Eigenfunction of a system of three fermions

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SUMMARY

The discussion focuses on finding the eigenfunction of the ground state \(\Psi_0\) for a system of three independent fermions with spin \(s=1/2\). The known eigenfunctions \(\phi_{n,s}(x) = \varphi_n(x) \chi_s\) and eigenvalues \(E_n\) of the single particle Hamiltonian are utilized. Due to the Pauli exclusion principle, the configuration must include two particles with opposite spins in the lowest energy level and one particle in the first excited level. The conclusion is that either the Slater determinant of \(\phi_{0,+}(x), \phi_{0,-}(x), \phi_{1,+}(x)\) or \(\phi_{0,+}(x), \phi_{0,-}(x), \phi_{1,-}(x)\) can be used, and it is acceptable to consider linear combinations of the degenerate states for calculations.

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I have to find the eigenfunction of the ground state \Psi_0 of a three independent s=1/2 particle system.

The eigenfunctions \phi_{n,s}(x) = \varphi_n(x) \ \chi_s and eigenvalues E_n of the single particle Hamiltonian are known.

Becuse of the Pauli exclusion principle, there must be two particles with opposite z component of the spin in the lowest energy single particle level and one particle in the first excited single particle level.
I have attempted to solve the problem saying that the eigenfunction \Psi_0 of the three particle system must be either the Slater determinant of ##\phi_{0,+}(x), \phi_{0,-}(x)## and ##\phi_{1,+}(x)## or the Slater determinant of ##\phi_{0,+}(x), \phi_{0,-}(x)## and ##\phi_{1,-}(x)## (two possible excited levels).

Now, my question is: since the particle with higher energy can be both in the state ##\phi_{1,+}(x)## and in the state ##\phi_{1,-}(x)## without any preference, is it fine to consider these two single particle states in order to calculate the two Slater determinants, or should I consider two linear combinations of them (i.e. ##\varphi_1(x) \ (\chi_+ + \chi_-)## and ##\varphi_1(x) \ (\chi_+ - \chi_-)##)?
 
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No, it does not matter. As long as the states are degenerate you may use either combination as a basis.
 

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