9.1: Introduction
( \newcommand{\kernel}{\mathrm{null}\,}\)
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:
[−ℏ22m(∇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:
[−ℏ22m∇21+V(r1)]|a(r1)⟩=E1|a(r1)⟩;[−ℏ22m∇22+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.