I was also having a problem with this, but I think it can be resolved by saying that every operator is symmetric in A and B. Therefore, whenever we take a measurement, we will fail to distinguish between a blob at (1,0) and a blob at (0,1). More fundamentally, any interaction with a third particle will be the same whether the blob is at (1,0) or (0,1).
Even more important is that a blob at (0,1) plus a blob with the opposite phase at (1,0) can have a subtractive effect, even cancelling out entirely if both have the same amplitude.
In a sense, then, factoring the topology of configuration-space by the identity A==B causes the symmetry of operators to be an unavoidable consequence of the topology, rather than some freakish coincidence.
I agree that taking quotients of the configuration space is a more natural way of doing things. But, when you say
don’t you mean you’re left with a 3-dimensional quotient space? Counting degrees of freedom: wherever we put A, that eats the translation. Wherever we put B, that eats the rotation and we’re left with the distance |AB| (one dimension). Wherever we put C, that eats reflection and we’re left with the position of C up to reflection. So, the space of triangles ends up as R x R x (R / ~), where a~b iff |a|=|b|.
But then, this space should be homeomorphic to the one Eliezer gives, with the relative distances. We’ll take a point (x,y,z) in R x R x (R / ~). Then |AB|=x, |AC|=hypot(y, z), |BC|=hypot(y-x, z), clearly this is continuous and nice, and also clearly the image doesn’t change if we replace z by -z (so the function is well-defined despite the domain being a quotient space, which generally needs to be checked). Showing that the mapping is invertible, with continuous inverse, is left as exercise for the reader.
Consider now the apparent boundary when we embed this in R³; it’s z=0, which corresponds to “A, B and C form a straight line”, which (triangle inequality) corresponds to the boundary of the subset of distance-space. But if you imagine the particles moving, it’s a lot more obvious that you should bounce off the ”/ ~” surface than that you should bounce off the “if you cross this surface you get a distance-tuple that’s un-geometric” surface. Similarly, straight lines in R x R x (R / ~) correspond to fixing any two particles and moving the third in a straight line.
I would conclude from this that the equations of physics in the quotient space are likely to be much nicer than the equivalent equations in distance-tuple space.
So why bother formulating the relational configuration space in distance-tuples? After all, with the distance-tuples, you still end up having to quotient afterwards on particle-swapping to get the quantum-mechanical picture. Isn’t it easier to just use quotients, rather than an odd mix of quotients, new bases, and subsets?