Photon absorption by electrons at opposite k-points

In summary, the transition of an electron from the valence to conduction bands can change its momentum due to the opposite group velocities in these bands. The direction of radiation plays a crucial role in determining the transition, as it can change the electron's group velocity. However, the momentum of a photon is too small to significantly affect the crystal momentum of the electron. This is demonstrated by the Moessbauer effect, where the crystal's large mass absorbs the momentum from the photon. Additionally, when an electron is excited by a photon, it jumps almost vertically in the E-k diagram, with its effective mass changing from negative to positive. Finally, while the hole effective mass is negative, this is not the case for an electron still in the
  • #1
hokhani
483
8
Transition of an electron from the valence to conduction bands (direct transition at a k-point near the band edge) would change the momentum of electron because the sign of the group velocity in valence and conduction bands are opposite. Could one infer that the direction of radiation is a determining factor in the transition? In other words, by radiating light from a specific direction, if we have transition at k we can not have the same transition at -k because if the radiation could change the group velocity at k from v to -v, it would change the group velocity at -k from -v to -2v while according to band structure the transition at -k requires changing from -v to v!
 
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  • #2
How large is the momentum of a photon compared to the size of the Brillouin zone?
 
  • #3
M Quack said:
How large is the momentum of a photon compared to the size of the Brillouin zone?
The momentum of photon is too small to change the crystal momentum of electron but it changes the real momentum of electron because ##v_g={1/\hbar} \nabla_k E## and assuming parabolic valence and conduction bands (with the same effective mass) this formula says that the velocity changes from, say, v to -v in the optical transition.
 
  • #4
The assumption is always that the real momentum is taken up by the whole crystal, which has a huge mass, and therefore the resulting velocity is nothing.
A very good example for this is the Moessbauer effect (OK, photons are absorbed/emitted by the nuclei, but the principle is the same).
 
  • #5
M Quack said:
The assumption is always that the real momentum is taken up by the whole crystal, which has a huge mass, and therefore the resulting velocity is nothing.
A very good example for this is the Moessbauer effect (OK, photons are absorbed/emitted by the nuclei, but the principle is the same).
No, this problem occurs even if we don't suppose the phonon effect.
 
  • #6
When a transition happens that an electron jumps from VB to CB by being excited only by a photon, the electron always jumps almost vertically in the E-k diagram. The momentum conversation is still held though the election velocity direction becomes reverse. But do not forget that its effective mass also becomes from negative into positive. As usual people prefer to use h with bar *k to describe the momentum instead of mv for simplicity. In the way. You just need to check k for the direction of momentum of electron.
 
  • #7
zhanghe said:
But do not forget that its effective mass also becomes from negative into positive.
Thanks. But I don't agree. The hole effective mass is negative (valence band) but it is not true for an electron which is still in the valence band. To describe the behavior of the whole valence band which has lost an electron, we use the hole language and consider a negative effective mass for the hole.
 
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  • #8
hokhani said:
Thanks. But I don't agree. The hole effective mass is negative (valence band) but it is not true for an electron which is still in the valence band.
Well, the m* of hole is positive.
 

Related to Photon absorption by electrons at opposite k-points

What is photon absorption by electrons at opposite k-points?

Photon absorption by electrons at opposite k-points refers to the process in which an electron absorbs a photon and moves from one k-point to the opposite k-point in a material's energy band structure. This phenomenon is a key factor in understanding the electronic properties of materials and is often studied in the field of condensed matter physics.

How does photon absorption by electrons at opposite k-points occur?

Photon absorption by electrons at opposite k-points occurs when an electron in a material absorbs a photon with enough energy to move from one k-point to the opposite k-point in the material's energy band structure. This process is governed by the laws of quantum mechanics and is essential for understanding the electronic behavior of materials.

What are k-points in the context of photon absorption by electrons?

In condensed matter physics, k-points refer to specific points in the Brillouin zone of a material's energy band structure. These points represent the allowed energy states for electrons in the material. In the context of photon absorption, k-points play a crucial role in determining the energy and momentum of the absorbed photon and the resulting movement of the electron.

What are the applications of studying photon absorption by electrons at opposite k-points?

Understanding photon absorption by electrons at opposite k-points has many important applications in the fields of materials science and technology. It can help researchers design new materials with specific electronic properties, improve solar cell efficiency, and develop new technologies such as quantum computing and optoelectronics.

Are there any challenges in studying photon absorption by electrons at opposite k-points?

Yes, there are several challenges in studying photon absorption by electrons at opposite k-points. These include accurately measuring and controlling the energy and momentum of photons, understanding the complex interactions between electrons and photons, and developing theoretical models that can accurately predict these processes in different materials.

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