Ground-state energies of electron gas

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SUMMARY

The discussion centers on the ground-state energies of an N electron system within a cubic volume V, specifically examining two boundary conditions: Dirichlet and periodic. It is established that while the individual energy levels differ based on the boundary conditions, the total ground state energy remains equal when the proper quantum numbers (n1, n2, n3) are applied. This equality arises from the distinct restrictions on the quantum numbers for each boundary condition. Additionally, a correction regarding a missing factor of π² in the energy levels for periodic boundary conditions is noted.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly fermions and their behavior.
  • Familiarity with boundary conditions in quantum systems, specifically Dirichlet and periodic conditions.
  • Knowledge of energy quantization in confined systems, such as particles in a box.
  • Basic mathematical skills to manipulate expressions involving quantum numbers and energy levels.
NEXT STEPS
  • Study the implications of Dirichlet vs. periodic boundary conditions in quantum mechanics.
  • Explore the derivation of energy levels for fermions in a cubic box using both boundary conditions.
  • Learn about the role of quantum numbers in determining the state of a fermionic system.
  • Investigate the significance of factors like π² in quantum mechanical expressions and their physical interpretations.
USEFUL FOR

Students and researchers in quantum mechanics, physicists studying condensed matter systems, and anyone interested in the behavior of fermions in confined spaces will benefit from this discussion.

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I read from a textbook that there are two boundaries conditions that may be used in order to determine the energies of N electron system in a cube of volume V (and side a).
...
(check out the attached file)
...
As you can see in the attached file, the energies got by using the the two boundary condition methods are different.

The textbook however states that these energies are not different but are EQUAL if proper values of n1, n2, n3 are taken. How can that be possible? I just see two different things that cannot be equal here. Please help.

Notice that ni = 1, 2 ,3 , ... in the first boundary condition and
ni = ... -2, -1, -1,0 , 1, 2 ,3 , ... in the second condition.
(i = 1,2,3)
 

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The set of energy levels of the individual states are in fact different for the two different boundary conditions. However, if you put N fermions in the box and calculate the total ground state energy of the system, you will get the same total energy for the two different boundary conditions. This is due to the different restrictions on the values of the n_i's for the different boundary conditions.

(There's a factor of pi^2 missing in your expression for the energy levels for the periodic boundary conditions.)
 
Thanks a lot. I got it.
 

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