When do we use notion of effective mass

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SUMMARY

The discussion centers on the concept of effective mass in the Schrödinger equation, which simplifies the many-body problem of interacting electrons into a series of one-body problems. Effective mass accounts for the coupling of electrons and allows for the treatment of electrons as non-interacting entities within a lattice potential. This transformation is essential for solving complex systems, as it ensures that both the original and modified systems describe the same physical reality by adjusting the mass of the electrons to include interaction effects.

PREREQUISITES
  • Understanding of the Schrödinger equation (SE)
  • Familiarity with many-body quantum mechanics
  • Knowledge of electron interactions and Coulombic potential
  • Concept of potential wells in quantum systems
NEXT STEPS
  • Study the derivation of effective mass in semiconductor physics
  • Explore the implications of effective mass on electronic band structure
  • Learn about the role of lattice potentials in quantum mechanics
  • Investigate the mathematical techniques for solving many-body problems
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Physicists, quantum mechanics students, and researchers in condensed matter physics who are interested in understanding electron behavior in complex systems and the application of effective mass in theoretical models.

amitrt
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If effective mass in Schrödinger equation takes into account for coupling by other bands or so to say by other electrons, and in this way we don't care about effect of other electrons and deal with lattice potential.
 
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amitrt said:
If effective mass in Schrödinger equation takes into account for coupling by other bands or so to say by other electrons, and in this way we don't care about effect of other electrons and deal with lattice potential.

What exactly is the question here ?

Intuitively, effective mass is a concept that uncouples one many body problem into a set of one body problems that are more easu to solve (i mean, of which the Schrödinger equation, ie the SE, is easier to solve).

Suppose you have 100 electrons mutually interacting through a coulombic potential. The SE cannot be solved exactly because of the mutual coupling between all the electrons (electron 1 interacts with electron 2,3, etc). To uncouple this many body system, we convert it into a system where you have "new electrons" interacting in a background potential. So, you look at the problem as if the new electrons are no longer interacting with each other but with some background potential. Since both systems need to be equivalent (ie you need to describe the same physical reality) you need to compare both systems : the original system as mutually interacting electrons, the new system has non interacting electrons in a certain potential well. To make sure that both systems are equivalent, we change the mass of the electrons in the second system, in such a way that both SE are describing the same reality. This new mass is the effective mass, which can be defined as the electron mass + some interactions (ie energy of those interactions) to uncouple the many body problem into many one body problems.

That is the philosophy behind effective mass.

marlon
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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