Indirect absorption processes -

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Discussion Overview

The discussion revolves around the concept of indirect absorption processes in solid-state physics, particularly focusing on the relationship between energy, wavevector, and photon transitions in band structures. Participants explore the implications of these concepts in the context of electron transitions between the valence and conduction bands, as well as the role of crystal momentum.

Discussion Character

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

Main Points Raised

  • One participant expresses confusion regarding the indirect absorption process, questioning how energy and wavevector conservation applies to photon transitions between bands.
  • Another participant clarifies that different states in a band can have varying energies and wavevector components, emphasizing the importance of understanding the band structure in three dimensions.
  • A later reply discusses the distinction between photon wavevectors and electron wavevectors, noting that while energy may match, the wavevector does not, necessitating additional mechanisms like phonon interactions for momentum transfer.
  • Participants mention that Bloch waves are not eigenstates of the momentum operator, leading to the concept of quasimomentum for electrons in crystals.
  • There is a suggestion that the conservation of crystal momentum differs from usual momentum, with implications for how forces act on electrons in a periodic lattice.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the relationship between photon and electron wavevectors, with ongoing questions about how these concepts interact in the context of indirect absorption processes.

Contextual Notes

Participants highlight the complexity of band structures and the necessity of considering multiple quantum numbers due to crystalline symmetries. There is an acknowledgment of the limitations in understanding the full implications of these concepts without further detail.

_Andreas
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Indirect absorption processes -- need help!

On page 188-190 in Introduction to Solid State Physics by C. Kittel, I read

In the indirect absorption process ...the minimum energy gap of the band structure involves electrons and holes separated by a substantial wavevector kc. Here a direct photon transition at the energy of the minimum gap cannot satisfy the requirement of conservation of wavevector, because photon wavevectors are negligible at the energy range of interest.

I don't get it. I thought it was as simple as this: the highest point in the valence band and the lowest point in the conduction band have two different energies, and they therefore have two different wavevectors (this is because different energies gives different wavenumbers). The energy difference is E, and therefore the least energetic photon possible of exciting an electron from the valence band to the conduction band must have this energy. But according to the above quote, the energy of the photon is enough, but not the magnitude of the wavevector. This leads me to think that the photon wavenumber is different from a matter wave wavenumber, which is 2pi/lambda. Is this correct?
 
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The different states in a band may have different energies but also other differences like the components of the wavevector.

The picture below shows the band diagram for Si:
si_banddiagram.gif

For full explanations see: http://www.tf.uni-kiel.de/matwis/amat/semi_en/kap_2/backbone/r2_1_5.html.

Just observe that the x-axis is the wave vector.
The various curves correspond to different directions of the wavector (this is a 3D topic!).
The picture indicates the band gap, and you can guess the two bands shown ont heis because above and below the band gap.
It is clear that these two bands are made of states with different energy but also different wavevectors.

You shoul read the details to understand why and how e-states in solids are characterised by more than 1 quantum number. Basically this is related to the crystaline symmetries: the hamiltonian for an electron does not change for translations compatible with the cristaline symmetry.

Sometimes the bands are represented without the x-axis. In such a representation, some information is lost. This information is not always useful, but for the analysis of photons emissions it is necessary.

Don't ask me for much more detail, I have forgotten 99% of what I have learned long ago.
But I could still go a little bit further.
 
Last edited:
_Andreas said:
But according to the above quote, the energy of the photon is enough, but not the magnitude of the wavevector. This leads me to think that the photon wavenumber is different from a matter wave wavenumber, which is 2pi/lambda. Is this correct?

If you have a look at free electrons, the wavevector is an essential quantity describing the momentum of an electron (\vec p= \hbar \vec k).

Bloch waves are not eigenstates of the momentum operator, so there is just a quasimomentum for crystal electrons, but in principle everything stays the same.
So the dispersion relation (band structure) shows the combinations of energy and momentum, which are allowed for electrons. If you have a look at the photon dispersion relation, you will see, that it is linear (\omega=c k). Compared to the electron dispersion relation, the photon dispersion is almost a vertical line at k=0. Therefore transitions to electron states where k is not 0 need some other mechanism to transfer the needed momentum, but almost no energy. Usually these are phonon processes.

So it's just the usual conservation of (crystal) momentum and energy, but it should be clear, that crystal momentum is not equal to usual momentum.
The change in usual momentum depends on the total force acting on an electron. The change in crystal momentum depends only on external forces, but not on the effects, which arise due to the periodic lattice structure.
 
Last edited:
I think that was helpful, thanks.

So an electron with a particular energy doesn't have the same wavevector (and hence not the same wavenumber) as a photon with the same energy then?
 

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