zonde said:
I can perform measurement that gives output for state ##\frac{1}{\sqrt{2}}(|0\rangle|-\rangle + |1\rangle|+\rangle)##. That's not the question.
The question is about performing measurement that gives outputs for states ##\frac{1}{\sqrt{2}}(|0\rangle|1\rangle + |1\rangle|0\rangle)## and ##\frac{1}{\sqrt{2}}(|0\rangle|-\rangle + |1\rangle|+\rangle)##
PeterDonis said:
Why wouldn't you be able to do this? The four output states described in the PBR paper are all orthogonal to each other and span the Hilbert space; therefore they must be eigenstates of some Hermitian operator, so there must be some measurement that has these states as its possible outcome states.
zonde said:
If I wish I can write all four measurements in the same basis and then do the PBR reasoning. So my objections do not matter.
So I test this approach.
I rewrite these four measurement states:
##|\xi_1\rangle=\frac{1}{\sqrt{2}}(|0\rangle\otimes|1\rangle+|1\rangle\otimes|0\rangle)##
##|\xi_2\rangle=\frac{1}{\sqrt{2}}(|0\rangle\otimes|-\rangle+|1\rangle\otimes|+\rangle)##
##|\xi_3\rangle=\frac{1}{\sqrt{2}}(|+\rangle\otimes|1\rangle+|-\rangle\otimes|0\rangle)##
##|\xi_4\rangle=\frac{1}{\sqrt{2}}(|+\rangle\otimes|-\rangle+|-\rangle\otimes|+\rangle)##
as:
##|\xi_1\rangle=\frac{1}{\sqrt{2}}(|0\rangle\otimes|1\rangle+|1\rangle\otimes|0\rangle)##
##|\xi_2\rangle=\frac{1}{2}(|0\rangle\otimes|0\rangle+|1\rangle\otimes|1\rangle-0\rangle\otimes|1\rangle+|1\rangle\otimes|0\rangle)##
##|\xi_3\rangle=\frac{1}{2}(|0\rangle\otimes|0\rangle+|1\rangle\otimes|1\rangle+0\rangle\otimes|1\rangle-|1\rangle\otimes|0\rangle)##
##|\xi_4\rangle=\frac{1}{\sqrt{2}}(|0\rangle\otimes|0\rangle-|1\rangle\otimes|1\rangle)##
But know I have another problem, measurements ##|\xi_2\rangle## and ##|\xi_3\rangle## are not operationally meaningful at least for photons. There is no measurement that can perform such a four way interference. Two way interference (like in ##|\xi_1\rangle## and ##|\xi_4\rangle##) can be performed by swapping measurement contexts of the two photons i.e. ##|0_A\rangle## mode is measured against ##|1_B\rangle## mode. But that approach is meaningless for four way interference.
Of course ##|\xi_2\rangle## and ##|\xi_3\rangle## could be measured if I express them in different basis, but that brings me back to starting point.