Excitons: Opposite Movements of Bound Electron-Hole Pairs

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Discussion Overview

The discussion centers on the movement of excitons, which are bound electron-hole pairs, and the relationship between the velocities of free electrons in the conduction band and holes in the valence band. Participants explore the implications of crystal momentum and the nature of excitons in semiconductors, addressing common confusions regarding their behavior.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that the velocity of the hole is not opposite to that of the electron, arguing that they represent two sides of the same phenomenon.
  • Others argue that the group velocity of the exciton can be derived from the dispersion relations of the bands, suggesting that both the electron and hole have the same velocity despite having opposing crystal momentum.
  • A participant questions the application of a simple one-particle picture to excitons, asserting that it fails to capture the nature of bound states and the total momentum of the exciton.
  • Another participant emphasizes the distinction between valence electrons and valence holes, explaining that while the exciton moves together, the valence electrons associated with the holes move in the opposite direction.
  • One participant provides an analogy comparing the movement of a valence-hole to an air bubble in water, illustrating the relationship between the hole and the surrounding valence electrons.
  • Another participant shares an image to clarify their point, indicating that the electron and hole appear to move in opposite directions according to their representation.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between the movement of electrons and holes, with no consensus reached on the interpretation of their velocities and the implications for excitons.

Contextual Notes

Participants note that the discussion involves complex concepts related to crystal momentum, band structure, and the nature of excitons, which may not be fully resolved in the current exchange.

hokhani
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How a bound electron-hole pair (exciton) can move together while the velocity of the free electron in the conduction band is opposite to that of the corresponding hole in the valence band?
 
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This is kind of a common confusion as it is hard to keep track of all the signs when discussing electrons and holes.
It turns out that the velocity of the hole is not opposite to the one of the electron. It also obviously cannot be as considering an electron and a hole picture are two sides of telling the same story.

The group velocity is defined as proportional to the derivative of the energy with respect to the crystal momentum:
v_g=\frac{1}{\hbar}\frac{d E}{d k}.

When you excite an electron from a full valence band to the conduction band, it will have momentum k. The valence band (and therefore the hole) will be left with a momentum of -k, so electron and hole have opposing crystal momentum. However, also the dispersions of the bands are different. Putting zero for simplicity between the two bands and assuming the parabolic approximation, you will find that both dispersions will be almost the same, but differ by the sign, so E_h=-E_e.

Plugging both into the equation for the group velocity, you find that both E and k change sign and therefore the velocity is the same for both and does not change. Other quantities, like effective mass indeed change their sign.

As a second comment, in semiconductors excitons are quite delocalized anyway and the crystal momentum and the velocity of electrons and holes change quite often.
 
Many thanks.
Please look at this picture.
http://postimg.org/image/kgr5cbpev/
Suppose the electron at k is excited from the valence band to the conduction band. According to the picture if we attribute hole to the electron in the valence band at -k, free electron and hole are moving in the same direction but we consider the empty place as hole which is moving in opposite direction compared to free electron.
could you please help me if I am wrong?
 
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The picture does not show up.

But according to your comment, you want to apply the simple one-particle picture to excitons. This is doomed to failure. If you excite an exciton, you do not create a free electron with momentum k and a free hole with opposite momentum, but you create a bound pair of these with total momentum k given by your excitation conditions. It is like having one process creating hydrogen and a second process creating free protons and electrons. These are very different things. Expressing a genuine two-particle state in a single-particle basis will most often go wrong.

On the other hand, you can excite free electrons and holes which may afterwards lose energy and form excitons. But in this case the electron/hole created by one photon are not necessarily the ones which will form the exciton.

It is unfortunate that some books tend to draw the exciton dispersion and the free electron hole dispersion into one graph as that may lead to misunderstandings. The book of Pelant and Valenta (luminescence spectroscopy of semiconductors) gives a good summary of why that is so.
 
Excuse me. I edit my last post sending the image. However I attached it here.
 

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Cthugha said:
On the other hand, you can excite free electrons and holes which may afterwards lose energy and form excitons. But in this case the electron/hole created by one photon are not necessarily the ones which will form the exciton.
By this, do you mean that my earlier comment (according to the picture) is correct?
 
hokhani said:
By this, do you mean that my earlier comment (according to the picture) is correct?

I think that you are conflating the valence-electrons with the valence-hole.

The valence-electron is not the same as the valence-hole. The valence-electron moves in the opposite direction the corresponding valence-hole. The kinetic-energy of the valence-hole is the negative of the energy of the valence-electron relative to the top of the valence-band.

In an energy-level schematic, the valence-hole smiles :-) while the valence-electron frowns :-( If you see the valence-band turned down, then this is a valence-electron band. If you see the valence-band turned up, it is a valence-hole band.

The picture of the exciton is of a conduction electron bound to a valence-hole. The conduction-electron and valence-hole have to travel together. However, the valence-electrons corresponding to the valence-hole are moving in the opposite direction.

The valence-electrons are tunneling from one atom to the other. The hole is really the gap in the valence-orbital, not the electron. So the valence-hole is traveling in the opposite direction.

It is like watch a air bubble under water. If the air bubble goes right, the water near the bubble is going left. If the air bubble goes up, the water near the air bubble is going down. The valence-hole is like the air of the bubble, and the valence-electron is like the water near the air bubble.
 
In the attached file, I showed two equivalent pictures; one in the real space and the other in the k-space. According to the picture you can see that electron and hole are moving in opposite directions.
 

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