Show that the total eigenfunction must be antisymmetric

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SUMMARY

The total eigenfunction for two noninteracting indistinguishable particles must be antisymmetric under particle exchange, as established by the Pauli exclusion principle. The spatial wavefunctions are defined as Ψ(x1,x2) = 1/√2 [ ψA(x1)ψB(x2) ± ψA(x2)ψB(x1)], where the negative sign indicates an antisymmetric wavefunction. This requirement arises from the indistinguishability of the particles, necessitating that swapping the particles results in the negative of the original eigenfunction.

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Homework Statement


[/B]
By considering the eigenfunctions for 2 noninteracting particles at distances r1 and r2,
show that their total eigenfunction must be antisymmetric.
.

Homework Equations



Spatial wavefunctions:

Ψ(x1,x2) = 1/√2 [ ψA(x1B(x2) ± ψA(x2B(x1)]

Where + gives a symmetric wavefunction and - gives an antisymmetric one.




The Attempt at a Solution


[/B]
Hi, not really sure what to do with this one. I know that the Pauli exclusion principle says that the total eigenfunction must be antisymmetric for fermions. But the question doesn't mention fermions, just "2 noninteracting particles". I also know that the antisymmetric spin wavefunctions are associated with the symmetric spatial wavefunctions, and vice versa, to produce a total antisymmetric wavefunction, but I don't get why, which is what the question seems to be asking...

 
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The question is very poorly worded. The wave function is anti-symmetric with respect to what? Bad questions have no good answers :frown:
 
DrClaude said:
The question is very poorly worded. The wave function is anti-symmetric with respect to what? Bad questions have no good answers :frown:

Hi, sorry, I should probably have said a bit more in my OP. Presumably, in the question, the 2 particles are indistinguishable. So it means that eigenfunction must be antisymmetric under particle exchange. ie. that if the particles are swapped, this will give the negative of the original eigenfunction
 

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