The transactional interpretation of quantum mechanics

John G. Cramer Department of Physics FM 15, -University of Washington, Seattle, Washington 98195 and Bereich Kernund Strahlenphysik, Hahn-Meitner-Institut f'ur Kernforschung, 0-1000 Berlin 39 The interpretational problems of quantum mechanics are considered. The way in which the standard Copenhagen interpretation of quantum mechanics deals with these problems is reviewed. A new interpretation of the formalism of quantum mechanics, the transactional interpretation, is presented. The basic element of this interpretation is the transaction describing a quantum event as an exchange of advanced and retarded waves, as implied by the work of Wheeler and Feynman, Dirac, and others. The transactional interpretation is explicitly nonlocal and thereby consistent with recent tests of the Bell inequality, yet is relativistically invariant and fully causal. A detailed comparison of the transactional and Copenhagen interpretations is made in the context of well-known quantum-mechanical Gedankenexperimente and "paradoxes. " The transactional interpretation permits quantum-mechanical wave functions to be interpreted as real waves physically present in space rather than as "mathematical representations of knowledge" as in the Copenhagen interpretation. The transactional interpretation is shown to provide insight into the complex character of the quantum-mechanical state vector and the mechanism associated with its "collapse. " It also leads in a natural way to justification of the Heisenberg uncertainty principle and the Born probability law (I' =gf*), basic elements of the Copenhagen interpretation.

[1]  Erwin Schrödinger,et al.  Quantisierung als Eigenwertproblem , 1925 .

[2]  W. Heisenberg A quantum-theoretical reinterpretation of kinematic and mechanical relations , 1925 .

[3]  M. Born Zur Quantenmechanik der Stoßvorgänge , 1926 .

[4]  M. Born Quantenmechanik der Stoßvorgänge , 1926 .

[5]  Erwin Schrödinger,et al.  Über das Verhältnis der Heisenberg‐Born‐Jordanschen Quantenmechanik zu der meinem , 1926 .

[6]  E. Schrödinger Energieaustausch nach der Wellenmechanik , 1927 .

[7]  E. Schrödinger Über den Comptoneffekt , 2022 .

[8]  E. Schrödinger Der Energieimpulssatz der Materiewellen , 1927 .

[9]  M. Born Physical Aspects of Quantum Mechanics , 1927, Nature.

[10]  Louis de Broglie,et al.  La mécanique ondulatoire et la structure atomique de la matière et du rayonnement , 1927 .

[11]  C. Darwin A Collision Problem in the Wave Mechanics , 1929 .

[12]  R. Peierls,et al.  Erweiterung des Unbestimmtheitsprinzips für die relativistische Quantentheorie , 1931 .

[13]  N. Bohr,et al.  Quantum Mechanics and Physical Reality , 1935, Nature.

[14]  Albert Einstein,et al.  Can Quantum-Mechanical Description of Physical Reality Be Considered Complete? , 1935 .

[15]  E. Schrödinger Discussion of Probability Relations between Separated Systems , 1935, Mathematical Proceedings of the Cambridge Philosophical Society.

[16]  N. Bohr II - Can Quantum-Mechanical Description of Physical Reality be Considered Complete? , 1935 .

[17]  W. H. Furry Note on the Quantum-Mechanical Theory of Measurement , 1936 .

[18]  W. H. Furry Remarks on Measurements in Quantum Theory , 1936 .

[19]  Paul Adrien Maurice Dirac,et al.  Classical theory of radiating electrons , 1938 .

[20]  J. Wheeler,et al.  Interaction with the Absorber as the Mechanism of Radiation , 1945 .

[21]  R. Feynman Space - time approach to quantum electrodynamics , 1949 .

[22]  J. Wheeler,et al.  Classical Electrodynamics in Terms of Direct Interparticle Action , 1949 .

[23]  M. Renninger Zum Wellen-Korpuskel-Dualismus , 1953 .

[24]  H. Everett "Relative State" Formulation of Quantum Mechanics , 1957 .

[25]  J. Wheeler Assessment of Everett's 'Relative State' Formulation of Quantum Theory , 1957 .

[26]  J. Lebowitz,et al.  TIME SYMMETRY IN THE QUANTUM PROCESS OF MEASUREMENT , 1964 .

[27]  J. Bell On the Einstein-Podolsky-Rosen paradox , 1964 .

[28]  O. Beauregard LE · PARADOXE · DES CORRELATIONS D'EINSTEIN: ET DE SCHRÖDINGER ET L'ËPAISSEUR TEMPORELLE DE LA TRANSITION QUANTIQUE , 1965 .

[29]  Robert Bruce Lindsay,et al.  The Current Interpretation of Wave Mechanics , 1965 .

[30]  J. Bell On the Problem of Hidden Variables in Quantum Mechanics , 1966 .

[31]  L. Mandel,et al.  Interference of Independent Photon Beams , 1967 .

[32]  G. Feinberg,et al.  Possibility of Faster-Than-Light Particles , 1967 .

[33]  James B. Hartle,et al.  Quantum Mechanics of Individual Systems , 1968, 1907.02953.

[34]  ELECTRODYNAMICS OF DIRECT INTERPARTICLE ACTION. I. THE QUANTUM MECHANICAL RESPONSE OF THE UNIVERSE. , 1969 .

[35]  A quantum theory of Wheeler–Feynman electrodynamics , 1970 .

[36]  Bryce S. DeWitt,et al.  Quantum mechanics and reality , 1970 .

[37]  Leslie E Ballentine,et al.  The statistical interpretation of quantum mechanics , 1970 .

[38]  E. H. Walker,et al.  Quantum‐mechanics debate , 1971 .

[39]  Electrodynamics of direct interparticle action: II. Relativistic treatment of radiative processes , 1971 .

[40]  Henry P. Stapp,et al.  S-MATRIX INTERPRETATION OF QUANTUM THEORY. , 1971 .

[41]  EXTENSION OF WHEELER--FEYNMAN QUANTUM THEORY TO THE RELATIVISTIC DOMAIN. I. SCATTERING PROCESSES. , 1971 .

[42]  Matison,et al.  Experimental Test of Local Hidden-Variable Theories , 1972 .

[43]  Extension of Wheeler-Feynman quantum theory to the relativistic domain. II. Emission processes , 1972 .

[44]  R. B. Partridge Absorber Theory of Radiation and the Future of the Universe , 1973, Nature.

[45]  J. Cramer,et al.  Importance of Coulomb interaction potentials in heavy-ion distorted-wave Born-approximation calculations , 1974 .

[46]  Nick Herbert Cryptographic approach to hidden variables , 1975 .

[47]  D. Pegg Absorber theory of radiation , 1975 .

[48]  W. Davidon Quantum physics of single systems , 1976 .

[49]  H. Stapp Theory of reality , 1977 .

[50]  O. C. D. Beauregard Time symmetry and the Einstein paradox , 1977 .

[51]  O. C. D. Beauregard Einstein-Podolsky-Rosen non-separability and Feynman non-locality , 1977 .

[52]  P. H. Eberhard,et al.  Bell's theorem without hidden variables , 1977 .

[53]  Nick Herbert,et al.  Generalization of Bell's theorem , 1978 .

[54]  G. Feinberg Lorentz invariance of tachyon theories , 1978 .

[55]  O. C. D. Beauregard S-matrix, Feynman zigzag and Einstein correlation , 1978 .

[56]  A. Shimony,et al.  Bell's theorem. Experimental tests and implications , 1978 .

[57]  P. H. Eberhard,et al.  Bell’s theorem and the different concepts of locality , 1978 .

[58]  B. D'espagnat,et al.  The Quantum Theory and Reality , 1979 .

[59]  O. C. D. Beauregard Time symmetry and the Einstein paradox. - II , 1979 .

[60]  T. Weber,et al.  On some recent suggestions of superluminal communication through the collapse of the wave function , 1979 .

[61]  M. Gyulassy,et al.  PION INTERFEROMETRY OF NUCLEAR COLLISIONS I: THEORY , 1979 .

[62]  O. C. D. Beauregard Ψ Collapse and locality , 1979 .

[63]  G. Ghirardi,et al.  A general argument against superluminal transmission through the quantum mechanical measurement process , 1980 .

[64]  F. Selleri,et al.  Unacceptability of the Pauli-Jordan propagator in physical applications of quantum mechanics , 1980 .

[65]  J. Cramer Generalized absorber theory and the Einstein-Podolsky-Rosen paradox , 1980 .

[66]  Anthony J Leggett,et al.  Macroscopic Quantum Systems and the Quantum Theory of Measurement (Progress in Statistical and Solid State Physics--In Commemoration of the Sixtieth Birthday of Ryogo Kubo) -- (Statistical Physics) , 1980 .

[67]  H. Stapp Locality and reality , 1980 .

[68]  E. Recami,et al.  On the physical nonexistence of signals going backwards in time, and quantum mechanics , 1980 .

[69]  K. Popper,et al.  Possible direct physical detection of de Broglie waves , 1981 .

[70]  N. Mermin Bringing Home the Atomic World: Quantum Mysteries for Anybody. , 1981 .

[71]  R. Voss,et al.  Macroscopic Quantum Tunneling in 1-μm Nb Josephson Junctions , 1981 .

[72]  R. Dicke,et al.  Interaction‐free quantum measurements: A paradox? , 1981 .

[73]  Nick Herbert FLASH—A superluminal communicator based upon a new kind of quantum measurement , 1982 .

[74]  O. C. D. Beauregard Disagreement with Garuccio, Popper and Vigier , 1982 .

[75]  G. Roger,et al.  Experimental Test of Bell's Inequalities Using Time- Varying Analyzers , 1982 .

[76]  W. Wootters,et al.  A single quantum cannot be cloned , 1982, Nature.

[77]  Peter W. Milonni,et al.  PHOTONS CANNOT ALWAYS BE REPLICATED , 1982 .

[78]  J. Vigier,et al.  New experimental set-up for the detection of de Broglie waves☆ , 1982 .

[79]  H. Stapp Bell's theorem as a nonlocality property of quantum theory , 1982 .

[80]  P. Grangier,et al.  Experimental Realization of Einstein-Podolsky-Rosen-Bohm Gedankenexperiment : A New Violation of Bell's Inequalities , 1982 .

[81]  Philippe H. Eberhard Constraints of determinism and of Bell's inequalities are not equivalent , 1982 .

[82]  D. Dieks Communication by EPR devices , 1982 .

[83]  J. Cramer The arrow of electromagnetic time and the generalized absorber theory , 1983 .

[84]  Relativistic quantum logic , 1983 .

[85]  N. David Mermin,et al.  Is the Moon There When Nobody Looks? Reality and the Quantum Theory , 1985 .

[86]  O. Costa de Beauregard On Some Frequent but Controversial Statements Concerning the Einstein-Podolsky-Rosen Correlations , 1985 .

[87]  Albert,et al.  Curious new statistical prediction of quantum mechanics. , 1985, Physical review letters.