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[SOLVED] Identical Particles in a 1-D Harmonic Oscillator
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).
How does this sound...
(a) The energy levels for a single particle in a 1-D harmonic oscillator are given by
[tex]E_{n}=\hbar \omega (n+\frac{1}{2})[/tex]
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,
[tex]E_{gnd,tot}=3 \hbar \omega (0+\frac{1}{2}) = \frac{3}{2} \hbar \omega[/tex]
(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, [itex]E_{0}[/itex] has degeneracy 2, and [itex]E_{1}[/itex] has degeneracy 1. The total energy will be,
[tex]E_{gnd,tot}=2 \hbar \omega (0+\frac{1}{2}) + \hbar \omega (1+\frac{1}{2}) = \frac{5}{2} \hbar \omega[/tex]
(c) I have no idea. They behave like two bosons since they're distinguishable?
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
[tex]E_{n}=\hbar \omega (n+\frac{1}{2})[/tex]
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,
[tex]E_{gnd,tot}=3 \hbar \omega (0+\frac{1}{2}) = \frac{3}{2} \hbar \omega[/tex]
(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, [itex]E_{0}[/itex] has degeneracy 2, and [itex]E_{1}[/itex] has degeneracy 1. The total energy will be,
[tex]E_{gnd,tot}=2 \hbar \omega (0+\frac{1}{2}) + \hbar \omega (1+\frac{1}{2}) = \frac{5}{2} \hbar \omega[/tex]
(c) I have no idea. They behave like two bosons since they're distinguishable?