Identical Particles in a 1-D Harmonic Oscillator

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SUMMARY

The discussion focuses on determining the energy and degeneracy of the ground state for three particles in a 1-D harmonic oscillator potential under different conditions: identical bosons, identical fermions, and distinguishable particles. For identical bosons, the total energy is E_{gnd,tot} = \frac{3}{2} \hbar \omega with a degeneracy of 3. For identical fermions, the total energy is E_{gnd,tot} = \frac{5}{2} \hbar \omega with a degeneracy of 2 for the ground state. The case of distinguishable particles requires careful consideration of their states and spins, leading to a degeneracy of 2 for the ground state.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the 1-D harmonic oscillator.
  • Familiarity with the Pauli Exclusion Principle and its implications for fermions.
  • Knowledge of particle statistics, specifically the differences between bosons and fermions.
  • Basic grasp of quantum state degeneracy and how it applies to multi-particle systems.
NEXT STEPS
  • Study the mathematical formulation of the 1-D harmonic oscillator in quantum mechanics.
  • Explore the implications of the Pauli Exclusion Principle in multi-particle systems.
  • Learn about the statistical mechanics of bosons and fermions, focusing on their respective distributions.
  • Investigate the concept of degeneracy in quantum systems and how to calculate it for various configurations.
USEFUL FOR

Students and professionals in physics, particularly those focusing on quantum mechanics, particle physics, and statistical mechanics. This discussion is beneficial for anyone looking to deepen their understanding of particle behavior in quantum systems.

logic smogic
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[SOLVED] Identical Particles in a 1-D Harmonic Oscillator

Homework Statement


Three particles are confined in a 1-D harmonic oscillator potential. Determine the energy and the degeneracy of the ground state for the following three cases.

(a) The particles are identical bosons (say, spin 0).
(b) The particles are identical fermions (say, spin 1/2).
(c) The particles are distinguishable spin 1/2 particles but have the same mass (e.g. a proton and a neutron).

The Attempt at a Solution


How does this sound...

(a) The energy levels for a single particle in a 1-D harmonic oscillator are given by

E_{n}=\hbar \omega (n+\frac{1}{2})

Since bosons can all occupy the same state, I presume they will. Therefore they will all be in the ground state with degeneracy 3. The energy will just be three times the ground state energy for one particle,

E_{gnd,tot}=3 \hbar \omega (0+\frac{1}{2}) = \frac{3}{2} \hbar \omega

(b) Because of the Pauli Exclusion Principle, more than one fermion cannot occupy the same state. Therefore, there will be two particles in the ground state (one spin-up, one spin-down), and one particle in the first excited state.

Hence, E_{0} has degeneracy 2, and E_{1} has degeneracy 1. The total energy will be,

E_{gnd,tot}=2 \hbar \omega (0+\frac{1}{2}) + \hbar \omega (1+\frac{1}{2}) = \frac{5}{2} \hbar \omega

(c) I have no idea. They behave like two bosons since they're distinguishable?
 
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Would you really say having three identical bosons in the ground state was threefold degenerate? I wouldn't. They are indistinguishable. Rethink your degeneracy numbers. For c) fermi exclusion only applies between identical particles. You have two of one type and one of the other.
 
Dick said:
Would you really say having three identical bosons in the ground state was threefold degenerate? I wouldn't. They are indistinguishable. Rethink your degeneracy numbers. For c) fermi exclusion only applies between identical particles. You have two of one type and one of the other.

a.) Oh, I think I see. I was thinking of degeneracy wrong? It refers to the number of possible states with a particular energy, not the number of particles occupying a specific energy level, right? How would I go about determining the degeneracy of a system like this? (of course, I'll do the work - I'm just not sure what I'm supposed to do..)

c.) Well, presumably all three are distinguishable (say an electron, proton, and neutron). So I treat them as three noninteracting particles in a harmonic oscillator?
 
For a) I would say the degeneracy is 1. There's only one ground state possibility. For c), yes, I think all three distinguishable. How many different ground states (think spin)? Also rethink b).
 
So (a) is one since they will all be in the same state. But (c) will be E_{0} has degeneracy 2, since they will each be in the ground state, but each can either be up or down (or since the Hamiltonian is just a superposition of the different individual particles Hamiltonians, is it (3!=6)?).

As for (b), I'm changing my answer to E_{0} has degeneracy 2 and E_{1} has degeneracy 2 (both can be occupied, and both have spin-up, spin-down options).

PS And thanks Dick! This is really instructive.
 
Think about b) again. You don't count degeneracies for each level and add them! You have to figure out how many different versions of the ground state there are. The E0 state will have two opposite spin fermions. There's only one way to do that! For c), I think you have the right picture but 3 particles with a choice of up/down does NOT give you 3! possibilities.
 
Wow, Logic Smogic, I had this same exact question on my final yesterday, the 13th. I wish I had seen this post beforehand. You don't happen to attend UPenn, do you? I think you'd make the ultimate study partner.
 

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