Fermi energy of multiple electrons, infinite potential well

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SUMMARY

The discussion focuses on calculating the Fermi energy level for five free electrons in a three-dimensional infinite potential well with a width of 12 angstroms. The relevant equation used is E = [(h_bar*pi)²/(2*m*a²)]*(nx² + ny² + nz²). Participants clarify that the correct filling of energy states starts from (111), with the first five electrons occupying (111), (112), and (122) states. The confusion arises from the interpretation of the energy state (221) containing both an electron and an empty state, which is clarified by understanding that the quantum numbers start from one.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically the concept of infinite potential wells.
  • Familiarity with the Fermi energy concept and its calculation.
  • Knowledge of quantum numbers and their significance in electron configuration.
  • Proficiency in using the equation E = [(h_bar*pi)²/(2*m*a²)]*(nx² + ny² + nz²) for energy calculations.
NEXT STEPS
  • Study the derivation and implications of the Fermi energy in quantum systems.
  • Learn about the filling of quantum states in multi-electron systems.
  • Explore the concept of degeneracy in quantum mechanics and its effects on energy levels.
  • Investigate the differences in energy state filling for varying numbers of electrons in infinite potential wells.
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Students and professionals in physics, particularly those studying quantum mechanics, semiconductor physics, or anyone involved in calculations related to electron configurations in potential wells.

ricardillo
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Homework Statement


[/B]
Five free electrons exist in a three-dimensional infinite potential well with all three widths equal to a 12 angstroms. Determine the Fermi energy level at T 0 K.

Homework Equations



E = [(h_bar*pi)2/(2*m*a2)]*(nx2 + ny2 + nz2)

The Attempt at a Solution



Tried using EF = (h_bar2/2*m)*(3*pi2*N/V)(2/3) but no luck; found the solution manual online, but the answer doesn't make sense:

"For a 3D infinite potential well,

E = [(h_bar*pi)2/(2*m*a2)]*(nx2 + ny2 + nz2) = E0*(nx2 + ny2 + nz2).

For 5 electrons, energy state corresponding to nx ny nz = 221 contains both an electron and an empty state, so

EF = E0*(22 + 22 + 12)..." (plug in values and solve from here on)

My question is, why does the 221 state "contain both an electron and an empty state"? It seems like the 5 electrons should fill up only the 111 and 211 levels since 111 has room for two states and 211 has room for six.
 
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Can you give the link to the solution you found?
 
Ah ok, sorry I was a bit confused because I forgot that ##n_i## starts from one instead of zero.
ricardillo said:
EF = (h_bar2/2*m)*(3*pi2*N/V)(2/3
This is an approximate formula when the number of electron is very large. For 5 electrons you have to count the possible states one after another starting from the lowest one, which is (111). Neglecting spin, if you have 5 electrons, which level you will end up to if you add the electrons one by one from (111) state?
 
If we include degeneracy, then there's one electron in (111), three in (112) and one in (122) with two states left over at that level. However, if I try the same method for thirteen electrons, as in part (b), I'd only get to level (123) rather than the (233) level given by the solution.
Is there something wrong with the way I'm filling up states?
 
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ricardillo said:
If we include degeneracy, then there's one electron in (111), three in (112) and one in (122) with two states left over at that level. However, if I try the same method for thirteen electrons, as in part (b), I'd only get to level (123) rather than the (233) level given by the solution.
Is there something wrong with the way I'm filling up states?
I am also facing the same problem.
 
Anik Paul said:
I am also facing the same problem.
I don't see how the manual arrived at its solution. The Fermi energy should be at (123).
 

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