Transactional interpretation

The transactional interpretation of quantum mechanics (TIQM) takes the psi and psi* wave functions of the standard quantum formalism to be retarded (forward in time) and advanced (backward in time) waves that form a quantum interaction as a Wheeler–Feynman handshake or transaction. It was first proposed in 1986 by John G. Cramer, who argues that it helps in developing intuition for quantum processes. He also suggests that it avoids the philosophical problems with the Copenhagen interpretation and the role of the observer, and also resolves various quantum paradoxes.[1][2] TIQM formed a minor plot point in his science fiction novel Einstein's Bridge.

More recently, he has also argued TIQM to be consistent with the Afshar experiment, while claiming that the Copenhagen interpretation and the many-worlds interpretation are not.[3] The existence of both advanced and retarded waves as admissible solutions to Maxwell's equations was explored in the Wheeler–Feynman absorber theory. Cramer revived their idea of two waves for his transactional interpretation of quantum theory. While the ordinary Schrödinger equation does not admit advanced solutions, its relativistic version does, and these advanced solutions are the ones used by TIQM.

In TIQM, the source emits a usual (retarded) wave forward in time, but it also emits an advanced wave backward in time; furthermore, the receiver, who is later in time, also emits an advanced wave backward in time and a retarded wave forward in time. A quantum event occurs when a "handshake" exchange of advanced and retarded waves triggers the formation of a transaction in which energy, momentum, angular momentum, etc. are transferred. The quantum mechanism behind transaction formation has been demonstrated explicitly for the case of a photon transfer between atoms in Sect. 5.4 of Carver Mead's book Collective Electrodynamics. In this interpretation, the collapse of the wavefunction does not happen at any specific point in time, but is "atemporal" and occurs along the whole transaction, and the emission/absorption process is time-symmetric. The waves are seen as physically real, rather than a mere mathematical device to record the observer's knowledge as in some other interpretations of quantum mechanics.

Cramer has used TIQM in teaching quantum mechanics at the University of Washington in Seattle.

Advances over previous interpretations

TIQM is explicitly non-local and, as a consequence, logically consistent with counterfactual definiteness (CFD), the minimum realist assumption.[1] As such it incorporates the non-locality demonstrated by the Bell test experiments and eliminates the observer dependent reality that plagues the Copenhagen Interpretation. Greenberger–Horne–Zeilinger state the key advance over Everett's Relative State Interpretation[4] is to regard the conjugate state vector of the Dirac formalism as ontologically real, incorporating a part of the formalism that, prior to TIQM, had been interpretationally neglected. Having interpreted the conjugate state vector as an advanced wave, it is claimed that the origins of the Born rule follow naturally from the description of a transaction.[1]

The transactional interpretation has similarities with the two-state vector formalism (TSVF)[5] which has its origin in work by Yakir Aharonov, Peter Bergmann and Joel Lebowitz of 1964.[6][7]

Debate

Being "atemporal", TIQM assigns ontological priority to events in pseudo-time. This appears to have acted as the foremost inhibition to mainstream acceptance of the interpretation and underpins Maudlin's (1996, 2002) objection.[8]

In his book, The Quantum Handshake, Cramer has added a hierarchy to the description of pseudo-time to deal with Maudlin's objection and has pointed out that some of Maudlin's arguments are based on the inappropriate application of Heisenberg's knowledge interpretation to the transactional description.[9]

Transactional Interpretation faces criticisms. The following is partial list and some replies:

1. “TI does not generate new predictions / is not testable / has not been tested.”

TI is an exact interpretation of QM and so its predictions must be the same as QM. Like the many-worlds interpretation (MWI), TI is a ‘pure’ interpretation in that it does not add anything ad hoc but provides a physical referent for a part of the formalism that has lacked one (the advanced states implicitly appearing in the Born rule). Thus the demand often placed on TI for new predictions or testability is a mistaken one that misconstrues the project of interpretation as one of theory modification.[10]

2. “It is not made clear where in spacetime a transaction occurs.”

One clear account is given in Cramer (1986), which pictures a transaction as a four-vector standing wave whose endpoints are the emission and absorption events.[11]

3. “Maudlin (1996, 2002) has demonstrated that TI is inconsistent.”

Maudlin's probability criticism confused the transactional interpretation with Heisenberg's knowledge interpretation. However, he raised a valid point concerning causally connected possible outcomes, which led Cramer to add hierarchy to the pseudo-time description of transaction formation, resolving the issue.[12][13][14][15][16]

4. "It is not clear how the transactional interpretation handles the quantum mechanics of more than one particle."

This issue is addressed in Cramer's 1986 paper, in which he gives many examples of the application of TIQM to multi-particle quantum systems. However, if the question is about the existence of multi-particle wave functions in normal 3D space, Cramer's 2015 book goes into some detail in justifying multi-particle wave functions in 3D space.[17]

See also

References

  1. 1 2 3 Cramer, John (1986). "The Transactional Interpretation of Quantum Mechanics". Reviews of Modern Physics. 58: 647–688. doi:10.1103/revmodphys.58.647.
  2. ↑ Cramer, John (1988). "An Overview of the Transactional Interpretation". International Journal of Theoretical Physics. 27: 227–236. doi:10.1007/bf00670751.
  3. ↑ A Farewell to Copenhagen?, by John Cramer. Analog, December 2005.
  4. ↑ Hugh Everett, Relative State Formulation of Quantum Mechanics, Reviews of Modern Physics vol 29, (July 1957) pp 454–462.
  5. ↑ Avshalom C. Elitzur, Eliahu Cohen: The Retrocausal Nature of Quantum Measurement Revealed by Partial and Weak Measurements, AIP Conf. Proc. 1408: Quantum Retrocausation: Theory and Experiment (13–14 June 2011, San Diego, California), pp. 120–131, doi:10.1063/1.3663720
  6. ↑ Y. Aharonov, P. G. Bergmann, J. L. Lebowitz, Phys. Rev. B, vol. 134, pp. 1410 ff., 1964
  7. ↑ Yakir Aharonov, Lev Vaidman: Protective measurements of two-state vectors, in: Robert Sonné Cohen, Michael Horne, John J. Stachel (eds.): Potentiality, Entanglement and Passion-At-A-Distance, Quantum Mechanical Studies for A. M. Shimony, Volume Two, 1997, ISBN 978-0792344537, pp. 1–8, p. 2
  8. ↑ Cramer's Transactional Interpretation and Causal Loop Problems, Synthese, Vol 150, Iss1, May 2006.
  9. ↑ The Quantum Handshake: Entanglement, Nonlocality and Transactions by John G. Cramer, Springer Verlag, 2015, ISBN 978-3-319-24642-0.
  10. ↑ The Quantum Handshake by John G. Cramer, p. 183: "No consistent interpretation of quantum mechanics can be tested experimentally, because each is an interpretation of the same quantum mechanical formalism, and the formalism makes the predictions. The Transactional Interpretation is an exact interpretation of the QM formalism. Like the Many-Worlds and the Copenhagen interpretations, the TI is a "pure" interpretation that does not add anything ad hoc, but does provide a physical referent for a part of the formalism that has lacked on (e.g. the advanced wave functions appearing in the Born probability rule and amplitude calculations). Thus the demand for new predictions or testability from an interpretation is based on a conceptual error by the questioner that misconstrues an interpretation as a modification of quantum theory. According to Occam's Razor, the hypothesis that introduces the fewest independent assumptions is to be preferred. The TI offers this advantage over its rivals, in that the Born probability rule is a result rather than an independent assumption."
  11. ↑ The Quantum Handshake by John G. Cramer, p. 183: The TIQM "pictures a transaction as emerging from an offer-confirmation handshake as a four-vector standing wave normal in three-dimensional space with endpoints at the emission and absorption verticies. Kastner has predicted an alternative account of transaction formation in which the formation of a transaction is not a spatiotemporal process but one taking place on a level of possibility in a higher Hilbert space rather than in normal three-dimensional space."
  12. ↑ Berkovitz, J. (2002). ``On Causal Loops in the Quantum Realm," in T. Placek and J. Butterfield (Ed.), Proceedings of the NATO Advanced Research Workshop on Modality, Probability and Bell's Theorems, Kluwer, 233–255.
  13. ↑ Kastner, R. E. (2006). "Cramer's Transactional Interpretation and Causal Loop Problems". Synthese. 150: 1–14. doi:10.1007/s11229-004-6264-9.
  14. ↑ Marchildon, L (2006). "Causal Loops and Collapse in the Transactional Interpretation of Quantum Mechanics". Physics Essays. 19: 422. doi:10.4006/1.3025811.
  15. ↑ The Quantum Handshake by John G. Cramer, p. 184: "Maulin raised an interesting challenge for the Transactional Interpretation by pointing out a paradox that can be constructed when the non-detection of a slow particle moving in one direction that modifies the detection configuration in another direction. This problem is dealt with by the TI ... by introducing a hierarchy in the order of the transactional formation ... Other solutions to the problem raised by Maudlin can be found in the references."
  16. ↑ The Quantum Handshake by John G. Cramer, p. 184: Maudlin also made the claim, based on his assumption that the wave function is a representation of observer knowledge, that it must change when new information is made available. "That Heisenberg-inspired view is not a part of the Transactional Interpretation, and introducing it leads to bogus probability argument. In the Transactional Interpretation, the offer wave does not magically change in mid-flight at the instant when new information becomes available, and its correct application leads to the correct calculation of probabilities that are consistent with observation."
  17. ↑ The Quantum Handshake by John G. Cramer, p. 184. Cramer's earlier publications "provided many examples of the application of the TI to systems involving more than one particle. These include the Freedman-Clauser experiment, which describes a 2-photon transaction with three vertices, and the Hanbury-Brown-Twiss effect,which describes a 2-photon transaction with four vertices. [Other publications contain] many examples of more complicated multi-particle systems, including systems with both atoms and photons. But perhaps the question posed above is based on the belief that quantum mechanical wave functions for systems of more than one particle cannot exist in normal three-dimensional space and must be characterized instead as existing only in an abstract Hilbert space of many dimensions. Indeed, Kastner’s "Possibilist Transactional Interpretation" takes this point of view and describes transaction formation as ultimately appearing in 3D space but forming from the Hilbert-space wave functions. ... The "standard" Transactional Interpretation presented here, with its insights into the mechanism behind wave function collapse through transaction formation, provides a new view of the situation that makes the retreat to Hilbert space unnecessary. The offer wave for each particle can be considered as the wave function of a free (i.e., uncorrelated) particle and can be viewed as existing in normal three-dimensional space. The application of conservation laws and the influence of the variables of the other particles of the system on the particle of interest come not in the offer wave stage of the process but in the formation of the transactions. The transactions "knit together" the various otherwise independent particle wave functions that span a wide range of possible parameter values into a consistent ensemble, and only those wave function sub-components that are correlated to satisfy the conservation law boundary conditions at the transaction vertices are permitted to participate in this transaction formation. The "allowed zones" of Hilbert space arise from the action of transaction formation, not from constraints on the initial offer waves, i.e., particle wave functions. Thus, the assertion that the quantum wave functions of individual particles in a multi-particle quantum system cannot exist in ordinary three-dimensional space is a misinterpretation of the role of Hilbert space, the application of conservation laws, and the origins of entanglement. It confuses the "map" with the "territory". Offer waves are somewhat ephemeral three-dimensional space objects, but only those components of the offer wave that satisfy conservation laws and entanglement criteria are permitted to be projected into the final transaction, which also exists in three-dimensional space."

Further reading

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