Undergrad Electron correlation vs electron exchange

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Electron correlation and electron exchange are distinct concepts in quantum mechanics. Electron exchange arises from the indistinguishability of particles and is linked to their spin, while electron correlation is related to the charge of the particles and their interactions. In a classical framework, non-interacting particles evolve independently, but quantum mechanics introduces effects like the exclusion principle for indistinguishable particles. When charged particles are considered, their evolution becomes interdependent, leading to correlation. The exchange-correlation term unifies these concepts in many-electron systems, with the Hartree product wavefunction serving as a classical approximation and the Slater matrix accounting for exchange symmetry.
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What is difference between electron correlation and electron exchange?
What is the difference between electron correlation and electron exchange?
Which of them is due to the spin of electrons and which is due to charge of electrons?
 
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All of this can be easily understood mathematically using the so-called correlation functions, but I'll try to explain with words.

First, consider two neutral (non interacting) classical particles. In this case the two particles basically ignore each others so the evolution in time of each particle is totally independent (uncorrelated) of the other.

Now let's add a little bit of quantum mechanics: suppose the two particles are now indistinguishable. This is a purely quantum mechanical phenomenon and it changes the system. The two particles are still non-interacting (so their time evolution is still independent from each other) but now you get all the quantum mechanical effects that follow from indistinguishability (ex. exclusion principle). This is roughly the electron-exchange.

Finally suppose the particles are charged. Now the evolution of one particle is dependent of the other in a pretty complicated way and we say the particles are correlated.

Schematically you can think it this way:
classical view + exchange + correlation = real qm description.

In some cases the exchange term and the correlation terms are unified into the so-called exchange-correlation term.
 
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Let me add this:
The most classical approximation to a many electron problem is via a Hartree product wavefunction. To get exchange symmetry, you have to consider all permutations and end up with a Slater matrix. This is the most general wavefunction describing somehow non-correlated electrons (each electron sees only the average field of the other electrons). The fully correlated wavefunction cannot be expressed as a single determinant but only as a (in principle infinite) sum of these. This is called the full CI (configuration interaction) limit.
 
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