Comment on “The quantum pigeonhole principle and the nature of
... They argue that if the imaginary first measurement had resulted in the two particles being in different boxes, and that imaginary measurement had been followed by the genuine second measurement, then Φ could not have been obtained as the postselected state. Hence (according to the authors), particle ...
... They argue that if the imaginary first measurement had resulted in the two particles being in different boxes, and that imaginary measurement had been followed by the genuine second measurement, then Φ could not have been obtained as the postselected state. Hence (according to the authors), particle ...
QBism, the Perimeter of Quantum Bayesianism
... worries: The universe didn’t have to wait billions of years to collapse its first wave function—wave functions are not part of the observer-independent world. But this much of the solution is an elderly and somewhat ineffective antibody. Its presence is mostly a call for more clinical research. Luck ...
... worries: The universe didn’t have to wait billions of years to collapse its first wave function—wave functions are not part of the observer-independent world. But this much of the solution is an elderly and somewhat ineffective antibody. Its presence is mostly a call for more clinical research. Luck ...
The quantum phases of matter - Subir Sachdev
... suppressed to yield a vanishing conductivity in the limit of zero temperature. For a simple example of a Mott insulator, consider electrons hopping in a single band on the triangular lattice. After the Coulomb repulsion localizes the electron charge, the Hilbert space can be truncated to the quantum ...
... suppressed to yield a vanishing conductivity in the limit of zero temperature. For a simple example of a Mott insulator, consider electrons hopping in a single band on the triangular lattice. After the Coulomb repulsion localizes the electron charge, the Hilbert space can be truncated to the quantum ...
