A reconstruction of quantum mechanics from quantum logics with unique conditional probabilities

          @misc{ scivideos_PIRSA:09080019,
            doi = {10.48660/09080019},
            url = {https://pirsa.org/09080019},
            author = {Niestegge, Gerd},
            keywords = {Quantum Foundations},
            language = {en},
            title = {A reconstruction of quantum mechanics from quantum logics with unique conditional probabilities},
            publisher = {Perimeter Institute for Theoretical Physics},
            year = {2009},
            month = {aug},
            note = {PIRSA:09080019 see, \url{https://scivideos.org/pirsa/09080019}}
          }
          

Abstract

The starting point of the reconstruction process is a very simple quantum logical structure on which probability measures (states) and conditional probabilities are defined. This is a generalization of Kolmogorov's measure-theoretic approach to probability theory. In the general framework, the conditional probabilities need neither exist nor be uniquely determined if they exist. Postulating their existence and uniqueness becomes the major step in the reconstruction process. A certain new mathematical structure can then be derived, and examples immediately reveal that probability conditionalization is identical with the Lüders - von Neumann measurement process. Some further postulates bring us to Jordan algebras, and the consideration of composite systems finally shows why these algebras must be the self-adjoint parts of von Neumann algbras such that they can be represented as linear operators on Hilbert spaces over the complex numbers. This is why the approach gets ahead of other ones that are not able to justify the need for the complex Hilbert space or the Jordan operator algebras. The mathematical structure of quantum mechanics can thus be reconstructed from a few probabilistic basic principles and becomes a non-Boolean extension of classical probability theory. Its link to physics is that probability conditionalization in this structure is identical with the Lüders - von Neumann measurement process.