rogerl
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A. Neumaier said:Not yet but in the right direction. In condensed matter, the bare theory makes sense in principle, since (due to lack of particle creation and annihilation) it is the theory of the asymptotic particles at zero temperature. But to do calculations, one wants to think of the effective degrees of freedom of the solid, which are the ground state excitations. One wants to consider the ground state to be the vacuum, and the collective excitations to be the (quasi-)particles. To get this view, one needs to renormalize the theory - this is like in particle physics, except that, because the bare theory is physically meaningful, all renormalizations are finite.
In relativistic quantum field theory, there is no substance (aether) that would fill the ground state (vacuum), upon which one could build the theory. The bare particles pretend to be such a substance but is found inadequate, as seen by the divergences. But by taking careful limits and adjusting the parameters of the bare theory to diverge while taking the limit - which is possible only since the bare stuff is unphysical - one can still arrive at a renormalized theory in which the vacuum is a Poincare invariant state and the Hilbert space has the required property of carrying covariant and causal field operators.
This has nothing to do with being or not being an effective theory - the latter only need an infinite number of renormalization parameters for their construction.
It has also nothing to do with nonlinearities - the field equations underlying condensed matter are also nonlinear. The difference to condensed matter theory comes from the requirement of causality, which necessitates processes that change particle number.
You mentioned that the vacuum is a poincare invariant state. So the quantum vacuum is another mathematical figment of imagination just like the virtual particles?? Or is quantum vacuum located in space? Or not? If not, then space has only empty contents that has no vacuum and virtual particles?