirect nature of silicon's bandgap arises because the maximum of the valence band and the minimum of the conduction band occur at different k-vectors, necessitating additional momentum transfer for electron-hole recombination.
  • One participant questions the underlying reasons for the energy band minima occurring at k-values other than zero in silicon, suggesting a need for further exploration of the band structure.
  • Another participant notes that the band structure is influenced by the number of electrons and covalent bonding in silicon, implying that symmetry arguments may not fully explain the indirect bandgap.
  • A participant mentions "stretched silicon," a technique that reduces the indirectness of the bandgap, enhancing silicon's switching speeds by altering its lattice structure during growth on mismatched substrates.
  • There is a suggestion that a qualitative argument using tight binding approximation and kp-perturbation theory could clarify how the valence and conduction bands behave at k=0, contributing to the indirect bandgap nature.
  • Another participant discusses the role of s and p orbitals in determining the band structure, explaining how their interactions lead to the indirect bandgap in silicon.

Areas of Agreement / Disagreement

Participants express various viewpoints on the reasons behind silicon's indirect bandgap, with no consensus reached on a singular explanation. Multiple competing models and theories are presented, indicating an ongoing exploration of the topic.

Contextual Notes

Some discussions involve assumptions about the band structure and the behavior of electrons and holes, which may depend on specific definitions and theoretical frameworks. Certain mathematical steps and implications remain unresolved.

vani_lj
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Can anybody explain...

what makes silicon indirect band semiconductor?

thanks in advance

Vani
 
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Look at the band structure diagram.

http://en.wikipedia.org/wiki/File:Si-band-schematics.PNG
http://en.wikipedia.org/wiki/File:Si-band-schematics.PNG

Find the maximum of the valence band and the minimum of the conduction band.

They are not at the same k-vector.

Holes and conduction electrons will be found near the maximum/minimum. In order for a hole/electron pair to recombine they must "get rid" of the difference in k. An optical photon carries next to no momentum, so some other elementary excitation like a phonon has to be created.

In GaAs on the other hand, min and max occur at the same k. Holes and electrons can recombine and emit just a photon.

The same hold vice-versa for absorption of a photon.
 
@M Quack, thanks for the explanation...

But I am still searching for answer that what makes energy band minima to occur at k other than zero in Si.
 
Hmm, that is just the way the band structure works out with the number of electrons on Si, covalent bonds, and so on. I don't think that you can find an argument based on symmetry.

BTW, Ge and diamond also have indirect band gaps.
 
The "stretched silicon" invented in the 90's reduced the degree of indirectness of the gap and allowed for more efficient silicon switching speeds. The idea was to grow silicon layers on mismatched substrates that were hot. When the wafer cooled, the silicon was stretched into a slightly different lattice constant.
 
I suppose there should be some qualitative argument using e.g. tight binding approximation on how the valence band and conduction band change at k=0 with k using kp-perturbation theory. As both bent downward, the band gap must be indirect.
 
The valence and conduction band are qualitatively due to the s and p orbitals of Si. The s orbitals are lower in energy than p. On the Gamma point, the total bonding-antibonding splitting is larger for s than for p orbitals. Taken together, the lowest valence band has s-character and is well separated from the highest valence band which has pure p character. The mainly anti-bonding p and s type conduction bands are nearly degenerate in energy. Once the Gamma point is left, the kp term will mix s and p bands. The p type valence band and s-type conduction band will repell whence the valence band has a maximum at k=0. On the other hand the s and p type conduction bands will repell even stronger as they are nearly degenerate. Hence the lowest conduction band will also have a maximum at k=0. If we believe in k=0 being the absolute maximum of the valence band then Si has to have an indirect band gap.
 
@DrDu, Thanks for the explanation...
 

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