Effective mass of electrons in metals

Click For Summary
SUMMARY

The discussion centers on the concept of effective mass of electrons in metals and semiconductors, particularly its derivation and applications beyond heat capacity. Effective mass is defined in relation to the curvature of the electronic dispersion relation, represented mathematically as E = hbar^2 k^2 / 2m* for particles in a band. The effective mass (m*) is often lower than the free electron mass (m), which raises questions about the physical implications of this phenomenon, especially in the context of mobility and response to external electric fields.

PREREQUISITES
  • Understanding of solid-state physics concepts
  • Familiarity with electronic band theory
  • Knowledge of fermionic renormalization methods
  • Basic principles of mobility in semiconductors
NEXT STEPS
  • Research the mathematical derivation of effective mass in solid-state physics
  • Explore the implications of effective mass on semiconductor mobility
  • Study the works of Shankar on fermionic renormalization methods
  • Investigate the relationship between effective mass and electronic dispersion relations
USEFUL FOR

Physicists, materials scientists, and electrical engineers interested in the behavior of electrons in metals and semiconductors, particularly in relation to mobility and effective mass concepts.

joel.martens
Messages
15
Reaction score
0
The literature i have on the origins / need for an effective mass of electrons seems only to relate it to the explanation of heat capacity of metals but it seems like the concept has applications far beyond this. Can someone pls provide a more general summary of its derivation and applications?
Cheers.
 
Physics news on Phys.org
Effective mass of holes and electrons in semiconductors is closely related to mobility. See
http://en.wikipedia.org/wiki/Effective_mass_(solid-state_physics )
 
Last edited by a moderator:
The cleanest understanding of effective mass in Fermi liquids comes from a solid understanding of fermionic renormalisation methods. See any number of papers by Shankar on the topic.
 
I think of effective mass as a curvature of the electronic dispersion relation. I.e. for a free electron:
E = hbar^2 k^2 / 2m

where m is the mass of free electron.

Now, in a crystalline solid, where electronic band diagram applies, any band (near a symmetry point) can be represented as parabolic in k space, with its own curvature, i.e.:

E = hbar^2 k^2 / 2m*

where m* is the 'renormalized' mass of an particle in band (electron or a hole).

What is puzzling to me is why in for example semiconductors the effective mass is lower than the free electron mass? If I apply an external electric field, these electrons will reach steady state velocity larger than the free ones... what is physically happening that electron acts as if its inertia is lowered?
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 0 ·
Replies
0
Views
3K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 0 ·
Replies
0
Views
3K
  • · Replies 4 ·
Replies
4
Views
5K
  • · Replies 1 ·
Replies
1
Views
7K
  • · Replies 10 ·
Replies
10
Views
3K