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I think this discussion goes in circles. As I've already stated, the term "vacuum fluctuations" is a pretty empty phrase if not clearly defined. I think it's best described as the (perturbative) corrections due to the quantization of the electromagnetic field beyond the approximation to treat the field as classical. You cannot observe them without having a detector and thus matter (i.e., particles). So it's not really the vacuum you test.friend said:The whole course does nothing except show how vacuum fluctuations get excited by acceleration and produces particles. In the second or third video he gets out a string with a weight and shows how parametric excitations (excited modes) can be produced by shortening the string in mid-oscillation. This is meant to show how the fluctuations of the vacuum state can be excited to produce particles.
As we also stated more than once, the Casimir effect is about the interaction of charged particles through the electromagnetic field and the quantum fluctuations of both these charges and fields (see the paper by Jaffe, I've cited). Another example, not yet observed, is the Schwinger pair production, i.e., the creation of electron-positron pairs at presence of strong electromagnetic fields. Again, there's matter and an electric field present making the observation of the quantum effects possible. Thus, I'd rather simply speak about quantum effects or quantum fluctuations rather than vacuum fluctuations.
A formal statement is utmost simple: A quantum system in its ground state let alone must stay in its ground state. There's no additional energy to make an excitation from the ground state possible, and the ground state of QFT is called "vacuum", because it's the state where no real particles and fields are present.