Understanding the Schrodinger Wave Equation for Multiple Electrons

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The discussion focuses on understanding the Schrödinger wave equation for multiple electrons, specifically how to interpret the probability density function for two electrons. The equation \(|\psi(r_{1},\theta_{1},\phi_{1},r_{2},\theta_{2},\phi_{2})|^2\) represents the likelihood of one electron being at position \(\vec{r}_1\) while the other is at \(\vec{r}_2\). It is noted that electrons are indistinguishable, complicating the interpretation, especially regarding their spins. If both electrons have the same spin, their spatial wavefunction must be antisymmetric, while opposite spins allow for a symmetric wavefunction. This highlights the importance of spin in determining the behavior of multiple electrons in quantum mechanics.
nobahar
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Hello!
No maths involved. I am just trying to qualitatively understand the Shrodinger wave equation.
So, the square:
(\psi(r,\theta,\phi))^2
is the probability of finding an electron at some distance r, and some angle\theta,\phi from the nucleus. THis is for one elctron. For two electrons, this becomes:
(\psi(r_{1},\theta_{1},\phi_{1},r_{2},\theta_{2},\phi_{2})^2
What does this mean? Is it saying that, if I choose an electron and place it at r1, theta1... and choose another and place it at r2..., then the probability that the two electrons will be in these places is the equation given above? I could keep one in the same place, and move the other?
Is this correct?
Any help appreciated.
 
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|\psi(r_{1},\theta_{1},\phi_{1},r_{2},\theta_{2},\phi_{2})|^2 is the probability that one of the electrons will be at \vec{r}_1 while the other is at \vec{r}_2.

Your example is slightly complicated by the fact that the electrons are indistinguishable from each other. If the electrons have the same spin, we would not be able to tell one from the other after we've prepared the state. However, by the spin-statistics theorem, if the electrons have the same spin, the spatial wavefunction must be antisymmetric:

\psi(\vec{r}_1,\vec{r}_2) = - \psi(\vec{r}_2,\vec{r}_1).

If the electrons have opposite spins, we can use that to distinguish them and spin-statistics tells us that the spatial wavefunction must be symmetric.
 
Thanks fzero.
 
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