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Quantum Logic PDF

167 Pages·1978·4.558 MB·English
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QU ANTUM LOGIC SYNTHESE LIBRARY STUDIES IN EPISTEMOLOGY, LOGIC, METHODOLOGY, AND PHILOSOPHY OF SCIENCE Managing Editor: JAAKKO HINTIKKA, Academy of Finland and Stanford University Editors: ROBERT S. COHEN, Boston University DON ALD DAVIDSON, University of Chicago GABRIEL NUCHELMANS, University of Leyden WESLEY C. SALMON, University of Arizona VOLUME 126 QUANTUM LOGIC by PETER MITTELST AEDT University of Cologne, Germany D. REIDEL PUBLISHING COMPANY DORDRECHT: HOLLAND I BOSTON: U.S.A. LONDON: ENGLAND Ubrary of Congress Cataloging In PubHcation Data Mittelstaedt, Peter, 1929- Quantum logic. (Synthese library; v. 126) Bibliography: p. Includes index. 1. Quantum theory. 2. Logic, Symbolic and mathe matical. I. Title. QCI74.17.M35M57 530.1'2 78-10433 ISBN-13: 978-94-009-9873-5 e-ISBN-13: 978-94-009-9871-1 DOl: 10.1007/978-94-009-9871-1 Published by D. Reidel Publishing Company, P.O. Box 17, Dordrecht, Holland Sold and distributed in the U.S.A., Canada, and Mexico by D. Reidel Publishing Company, Inc. Lincoln Building, 160 Old Derby Street, Hingham, Mass. 02043, U.S.A. All Rights Reserved Copyright © 1978 by D. Reidel Publishing Company, Dordrecht, Holland No part of the material protected by this copyright notice may be reproduced or utilized in any form or by any means, electronic or mechanical, including photocopying, recording or by any informational storage and retrieval system, without written permission from the copyright owner TO MECHTHILD T ABLE OF CONTENTS INTRODUCTION CHAPTER 1/ THE HILBERT SPACE FORMULATION OF QUANTUM PHYSICS 6 1.1 The Hilbert Space 6 1.2 The Lattice of Subspaces of Hilbert Space 11 1.3 Projection Operators 16 1.4 States and Properties of a Physical System 21 CHAPTER 2/ THE LOGICAL INTERPRETATION OF THE LATTICE Lq 27 2.1 The Quasimodular Lattice Lq 27 2.2 The Relation of Commensurability 31 2.3 The Material Quasi-implication 37 2.4 The Relation between Lattice Theory and Logic 42 CHAPTER 3 / THE MATERIAL PROPOSITJONS OF QUANTUM PHYSICS 48 3.1 Elements of a Language of Quantum Physics 48 3.2 Argument-rules for Compound Propositions 53 3.3 Commensurability and Incommensurability 60 3.4 The Material Dialog-game 65 CHAPTER 4/ THE CALCULUS OF EFFECTIVE QUANTUM LOGIC 72 4.1 Formally True Propositions 72 4.2 Formal Dialogs with Material Commensurabilities 76 4.3 The Formal Dialog-game 82 4.4 The Calculus Qeff of Effective Quantum Logic 88 CHAPTER 5/ THE LATTICE OF EFFECTIVE QUANTUM LOGIC 99 5.1 The Quasi-implicative Lattice Lqi 99 5.2 Properties of the Lattice L 104 qj viii TABLE OF CONTENTS 5.3 The Relation between Lqi and the Lattice Li 109 5.4 The Relation between Lqi and the Lattice Lq 113 CHAPTER 6/ THE CALCULUS OF FULL QUANTUM LOGIC 119 6.1 Value-definite Material Propositions 119 6.2 The Value-definiteness of Compound Propositions 124 6.3 The Extension of the Calculus Qelf 128 6.4 The Principle of Excluded Middle 134 CONCLUDING REMARKS: CLASSICAL LOGIC AND QU ANTUM LOGIC 140 BIBLIOGRAPHY 144 INDEX 147 INTRODUCTION In 1936, G. Birkhoff and J. v. Neumann published an article with the title The logic of quantum mechanics'. In this paper, the authors demonstrated that in quantum mechanics the most simple observables which correspond to yes-no propositions about a quantum physical system constitute an algebraic structure, the most important proper ties of which are given by an orthocomplemented and quasimodular lattice Lq. Furthermore, this lattice of quantum mechanical proposi tions has, from a formal point of view, many similarities with a Boolean lattice L8 which is known to be the lattice of classical propositional logic. Therefore, one could conjecture that due to the algebraic structure of quantum mechanical observables a logical calculus Q of quantum mechanical propositions is established, which is slightly different from the calculus L of classical propositional logic but which is applicable to all quantum mechanical propositions (C.F. v. Weizsacker, 1955). This calculus has sometimes been called 'quan tum logic'. However, the statement that propositions about quantum physical systems are governed by the laws of quantum logic, which differ from ordinary classical logic and which are based on the empirically well-established quantum theory, is exposed to two serious objec tions: (a) Logic is a theory which deals with those relationships between various propositions that are valid independent of the content of the respective propositions. Thus, the validity of logical relationships is not restricted to a special type of proposition, e.g. to propositions about classical physical systems. (b) The laws of logic, though valid for all statements encountered in experience, do not derive their validity from experience. Instead, logic must be considered as a theory the statements of which can be justified exclusively by its inherent evidence and irrespective of all empirical knowledge. These arguments become particularly apparent in the framework of the operational foundation of logic, which explains the 'truth' of a 2 INTRODUCTION logical statement by the existence of a strategy of success in a dialog. In this approach, the laws of logic are completely determined by the possibilities of proving or disproving elementary and compound pro positions within a well-defined proof procedure which can be represented by a dialog. Hence, the logical statements are 'true' independent of the special content of the actual propositions and for this reason they can neither be proved nor disproved by arguments which are based on empirical knowledge. The controversial situation which thus arises can, however, be clarified if the dialogic justification of ordinary propositional logic is investigated in more detail. In this way, it turns out that in the framework of the dialogic method an assumption is always tacitly made which restricts the propositions considered to those of classical physics and mathematics. Technically, this means that within the dialogic proof procedure of compound propositions only the truth or falsity of the respective sUb-propositions is tested but not their mutual commensurability. Therefore, one could try to search for an operational foundation of logic which is independent of the presup position just mentioned. By this it is not meant that some emprical knowledge about quantum mechanical propositions should be in corporated into the foundation of logic. Conversely, we will rather eliminate that empirical supposition which is still contained in the operational foundation of ordinary logic - namely the assertion that all propositions are mutually commensurable. Technically, this generalization of the dialogic method can be performed by in corporating an additional testing procedure which - apart from the truth and falsity - examines the mutual commensurability of two propositions. In this way, the generalized dialog-game can be equally applied to propositions of classical physics and of quantum physics. Starting from this generalized operational foundation of logic one arrives at a logical calculus Qeff. which will be called the calculus of effective quantum logic, and which differs from the well-known cal culus of effective (intuitionistic) logic inasmuch as some of the laws of this logic are valid only in a relaxed version. Furthermore, by a rather weak assumption concerning the measurability of commen surabilities, the 'tertium non datur' can be justified for all finite compound propositions and the calculus Qeff can be extended to the calculus Q of full quantum logic which incorporates the principle of excluded middle as a general law. It can then be shown that this calculus Q of full quantum logic is, in INTRODUCTION 3 fact, a model of the orthocomplemented and quasimodular lattice Lq which has been obtained previously from the algebraic structure of quantum mechanical observables. In this way, one obtains the following important results: (a) The orthocomplemented quasimodular lattice Lq which follows from a formal analysis of quantum mechanics can be interpreted as a generalized propositional logic. This 'quantum logic' is universal in the sense that the validity of its laws is not restricted to a special type of proposition. Instead, the laws of quantum logic are equally valid for all propositions of classical physics and of quantum physics. (b) Since the calculus Q of full quantum logic can be justified by theoretical reasons only and independent of any empirical knowledge, it follows that at least those structures of quantum mechanics which are summarized in the lattice Lq are non-empirical and may be considered as cognitions a priori. In order to demonstrate these results, we proceed in the following way: In Chapter 1, we summarize some formal properties of quantum mechanics which are of special importance for the problem of quan tum logic. It is shown that the yes-no propositions A, B, ... about a physical system S correspond respectively to sub-spaces MA, MH, ••• of the Hilbert space ~(S) which is associated with the system S as its state-space. On the other hand, these subspaces of a Hilbert space constitute a lattice, the most important properties of which are given by an orthocomplemented and quasimodular lattice L Hence, quan q• tum mechanical propositions form a lattice which has many proper ties in common with the Boolean lattice La of classical propositional logic and the operations of which have many similarities with the logical operations 'and', 'or' and 'not'. The formal properties of the lattice Lq and its relations to a Boolean lattice La are investigated in Chapter 2. Firstly, we show that a commensurability relation can be defined in Lq such that mutually commensurable propositions form Boolean sublattices of L q. Secondly, it is shown that the most important syntactical require ments for a logical calculus which can be formulated on the basis of La are also fulfilled by the lattice Lq. Hence, there are no formal arguments which exclude the possibility of an interpretation of Lq as a logical calculus. However, it is obvious that the formal similarities of Lq and La are by no means sufficient in order to justify a logical interpretation of the lattice L q• Therefore, for the present, we leave lattice theory and in Chapter 3

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