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Physics LibreTexts

9.1: Introduction

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Quantum mechanics allows us to predict the results of experiments. If we conduct an experiment with indistinguishable particles a correct quantum description cannot allow anything which distinguishes between them. For example, if the wavefunctions of two particles overlap, and we detect a particle, which one is it? The answer to this is not only that we don’t know, but that we can’t know. Quantum mechanics can only tell us the probability of finding a particle in a given region. The wavefunction must therefore describe both particles. The Schrödinger equation is then:

[22m(21+22)+V(r1)+V(r2)]Φ(r1,r2)=EΦ(r1,r2)

where the subscripts label each particle, and there are six coordinates, three for each particle. Φ is a wave in six dimensions which contains the information we can measure: the probability of finding particles at r1 and r2, but not what we can’t measure: which particle is which.

What basis states would be appropriate for Φ? An approximation is to use a product such as Φ(r1,r2)=|a(r1)b(r2) where a(r1) and b(r2) are one-particle wavefunctions of atoms 1 and 2. This allows us to separate the two particle equation into two one particle equations:

[22m21+V(r1)]|a(r1)=E1|a(r1);[22m22+V(r2)]|b(r2)=E2|b(r2)

provided that the particles do not interact (n.b 21 does not act on b(r2)).

Unfortunately, by doing this we have introduced unphysical labels to the indistinguishable particles. And this is wrong: the effect of it is that the particles do not interfere with each other because they are in different dimensions (six dimensional space - remember?). When we construct a twoparticle wavefunction out of two one-particle wavefunctions we must be ensure that the probability density (the measurable quantity |Φ|2) is independent of the artificial labels.


This page titled 9.1: Introduction is shared under a CC BY 4.0 license and was authored, remixed, and/or curated by Graeme Ackland via source content that was edited to the style and standards of the LibreTexts platform.

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