Extended Quantum Mechanical Framework

Malin Premaratne, Govind Prasad Agrawal

Kohtaro Tadaki

The notion of probability plays a crucial role in quantum mechanics. It appears in quantum mechanics as the Born rule. In modern mathematics which describes quantum mechanics, however, probability theory means nothing other than measure theory, and therefore any operational characterization of the notion of probability is still missing in quantum mechanics. In our former works [K. Tadaki, arXiv:1804.10174], based on the toolkit of algorithmic randomness, we presented a refinement of the Born rule, called the principle of typicality, for specifying the property of results of measurements in an operational way. The Wigner's friend paradox is a Gedankenexperiment regarding when and where the reduction of the state vector occurs in a chain of the measurements by several observers where the state of the consciousness of each observer is measured by the subsequent observer. In this paper, we extend the framework of the principle of typicality so that it can be applicable to situations where apparatuses perform measurements over other apparatuses. We then make an analysis of the Wigner's friend paradox within this extended framework of quantum mechanics based on the principle of typicality. We draw common sense conclusions about it. Deutsch's thought experiment is a variant of the Wigner's friend paradox, which can, in principle, verify the effect of the consciousness of observer on the reduction of the state vector. We make an analysis of it comprehensively within the extended framework. We then make a prediction which is testable in principle. In our extended framework, we can analyze still more complicated situations. As such an example, we introduce a combination of the above two, named the Wigner-Deutsch collaboration, and perform a thorough analysis of it.

Rudra Pandey

In this paper we introduce a mathematical framework, developed within the extended classical mechanics setup , which helps us derive quantum nature and the relation E = hν from it. By doing so, we give a solid mathematical foundation to quantum nature and remove the inherent incompatibilities between classical mechanics and quantum mechanics. We also derive Schrödinger's equation with the help of this framework to establish the validity of this framework.

Rainer Dick

R. P. Rundle, Todd Tilma, John H. Samson +3 more

Since the very early days of quantum theory there have been numerous attempts to interpret quantum mechanics as a statistical theory. This is equivalent to describing quantum states and ensembles together with their dynamics entirely in terms of phase-space distributions. Finite dimensional systems have historically been an issue. In recent works [Phys. Rev. Lett. 117, 180401 (2016) and Phys. Rev. A 96, 022117 (2017)] we presented a framework for representing any quantum state as a complete continuous Wigner function. Here we extend this work to its partner function---the Weyl function. In doing so we complete the phase-space formulation of quantum mechanics---extending work by Wigner, Weyl, Moyal, and others to any quantum system. This work is structured in three parts. First we provide a brief modernized discussion of the general framework of phase-space quantum mechanics. We extend previous work and show how this leads to a framework that can describe any system in phase space---putting it for the first time on a truly equal footing to Schr\"odinger's and Heisenberg's formulation of quantum mechanics. Importantly, we do this in a way that respects the unifying principles of ``parity'' and ``displacement'' in a natural broadening of previously developed phase-space concepts and methods. Secondly we consider how this framework is realized for different quantum systems; in particular we consider the proper construction of Weyl functions for some example finite dimensional systems. Finally we relate the Wigner and Weyl distributions to statistical properties of any quantum system or set of systems.