Sum of two slater determinants

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Discussion Overview

The discussion revolves around the properties and implications of Slater determinants in the context of fermionic wave functions. Participants explore whether the sum of two Slater determinants can be expressed as a new Slater determinant and the conditions under which this might be possible.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that a Slater determinant provides an antisymmetric wave function for fermions.
  • One participant suggests that if all the orbitals in the two Slater determinants are orthogonal, then their sum can be expressed as a new Slater determinant.
  • Another participant asserts that while the product of two Slater determinants can be expressed as a new Slater determinant, the sum cannot, as it may not retain antisymmetry.
  • A participant mentions that a general antisymmetric wave function can be represented as a linear combination of Slater determinants, although this may complicate the total spin of the particles.
  • It is noted that there are cases, such as certain two-electron wave functions, that cannot be expressed in Slater product form, indicating limitations in the applicability of Slater determinants.
  • Some participants express uncertainty about the practical need for summing two different Slater determinants, questioning the scenarios in which this would be desirable.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether the sum of two Slater determinants can be expressed as a new Slater determinant. Multiple competing views remain regarding the conditions under which this might be possible and the implications of such representations.

Contextual Notes

Limitations include the dependence on the orthogonality of orbitals and the specific conditions of the systems being discussed. The discussion also highlights unresolved aspects regarding the preservation of total spin eigenstates and the nature of wave functions that cannot be decomposed into Slater functions.

wdlang
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a slater determinant gives an asymmetric wave function for fermions

is the inverse right?

i.e., can the wave function of some fermions always be written in the form a slater determinant?

To make things concret, can the sum of two slater determinants be put into the form of a new slater determinant?
 
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i guess if all the orbits in the two slater determinants are orthogonal to each other, then the sum of the two can be put into a new slater determinant.
 
wdlang said:
i.e., can the wave function of some fermions always be written in the form a slater determinant?

Yes.

To make things concret, can the sum of two slater determinants be put into the form of a new slater determinant?

The product, yes. The sum, no, because it's not necessarily antisymmetric any more to begin with.
I'm not sure why you'd want to form a sum of two different wavefunctions though.
 
If it is expressed in product form of orbitals, a general anti-symmetric wave function could be written as a linear combination of slater determinants. This will normally mess up the total spin of the particles, but you get anti-symmetry which is good. For N particles you have 2^N spinor (anti-symmetric) eigen states to take a linear combination of.
 
per.sundqvist said:
If it is expressed in product form of orbitals, a general anti-symmetric wave function could be written as a linear combination of slater determinants. This will normally mess up the total spin of the particles, but you get anti-symmetry which is good. For N particles you have 2^N spinor (anti-symmetric) eigen states to take a linear combination of.

Hmm sorry, I meant that a single slater determinant does not necessary preserve the total spin eigenstate, but that you can obtain such if you take a proper linear combination of the slater determinants (alpha, beta spinor functions). Generally you don't need Slater determinants to obtain anti-symmetry, but it could be easier. Also, there exist cases where you could find exact solutions of the two-electron wave function (harmonic oscillator) which is not of the slater product form, but F(r)*G(R) (center of mass R, and relative coordinate r). Clearly this cannot be decomposed into slater functions. It is also common to use extended sums of Slater orbitals in order to reduce the correlation problem.
 
per.sundqvist said:
Hmm sorry, I meant that a single slater determinant does not necessary preserve the total spin eigenstate, but that you can obtain such if you take a proper linear combination of the slater determinants (alpha, beta spinor functions). Generally you don't need Slater determinants to obtain anti-symmetry, but it could be easier. Also, there exist cases where you could find exact solutions of the two-electron wave function (harmonic oscillator) which is not of the slater product form, but F(r)*G(R) (center of mass R, and relative coordinate r). Clearly this cannot be decomposed into slater functions. It is also common to use extended sums of Slater orbitals in order to reduce the correlation problem.

Yes, thank you for your good example.

It is a shame that i do not understand you well
 
alxm said:
Yes.



The product, yes. The sum, no, because it's not necessarily antisymmetric any more to begin with.
I'm not sure why you'd want to form a sum of two different wavefunctions though.

If the sum of two different slater determinant can be made into the form of a single slater determinant, it is a desirable thing, isn't it?
 
wdlang said:
If the sum of two different slater determinant can be made into the form of a single slater determinant, it is a desirable thing, isn't it?

What I meant was that I'm not quite sure what kind of system/situation you'd have to need/want to form the sum of two Slater-determinant wavefunctions. It'd mean the two Hamiltonians are independent. So why merge them?
 

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