msumm21
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If you have 2 identical, noninteracting Fermions in an infinite 1 dimensional square well of width a, I was thinking the state would be:
\frac{1}{\sqrt{2}}\psi_1(x_1)\psi_1(x_2)(\uparrow\downarrow - \downarrow\uparrow )
where \psi_1 is the ground state of the single particle well problem.
However, I just looked in Griffths "Introduction to QM, 2nd Ed" and it says there is no state with the energy of that state and that in fact the ground state is \psi_1(x_1)\psi_2(x_2)-\psi_2(x_1)\psi_1(x_2).
The state I gave seems to be (1) antisymmetric, (2) an eigenstate of the Hamiltonian, and (3) have lower energy than the ground state given by Griffths.
Do you see a problem with ground state I gave?
\frac{1}{\sqrt{2}}\psi_1(x_1)\psi_1(x_2)(\uparrow\downarrow - \downarrow\uparrow )
where \psi_1 is the ground state of the single particle well problem.
However, I just looked in Griffths "Introduction to QM, 2nd Ed" and it says there is no state with the energy of that state and that in fact the ground state is \psi_1(x_1)\psi_2(x_2)-\psi_2(x_1)\psi_1(x_2).
The state I gave seems to be (1) antisymmetric, (2) an eigenstate of the Hamiltonian, and (3) have lower energy than the ground state given by Griffths.
Do you see a problem with ground state I gave?
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