Highly degenerate semiconductor uses

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    Semiconductor
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Discussion Overview

The discussion revolves around the potential applications of a hypothetical material that behaves like a highly degenerate p-type direct gap semiconductor. Participants explore the implications of its properties, particularly its significant p-orbital contribution to the density of states (DOS) at and above the Fermi level, and consider various devices and technologies that could utilize such a material.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant proposes that the material could be useful for ensuring good ohmic contact with metals, but seeks further ideas on its applications.
  • Another participant questions the classification of the material as a semiconductor if its Fermi energy lies deep within the conduction band.
  • A participant notes that the material's direct band gap of around 1.6 eV could make it suitable for LEDs, although the emitted photons would be in the near-infrared range, which may limit its technological interest.
  • One participant suggests that the material might serve as a solid-state laser active medium, considering its emission properties.
  • Another participant mentions that to create useful semiconductors from the material, it may require doping or incorporation into heterostructures.
  • A participant discusses the efficiency of solid-state lasers and the potential for stimulated emission, questioning the effectiveness of optical pumping versus direct electron injection.
  • One participant raises the importance of metastable excited states for lasing and suggests measuring luminescence decay times to compare with established materials like GaAs.
  • Another participant expresses uncertainty about the efficiency of optical pumping and questions the rationale for using the hypothetical material over established semiconductor laser materials.

Areas of Agreement / Disagreement

Participants express a range of ideas and hypotheses regarding the material's applications, with no consensus reached on its potential uses or the effectiveness of various methods for excitation and lasing. Multiple competing views remain regarding the best approach to utilize the material.

Contextual Notes

Participants highlight limitations related to the assumptions about the material's properties, such as the Fermi level position and the implications for its classification as a semiconductor. There are unresolved questions regarding the efficiency of different excitation methods and the conditions necessary for effective lasing.

uncanny_man
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Hello.
"Hypothetically" let's say that I have a material that intrinsically behaves like a highly degenerate p-type direct gap semiconductor (significant p-orbital contribution to the DOS at and above the fermi level). Can anyone think of what in the world such a material may be useful for? I know that such doping is useful for ensuring a good ohmic contact with a metal, but what devices might that be useful for? Keep in mind, this is intrinsically heavily p-type, I didn't dope it to get it that way and so there is no gradient of p-type carrier (which is typically desirable for pn or pin diodes).
Thanks anyone who reads this.
 
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Ah! The wafer spammers have followed me here!
 
If intrinsically it had its Fermi energy lying deep inside the conduction band, it will not be called a semiconductor in the first place.
 
Thats a tough call because, unlike most metallic band diagrams, there is a largish (around 1.6 eV) direct band gap above the the fermi level, valence states, and some of the p-band conduction states. As an intrinsic crystal, it really does more closely resemble the band diagram for a highly degenerate semiconductor than it does a metal, but I'm at a loss as to what such a thing could be useful for...
 
If it has a direct band gap, then it should be good for LEDs. If you can inject electrons above the band gap, you should get plenty of 1.6eV (780 nm) photons coming out. Unfortunately, that is just below red in the near infrared and technologically not all that interesting.
 
Now that's an interesting idea. I had been thinking in terms of absorption, I hadn't been thinking in terms of emission. It might actually be interesting as a solid state laser active medium...
 
GaAs is in the same ball park, and that also has a direct band gap

http://en.wikipedia.org/wiki/Band_gap

However, I am afraid that to make any useful semiconductors out of your mystery compound, you might have to find a way of filling up the valence band (e.g. by doping), or by using it in heterostructures.
 
In terms of a p-n semiconductor laser, I would agree with you. However, what about a solid state laser (probably optically pumped...)? The low fermi level likely won't help the efficiency, but once the population of electrons is inverted, that direct gap should still lead to lazing as the electrons relax back down, shouldn't it? Thanks M Quack, I appreciate being able to bounce ideas off someone.
 
Ideally for lasing you want a metastable excited state so that stimulated emission dominates spontaneous emission. Depending on the matrix elements that might not be the case for a direct band gap - to be checked. For example one could try to optically excite the material (as you propose) and then measure the decay time of the luminescence. Then compare to GaAs or similar materials used in semiconductor lasers. I am not sure if you could directly measure the carrier lifetime as your material should be conducting anyways.

I would imagine that direct injection of electrons is much more efficient than optical pumping. You need a higher photon energy/band gap to excite electrons across the gap. So if you want to pump with a semiconductor source (LED) you need CdTe, AlGaAs or similar. Then you have to ask yourself why do the intermediate step, and why not use AlGaAs as laser material in the first place.

I am not an expert, all these arguments are seat-of-the-pants.
 

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