gentzen
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Even for Fermions, I can just ignore the wavefunction for the equivalence relation. I realized this when the skeptic in me started to ponder over a "serious omission" in the given quotient construction:gentzen said:I will elaborate it for Bosons, so that I can ignore the wavefunction for the equivalence relation.
If we interpret the trajectories as a function ##(x_1, \ldots, x_n)(t) : \mathbb R \to \mathbb R^{3n}## and consider "piecewise constant" permutations ##\pi(t):\mathbb R \to S_n##, then ##(x_{\pi(t)(1)}, \ldots, x_{\pi(t)(n)})(t)## is only "piecewise continuous". So it is not a "strong" solution of the guiding equation. Weakening the continuity requirements is possible (and needed, because otherwise uniqueness of solution together with continuity allows identification of particles between different times), but it feels very much like a "patchwork construction".
Turns out my attempt to illustrate the character of "unnatural" constructions as "patchwork constructions" in the initial reply to A. Neumaier failed to identify the crucial points. Glueing together the endpoints of a closed interval to get a circle is an "unnatural" construction, but taking an open interval and identifying two small open intervals at both ends (pointwise) with each other to get a circle is a not an "unnatural" construction, despite allowing patchwork. (And the "quotient by a discrete subgroup" fails even worse to identify the crucial points, "discrete" is neither necessary nor sufficient, and "subgroup" instead of "group" was superfluous.)
I guess the point of "natural quotient" constructions is rather that at least locally, the real work should already be finished before taking the quotient, so that it doesn't make a difference for "local topological" constructions whether they are applied before or after taking the quotient.
Of course, it is completely unclear what "much more efficient" is supposed to mean in this context. The meaning of "anything physical" is clearer, but for me it is enough that dBB and quotient constructions provide "something mathematical".vanhees71 said:Of course, it's much more efficient to simply not use any kind of trajectories as in the dBB interpretation. They do not provide anything physical to QT anyway. You may solve some philosophical quibble but introduce more complication without gaining any new insights from a scientific point of view.
The relationship between "mathematical constructions" and "philosophical quibbles" has always been a complicated one. Legend says that the Pythagoreans killed the one who discovered irrational numbers. And Zeno of Elea attacked the continuum on philosophical grounds. In both cases, the attacked concepts turned out to have hidden complexities and dangers, but the attacks themselves failed to clearly isolate those or show a way forward. Maybe philosophers are better at articulating hidden problems, than at helping to overcome them.
At least for me, reading philosophical texts is sometimes both fun and useful. SEP comes to mind, and also:
Teller made quite some effort to help his reader grasp how radically different truly "indistinguishable particles" are compared to our everyday experience. Looking at them in dBB on the other hand shows you how they require (anti-)symmetric wavefunctions and some form of discontinuity. As always, the discontinuity required in dBB is "too nonlocal" compared to what you actually need. And of course, lessons from dBB apply primarily to non-relativistic QM.gentzen said:..., then I read An Interpretive Introduction to Quantum Field Theory cover to cover. It was easy to read, with a good mix of technical details, explanations, interpretations, and philosophical clarification.
… much of the interpretive work Teller undertakes is to understand the relationship and possible differences between quantum field-theory — i.e., QFT as quantization of classical fields — and quantum-field theory — i.e., a field theory of ‘quanta’ which lack radical individuation, or as Teller says, “primitive thisness.”