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CRC Press eBooks

Basic Theory

Inge Svein Helland, Harish Parthasarathy

Published Oct 23, 2025• 0 citations
Publisher

Abstract

In the Preface of this book, we have mentioned several approaches [ 1 , 2 , 3 , 4 ] to the problem of connecting quantum theory and general relativity theory. In our opinion, before a final thinking around this problem, it is vital to make some efforts to find a new and less formal foundation of quantum theory. This has now been done by the first author in a process starting with the book [ 5 ] and further developed in a series of articles. A summary of the theory is now given in [ 6 ]. Central to the theory is a simple model of the mind of an observer, a model which may be generalized to the mind of any person. It first relies on what is called theoretical variables , which may be physical variables, but in the process of planning, doing, or interpreting experiments, the variables are also assumed to exist in the mind of a relevant actor. From a mathematical point of view, our only requirement for the theoretical variables is the following: If λ is a theoretical variable and θ = f ( λ ) for some fixed function f , then θ is also a theoretical variable.

DOI
10.1201/9781003726470-2

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In the Preface of this book, we have mentioned several approaches [ 1 , 2 , 3 , 4 ] to the problem of connecting quantum theory and general relativity theory. In our opinion, before a final thinking around this problem, it is vital to make some efforts to find a new and less formal foundation of quantum theory. This has now been done by the first author in a process starting with the book [ 5 ] and further developed in a series of articles. A summary of the theory is now given in [ 6 ]. Central to the theory is a simple model of the mind of an observer, a model which may be generalized to the mind of any person. It first relies on what is called theoretical variables , which may be physical variables, but in the process of planning, doing, or interpreting experiments, the variables are also assumed to exist in the mind of a relevant actor. From a mathematical point of view, our only requirement for the theoretical variables is the following: If λ is a theoretical variable and θ = f ( λ ) for some fixed function f , then θ is also a theoretical variable.
The purpose of this part of the book has been to sketch a new, and in our opinion quite promising, attempt to understand parts of quantum theory and general relativity theory from a common basis. One important background for us is that relativity theory is developed by the mind of a single person, while quantum theory, in the way that it has existed up to now, is a patchwork of contributions from many different persons. Empirically, both theories have been verified to an impressive degree, but the foundation of and interpretation of quantum theory has been the source of much confusion. The book [ 5 ] is an attempt to develop the epistemic side of a new foundation, and from this propose a new interpretation: In every application, but also more generally, it is connected to the mind of a single actor or to the joint mind of a group of communicating actors.
It is very likely that most readers and authors of articles appearing in Classical and Quantum Gravity are interested in what might loosely be termed the philosophy of science. It is equally likely, with perhaps a few exceptions, that the research of these same readers and authors has not been influenced in the least by the work of professional philosophers of science. This is certainly the case for those of us who work in quantum field theory. One must therefore ask who the intended audience is for a book which purports to discuss the philosophical implications of quantum field theory. In the preface, the author states that there are two intended audiences for his book. The first is `other interested interpreters of physics' who wish to learn something about quantum field theory in as painless a way as possible. The second is for students of physics who are bogged down in the details of learning quantum field theory and cannot see the overall picture. I am not convinced that either audience will find this book to be of much use. There are two basic problems with this book. The first is that the quantum field theory in it is of the old-fashioned kind, and is not really representative of the way the subject is either taught or thought of today. The second is that there is not sufficient background material present to make this book suitable for a novice reader. For example, I wonder how much a reader who has not studied quantum mechanics in any depth will get out of a treatment which launches into Hilbert space and a discussion of states without much in the way of proper introduction. Any reader who is familiar with the workings of quantum field theory will find much to disagree with in this book. For example, the author tries to make a case that a Fock space description is better than talking about particle labels and restricting to symmetric or antisymmetric states. The reason claimed for this is that there are states in Fock space which are neither symmetric nor antisymmetric under particle interchange which must be discarded. (In the author's words, this introduces `surplus formal structure'.) However, in Fock space an equally arbitrary choice is made by focusing on relations among the creation and annihilation operators which involve only commutation or anticommutation relations. Although this is acknowledged by Teller, no satisfactory explanation is given as to why one procedure is any less arbitrary than the other. The book is incomplete in many ways, with many interesting points mentioned just in passing. For example, the discussion around the Newton--Wigner position operator would have been greatly enhanced by including more details, such as an explanation as to why quanta described by Newton--Wigner states seem to propagate at superluminal speeds. It is hard to believe that a reader who has not met the Rindler vacuum before would find Teller's discussion to be very informative. After being so critical of this book, I should mention a part which I did enjoy and would recommend to students of physics. This is the last chapter of the book which contains a discussion of renormalization theory. It is my experience that students often find renormalization theory confusing, and may find Teller's semiqualitative discussion illuminating.
A general theory based on six postulates is introduced. The basic notions are theoretical variables that are associated with an observer or with a group of communicating observers. These variables may be accessible or inaccessible. From these postulates, the ordinary formalism of quantum theory is derived. The mathematical derivations are not given in this article, but I refer to the recent articles. Three possible applications of the general theory can be given as follows: (1) the variables may be decision variables connected to the decisions of a person or a group of persons, (2) the variables may be statistical parameters or future data, and (3) most importantly, the variables are physical variables in some context. The last application gives a completely new foundation of quantum mechanics, a foundation which in my opinion is much easier to understand than ordinary formalism. So-called paradoxes like that of Schrödinger’s cat can be clarified under the theory. Explanations of the outcomes of David Bohm’s version of the EPR (Einstein–Podolsky–Rosen) experiment and the Bell experiment are provided. Finally, references to links toward relativity theory and quantum field theory are given. The concluding remarks point to further possible developments.
Much of the remainder of this book will concern itself with those aspects of theoretical physics which seek to understand the nature of matter. Such understanding as we have has mainly been achieved by probing the structure of successively smaller constituents and, at least on the face of things, the regions of space and time we need to consider are far too small for spacetime curvature to be of any significance. Many of our considerations will therefore be restricted to Minkowski or, as in the present chapter, Galilean spacetime. Paradoxically, however, it seems that gravity and the structure of space and time may have a vital role to play in our understanding of matter on the very smallest scales, and we shall see something of the ways in which this comes about in later chapters.
Much of the remainder of this book will concern itself with those aspects of theoretical physics which seek to understand the nature of matter. Such understanding as we have has mainly been achieved by probing the structure of successively smaller constituents and, at least on the face of things, the regions of space and time we need to consider are far too small for spacetime curvature to be of any signicance. Many of our considerations will therefore be restricted to Minkowski or, as in the present chapter, Galilean spacetime. Paradoxically, however, it seems that gravity and the structure of space and time may have a vital role to play in our understanding of matter on the very smallest scales, and we shall see something of the ways in which this comes about in later chapters.
A general theory based upon 7 postulates is introduced. The basical notions are theoretical variables that are associated with an observer or with a group of communicating observers. These variables may be accessible or inaccessible. From these postulates, the ordinary formalism of quantum theory is derived. The mathematical derivations are not given in this article, but I refer to the recent articles [9, 10]. Three possible applications of the general theory can be given; 1) The variables may decision variables connected to the decisions of a person or of a group of persons. 2) The variables may be statistical parameters or future data, But most importantly here: 3) The variables are physical variables in some context. This last application gives a completely new foundation of quantum mechanics, a foundation which in my opinion is much more easy to understand than the ordinary formalism.The other applications seem also to give interesting consequences of the approach. Socalled paradoxes like that of Schrödinger's cat can be clarified under the theory. Explanations of the outcomes of David Bohm's version of the EPR experiment and of the Bell experiment are provided. Finally, references to links towards relativity theory and to quantum field theory are given. The concluding remarks point at further possible developments.