In probability theory and specifically in discussion of measurement one speaks of postselection if only processes with certain (measurement) outcomes are selected for (further) discussion.
Postselection plays a special role in quantum measurement due to the latter’s intrinsically non-deterministic nature, cf. repeat-until-success computing.
See also:
Early discussion of quantum (pre- and) post-selection in a context of a notion called “weak” quantum measurement:
Yakir Aharonov, David Z. Albert, Lev Vaidman: How the result of a measurement of a component of the spin of a spin- particle can turn out to be , Phys. Rev. Lett. 60 1351 [doi:10.1103/PhysRevLett.60.1351]
Yakir Aharonov, Lev Vaidman: Complete description of a quantum system at a given time, J. Phys. A: Math. Gen. 24 (1991) 2315 [doi:10.1088/0305-4470/24/10/018]
Yakir Aharonov, Lev Vaidman: The Two-State Vector Formalism of Qauntum Mechanics: an Updated Review [arXiv:quant-ph/0105101]
Review of the general notion of quantum postselection:
See also:
In the context of quantum complexity theory (cf. PostBQP):
In the context of quantum advantage:
Last revised on May 6, 2025 at 10:23:35. See the history of this page for a list of all contributions to it.