Hi, akhmeteli, the measurement problem is "semi-solved". The problem is where is the cut between classical and quantum. I don´t know link, but I answer a question about it a little ago. There ir wavefunction more or less semiclassical ( WKB aproxximation), and if and system is more classical than another that it is used like measurement device, then all the apparatus more classical than this are of course measurement device too. There is no problem in praxis. I was more interested with the contradiction between collapse and relativity. I don´t know if there a solution, the problem is not it may be antiintuitive, the problem is we lost any reference to define the position operator. And I don´t know what happens with the GR invariance in collapse moment