In summary, the conversation discusses the use of geometric measure of entanglement for spin chain systems and its absence in fermionic systems. It is suggested that this is due to the difference in the total Hilbert space structure between the two systems. Some references have explored using Slater wave function to approximate fermionic wave functions and its potential use in measuring entanglement.
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For a system consisting of multiple components, say, a spin chain consisting ofN≥3spins, people sometimes use the so-called geometric measure of entanglement. It is related to the inner product between the wave function and a simple tensor product wave function. But it seems that none used this idea on fermionic systems. Why? Is the reason that for the spin systems, the total hilbert space is a tensor product of the hilbert spaces of each spin, while for identical fermions, the total hilbert has not such a tensor product structure?
 
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After some search, I found a reference using this idea for fermions:journals.aps.org/pra/abstract/10.1103/PhysRevA.89.012504. Their idea is to use the Slater wave function to approximate a given fermionic wave function. They mentioned that this will provide a geometric measure of entanglement for identical fermions, but they did not pursue this much further.

Essentially, their idea is that the slater wave function should be considered as un-entangled. Hence, if the wave function is close to a Slater determinant, then the fermions are weakly entangled. Quantitatively, the distance is measured by the inner product of the best Slater determinant and the given wave function.
 

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