Dear Professor Ellis,
Thank you very much for commenting about my presentation.
We can disagree about unitarity. At this point I find both unitary and discontinuous collapse explanations incomplete. I will take this opportunity to explain why it is not that clear there is a discontinuous collapse. For example, in the case of the experiment with Mach-Zehnder interferometer, with delayed choice. Our choice concerning the second beam splitter seems to affect what happened to the photon at the first beam splitter. Assuming there's a discontinuous collapse, it should happen somewhere between the first and the second beam splitter. But this means that a photon which was split and travels along both arms of the interferometer, suddenly collapses on one arm. This would be strange, and conservation laws would be violated. Assuming that the collapse happened before the photon entered the first beam splitter, then why not saying as well that it never happened, or that it happened at the Big-Bang.
The case of preparation-measurement, which is generally considered the irrefutable proof of collapse, was explained at the slides you quote, "The measurement of O1 in fact refines both the initial conditions of the system \psi, and those of the apparatus \eta". Those slides present a possible unitary explanation of the collapse, by using the entanglement with the preparation device. It is very similar to the Mach-Zehnder interferometer experiment with delayed choice: what we choose to measure determines the way the system interacted with the preparation device.
Another argument I find convincing is that of conservation laws. They normally follow from unitary evolution - from commutation with the Hamiltonian. Is there a method to obtain the conservation laws, method which holds even when there is a discontinuous collapse?
I admit though that, besides these arguments and others I put in those slides, one can't find an irrefutable experimental evidence for or against discontinuous collapse. If there's discontinuous collapse, it will always hide no matter how we rearrange the experiment. If it takes place unitarily, locally appears like serendipity, as if a disturbance distributed between the preparation device and the measurement device "accidentally" puts the system in the observed state, so that it doesn't need to collapse. But, even if we allow discontinuous collapse, this kind of "accidents" happen. This is in fact what makes QM contextual. So, if we have anyway to accept strange contextual nonlocal backward in time behavior, then the worst about unitary collapse is already accepted when we accept discontinuous collapse.
Best wishes,
Cristi Stoica