Still confused about (anti)symmetrization of wavefunctions

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Discussion Overview

The discussion centers around the anti-symmetrization of wavefunctions in quantum mechanics, particularly in the context of many-fermion systems and their implications for quantum chemical theories. Participants explore the challenges and methodologies associated with anti-symmetrization, questioning the validity of certain wavefunctions used in theoretical models.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant expresses confusion about how to anti-symmetrize wavefunctions, noting that the wavefunctions in question lack information necessary for this process.
  • Another participant questions whether the wavefunctions discussed could already be considered anti-symmetrized, suggesting that many quantum chemical theories would be invalid if anti-symmetrization is not accounted for.
  • Concerns are raised about the practical difficulties of anti-symmetrization, especially for larger molecules, and the potential for alternative methods to simplify the process.
  • One participant requests examples of non-anti-symmetrized wavefunctions being successfully used in many-fermion systems, emphasizing the necessity of the Pauli principle in understanding atomic and molecular structures.
  • Another participant references a specific paper that uses wavefunctions for singlet excited states, arguing that these wavefunctions cannot be anti-symmetrized due to insufficient information, which raises questions about the validity of the theories presented in that paper.

Areas of Agreement / Disagreement

Participants express differing views on the necessity and feasibility of anti-symmetrization for certain wavefunctions. There is no consensus on whether the wavefunctions discussed can be considered valid representations of molecular states without anti-symmetrization.

Contextual Notes

Participants highlight limitations related to the lack of information in the wavefunctions discussed, which complicates the anti-symmetrization process. There are unresolved questions about the applicability of certain quantum chemical theories if anti-symmetrization is not performed.

HAYAO
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I am currently confused about anti-symmetrization of wavefunctions. In a thread "Still confused about super position and mixed state", kith responded that anti-symmetrization was not done thus the none of the bras and kets shows any properties of a possible state of a molecule I have mentioned in the thread OP.

1) So then how can it be done? The wavefunctions used in the problem has no information about what kind of equation it is composed of. So we have no way of knowing how to anti-symmetrize the wavefunctions.

2) Couldn't the wavefunctions used in the thread be considered as wavefunction that have already been antisymmetrized? Otherwise, quite some quantum chemical theories (such as spin-orbit coupling, excitonic interactions, ligand field, etc.) would fails because most textbooks and papers regarding these theory typically don't consider antisymmetrization or at least don't mention it.

3) Practically, how is anti-symmetrization done in general? It seems to me that anti-symmetrization is a tedious work considering how many electrons are included in a molecule. Both Antisymmetrizer and Slater determinants seems to be tons of work. Are there any way to come around this tremendous amount of work?
 
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vanhees71 said:
Have a look at this

https://en.wikipedia.org/wiki/Slater_determinant

This explains the basics about antisymmetrization in the context of wave mechanics.

Yes, and I am well aware of this.

I am, however, not aware of the actual calculation when handling relatively larger molecules. For example, mathematically, no analytical solution is available for Slater determinants for matrix over 4x4 unless in special cases (no formula is available if my memory is right). But typical organic molecules surely have electrons over 4.

The specific case I have presented above is a general representation of excitonic interaction. So each of the wavefunctions presented in the thread shouldn't be able to be anti-symmetrized due to lack of information. Despite this, kith has responded that none of the wavefunction can actually represent a molecule. That means it is absolutely impossible to generalize any quantum chemical theory. But the fact is, there are tons of famous theory that uses wavefunction that is not defined specifically (thus antisymmetrization is not possible). If kith is right, then all these theory cannot be true. I feel that there is some contradiction or confusion here that I need clarification of.
 
Ok, can you point me to a concrete example, where non-antisymmetrized wave functions for many-fermion systems are successfully used? For atomic and molecular structure, for sure the Pauli principle is mandatory. How else can one, e.g., understand the periodic table of elements?
 
vanhees71 said:
Ok, can you point me to a concrete example, where non-antisymmetrized wave functions for many-fermion systems are successfully used? For atomic and molecular structure, for sure the Pauli principle is mandatory. How else can one, e.g., understand the periodic table of elements?

For example, page 2491 of http://www.itc.univie.ac.at/~wichard/JCP120_2490.pdf from Journal of Chemical Physics uses wavefunction \left | S_{i_{A}} \right \rangle and \left | S_{j_{B}} \right \rangle for singlet excited state of molecule A and B. These two wavefunction is clearly a general representation of unknown molecules A and B, and thus there is no way to antisymmetrize this. We lack the information of the actual wavefunction to antisymmetrize. I always althought that these wavefunctions are used under the premise that they are already antisymmetrized but according to kith's post, he argues otherwise.

Of course, I am well aware of the Pauli principle and its importance. That is why I was extremely confused when kith pointed out that none of the wavefunction used in the thread I've mentioned in OP represent any of the state of the molecules mentioned. Because if what kith said is true, then the paper I mentioned above is already wrong starting from the premise.
 

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