# Does the symmetrization of the wave function change the energy?

Suppose two non interacting electrons, in a time independent potential, described by the equation:

$$$${H} \psi(r_1, r_2) = \frac{-\hbar^2}{2m} (\nabla^2_1 + \nabla_2^2) \psi(r_1, r_2) + V(r_1) \,\psi + V(r_2) \,\psi = E$$$$ We can separate this equation supposing $$\psi(r_1, r_2) = \psi_1(r_1) \psi_2(r_2)$$. In the process of solving we get $$E = E_1 + E_2$$, so:

$$$$H \psi_1(r_1) \psi(r_2) = (E_1 + E_2)\psi_1(r_1) \psi(r_2) = E\psi_1(r_1) \psi(r_2)$$$$

Now if I say that the total wave function must be antisymmetric, I can combine both solutions:

$$\psi_{TOTAL} = \frac{1}{\sqrt{2}}[\psi_1(r_1) \psi_2(r_1) - \psi_2(r_1) \psi_1(r_2)]$$

But now, this wave function is not necessarily an eigenvector of $$H$$, so does writing the wave function like this change the energy of the total state? I know the first term of the total wave function is eigenvector of $$H$$, but the second one not, so what are the possibles energies for this system?

In your particular case where you consider separable wave functions (Hamiltonian has your particles non-interacting), I don't get why you say that the form $$\psi_{TOTAL} = \frac{1}{\sqrt{2}}[\psi_1(r_1) \psi_2(r_1) - \psi_2(r_1) \psi_1(r_2)]$$ is not necessarily a solution.

Indeed, this is just a linear combination of Hartree products of one-electron wavefunctions. You were OK to accept those procuts individually as a solution, so why would a linear combination not be?

Plus, if you do understand that $$<\psi_1(r_1) \psi(r_2)| H |\psi_1(r_1) \psi(r_2)> = E_1 + E_2 = E$$, you can check very easily what is going on for your slater determinant: $$H |\psi_1(r_1) \psi_2(r_2)-\psi_2(r_1) \psi_1(r_2)> = H |\psi_1(r_1) \psi_2(r_2)> -H |\psi_2(r_1) \psi_1(r_2)>$$ $$= (E1+E2)|\psi_1(r_1) \psi_2(r_2)> - (E1+E2)|\psi_2(r_1) \psi_1(r_2)> = E |\psi_1(r_1) \psi_2(r_2)-\psi_2(r_1) \psi_1(r_2)>$$

so that $$<\psi_{TOTAL}|H|\psi_{TOTAL}>=E$$, giving you the same Energy

EDIT: To see that the exchanged product yields the same value, consider that you can spearate your Hamiltonian in two: $$H=H_1+H_2$$ where $$H_i= \frac{-\hbar^2}{2m} \nabla^2_i + V(r_i)$$ each of those hamiltonian acts only on one particle so you have: $$H |\psi_1(r_1) \psi_2(r_2)> = (H_1 |\psi_1(r_1)>)\otimes|\psi_2(r_2)> + \psi_1(r_1)> \otimes (H_2 |\psi_2(r_2)>)$$ with $$H_1 |\psi_1(r_1)>=E_1|\psi_1(r_1)>$$ and $$H_2 |\psi_2(r_2)>=E_2|\psi_2(r_2)>$$

Now, you can realize that the two hamiltonians are the same, only they are acting on different particles. Right? So if you have $$H_1 |\psi_1(r_1)>=E_1|\psi_1(r_1)>$$, you MUST have $$H_2 |\psi_1(r_2)>=E_1|\psi_1(r_2)>$$ because H1 and H2 are those same hamiltonians (only acting on r1 or r2), and give the same eigenvalue for the same eigenvector. Therefore: $$H|\psi_2(r1)\psi_1(r2)>=(H_1 |\psi_2(r_1)>)\otimes|\psi_1(r_2)> + \psi_2(r_1)> \otimes (H_2 |\psi_1(r_2)>)$$ $$=E_2 |\psi_2(r_1)>\otimes|\psi_1(r_2)> + E_1\psi_2(r_1)> \otimes |\psi_1(r_2)>=(E_1+E_2)|\psi_2(r_1)\psi_1(r_2)>$$

• I know it is a solution, my question was if it was a solution with the same eigenvalue. The point of confusion is because I can't see why $H \psi_2(r_1) \psi_1(r_2) = E_2 +E_1$. If I only know the case with changed coordinates. Commented Nov 1, 2019 at 4:04
• Ask yourself why you accepted in the first place that $\psi_1(r_1) \psi_2(r_2)$ was an eigenvector of H with eigenvalue $E_1+E_2$. The same line of thought should lead you to accept the same for the exchanged wavefunction, since the Hamiltonain is the same for both particles. On a side note, you are writing your eigenvalue relationship wrong; the hamiltonian does not reduce a wavefunction to a real value Commented Nov 1, 2019 at 4:14
• I supposed that I solved the equation and found out, now if you solve for the other case why would you get the same Commented Nov 1, 2019 at 4:15
• In the process of separating variables, whe define two constans, in the end we get that $E$ is the sum of both. Commented Nov 1, 2019 at 4:17
• edited to answer by separating the hamiltonian Commented Nov 1, 2019 at 4:39