A time-symmetric formulation of quantum mechanics

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Nonperturbative theory of weak pre-and post-selected measurements (2011, background): “ariables R and F. For such a meter, the shift of the pointer distribution is known to be proportional to Re Aw, at least, when the initial meter state in the pointer representation is a real Gaussian [24, 69, 80, 118]. However, for the general case the shift has not been discussed yet. Here we assum”
Do We Really Understand Quantum Mechanics? (2012, background): “The authors of [384] propose to interpret this situation in a nonstandard way, by considering that the preselection and postselection processes, when combined, select spins having two orthogonal components perfectly well defined (which is of course totally impossible in the usual formulation of quan”
Direct measurement of the quantum wavefunction (2011, methodology): “weak measurement [9–18]) so as not to invalidate the second.”