Quantum mechanics, by itself, implies perception of a classical world

Joseph Mendola

Casey Blood

The three major theoretical principles of quantum mechanics relevant to its interpretation are: (T1), linearity; (T2), invariance under certain groups; and (T3) the orthogonality and isolation of the different branches of the state vector. These three imply the particle-like properties of mass, energy, momentum, spin, charge, and locality are actually properties of the state vector; and this in turn implies there is no evidence for the existence of particles. Experimentally there is no evidence for collapse (E1) and theoretically linearity prohibits collapse. One also has the experimentally verified probability law (E2), which is found to rule out the many-worlds interpretation. The failure of these three major interpretation, particles, collapse, and many-worlds, apparently implies an acceptable interpretation must be based on perception. Rather than being a separate principle, probability follows in this interpretation from a weak assumption on perception plus the combinatorics when an experiment is run many times. This suggests a relatively simple experimental test of the perception interpretation.

Loyal Durand

This paper is concerned with the description of the process of measurement within the context of a quantum theory of the physical world. It is noted that quantum mechanics permits a quasi-classical description (classical in the limited sense implied by the correspondence principle of Bohr) of those macroscopic phenomena in terms of which the observer forms his perceptions. Thus, the process of measurement in quantum mechanics can be understood on the quasi-classical level by transcribing from the strictly classical observables of Newtonian physics to their quasi-classical counterparts the known rules for the measurement of the former. The remaining physical problem is the delineation of the circumstances in which the correlation of a peculiarly quantum mechanical observable A with a classically measurable observable B can result in a significant measurement of A. This is undertaken within the context of quantum theory. The resulting clarification of the process of measurement has important implications relative to the philosophic interpretation of quantum mechanics.

Arthur Jabs

Erich Joos

Michael B. Mensky

Subjective aspects of quantum mechanics (QM) are most radically expressed in the (EI) of QM which suggests coexisting macroscopically distinct configurations of the world in the form of a superposition of the (quasi-)classical state vectors. The components of such a superposition are often verbally denoted as Everett's worlds, hence the name Many-Worlds Interpretation (MWI) for EI. Explicit accounting the correlation of each classical configuration of the world with the corresponding state of an observer's mind yields the so-called Many-Minds interpretation (MMI). This is maximum that may be done in the context of EI if the restriction by pure physics is implied. In the author's Extended Everett Concept (EEC) the observer's consciousness is defined in the spirit of psycho-physical parallelism, i.e. as going beyond pure physics. As a consequence, according to EEC, an observer, if he/she weakens or turns off his/her consciousness (perception), obtains the ability of super-intuition (obtaining seemingly unavailable information) and even of controlling the subjective reality (a picture of classical reality as it will be subjectively perceived). This may be interpreted as a realization of the Jung's collective unconscious as well as an explanation of the mystical elements in Oriental philosophies, world religions and deep psychological practices. NeuroQuantology | March 2013 | Vol 11 | Issue 1 | Suppl 1 | Page 85-96