Ground State Energy Levels of He with Two Identical or Distinguishable Electrons

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Homework Help Overview

The discussion revolves around the ground state energy levels of helium (He) with two electrons, considering two scenarios: when the electrons are treated as identical bosons and when they are treated as distinguishable particles. The participants explore the implications of particle identity on energy levels.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants question the rules governing identical particles, particularly the implications of the Pauli exclusion principle for bosons and fermions. They also discuss the rules for distinguishable particles and the necessity of considering wave functions for each case.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some have suggested writing down the wave functions for both distinguishable and identical particles, while others emphasize the importance of understanding the eigenvalues of energy and the occupancy of these states.

Contextual Notes

There is a noted uncertainty regarding the comparison of energy levels without substituting specific wave functions for helium in each scenario. Participants are navigating the constraints of the problem setup and the definitions of particle identity.

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Homework Statement


Discuss the ground state energy levels of He, if

i) two electrons are identical bosons
ii) two electrons are distinguishable particles (but with same mass and same charge)


Homework Equations


err...


The Attempt at a Solution


well...

i) no change in energy. we notice both electron(fermions) have same energy. even if we change it to boson where the quantum state for both electron are equal (ground state), there'll be no changes?

ii) errr... actually i have no idea! some hint please?
 
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i.) What are the rules for identical particles? I.e. what does the Pauli exclusion say about bosons and fermions? What's different for the two?

ii.) What are the rules for distinguishable particles?

Basically you should start by thinking about the wave functions for these cases.
 
Feldoh said:
i.) What are the rules for identical particles? I.e. what does the Pauli exclusion say about bosons and fermions? What's different for the two?

ii.) What are the rules for distinguishable particles?

Basically you should start by thinking about the wave functions for these cases.

Hm.. I was thinking of:
1. write down both formula for distinguishable, fermions & bosons

[tex]\psi \left( r_{{1}},r_{{2}} \right) =\psi_{{a}} \left( r_{{1}} \right) \psi_{{b}} \left( r_{{2}} \right)[/tex]

and

[tex]\psi \left( r_{{1}},r_{{2}} \right) =1/ \sqrt {2} \left( \psi_{{a}}<br /> \left( r_{{1}} \right) \psi_{{b}} \left( r_{{2}} \right) +\psi_{{a}}<br /> \left( r_{{2}} \right) \psi_{{b}} \left( r_{{1}} \right) \right)[/tex]

2. Then I use [tex]H\psi=E\psi[/tex] to get the energies?

However I notice it's quite impossible to compare directly (ie without substituting the wavefunction for He). Am I wrong, or it's a must to substitute wavefunction for each case to compare?
 
You don't need to know the exact states, what you need to know are what particles can be in any given eigenvalue of the energy, and how many can be in the same eigenvalue.
 

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