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- Is theory around Delayed Choice remote polarization entanglement swapping of photons derived from TDSE or TISE?
Is theory around Delayed Choice remote polarization entanglement swapping of photons derived from Time Dependent Schrodinger equation (TDSE) or Time Independent Schrodinger equation (TISE)? I say the answer is no. I collectively group TDSE and TISE under the umbrella SE. And the following experiments are for us to use to discuss regarding the state of the art in entanglement theory/experiment:
A. High-fidelity entanglement swapping with fully independent sources
Rainer Kaltenbaek, Robert Prevedel, Markus Aspelmeyer, Anton Zeilinger (2008)
Abstract: Entanglement swapping allows to establish entanglement between independent particles that never interacted nor share any common past. This feature makes it an integral constituent of quantum repeaters. Here, we demonstrate entanglement swapping with time-synchronized independent sources with a fidelity high enough to violate a Clauser-Horne-Shimony-Holt inequality by more than four standard deviations. The fact that both entangled pairs are created by fully independent, only electronically connected sources ensures that this technique is suitable for future long-distance quantum communication experiments as well as for novel tests on the foundations of quantum physics.
B. Experimental delayed-choice entanglement swapping
Xiao-song Ma, Stefan Zotter, Johannes Kofler, Rupert Ursin, Thomas Jennewein, Časlav Brukner, Anton Zeilinger (2012)
Abstract: Motivated by the question, which kind of physical interactions and processes are needed for the production of quantum entanglement, Peres has put forward the radical idea of delayed-choice entanglement swapping. There, entanglement can be "produced a posteriori, after the entangled particles have been measured and may no longer exist". In this work we report the first realization of Peres' gedanken experiment. Using four photons, we can actively delay the choice of measurement-implemented via a high-speed tunable bipartite state analyzer and a quantum random number generator-on two of the photons into the time-like future of the registration of the other two photons. This effectively projects the two already registered photons onto one definite of two mutually exclusive quantum states in which either the photons are entangled (quantum correlations) or separable (classical correlations). This can also be viewed as "quantum steering into the past".
C. Bell's Theorem Without Inequalities
Daniel M. Greenberger; Michael A. Horne; Abner Shimony; Anton Zeilinger (1990)
Abstract: It is demonstrated that the premises of the Einstein–Podolsky–Rosen paper are inconsistent when applied to quantum systems consisting of at least three particles. The demonstration reveals that the EPR program contradicts quantum mechanics even for the cases of perfect correlations. By perfect correlations is meant arrangements by which the result of the measurement on one particle can be predicted with certainty given the outcomes of measurements on the other particles of the system. This incompatibility with quantum mechanics is stronger than the one previously revealed for two‐particle systems by Bell’s inequality, where no contradiction arises at the level of perfect correlations. Both spin‐correlation and multiparticle interferometry examples are given of suitable three‐ and four‐particle arrangements, both at the gedanken and at the real experiment level.
I am not debating the importance of SE to QM. What I am saying is that modern entanglement theory requires additional theory that cannot be directly traced back to the SE. And I am using what I consider the farthest possible elements of modern entanglement theory to demonstrate how far away the SE is. Those elements being:
i) Application of SE to polarization states of spin 1 photons;
ii) Creation of entangled photons pairs via parametric down conversion;
iii) Entanglement swapping by use of a Bell State Measurement (BSM) apparatus (requiring indistinguishable photon detections);
iv) Polarization entangling photons from independent sources;
v) Polarization entangling photons by a distant BSM operation;
vi) Polarization entangling photons after they cease to exist; and
vii) Creation of GHZ states (a bonus requirement).
Basically, I am disputing there is any direct derivation or connection of any of these well known and well tested phenomena with the SE. And in fact, since most of these were discovered prior to 2000, I would ask for references that precede this date. Here is a chapter from a 2023 book, entirely about the SE, which contains a chapter on the SE for photons:
A Schrödinger Equation for Light (Daniel R.E. Hodgson)
None of the above 7 items are discussed. However, there are numerous references to Maxwell's equations. Further, there are some basic derivations of an SE for the photon in his E25. That might count for i) above.
But I don't think there exists pre-2000 references reasonably connecting the SE to the experimental results of references A, B or C above. I am asking for those. If the authors of my references were able to deduce everything in their papers from the earlier works using the SE, where are those references?
For example: How do you get the 4 two-particle Bell states (with their Entangled polarization correlations) from the SE? That would be a good start. Bell didn't need anything like that in his 1964 paper: "With the example advocated by Bohm and Aharonov [1957], the EPR argument [1935] is the following. Consider a pair of spin one-half particles formed somehow in the singlet spin state and moving freely in opposite directions. ... " Presto, here's a Bell state, and no SE required.
So what is the point of even asking this question in the first place? It has been argued by @PeterDonis and others in another thread (and we have discussed off and on at various times) that any new interpretation that recreates the basic SE must naturally lead to predictions fully consistent with all existing entanglement experiments - without any need to explain how. That deduction doesn't really follow, because the entire point of a novel interpretation is to ADD "something" to existing canon in the way of explanation. Maybe that novel explanation itself contradicts an experiment! It should be clear that in the year 2000, the SE had long been left behind as a basis for most entanglement research. Things like quantum nonlocality (remote entanglement swapping) and quantum causality (delayed choice) have no practical analog in the various forms of the SE. So I'm not sure how anyone can make the proposed leap that I am criticizing.
So if someone wants to put forth a new interpretation of QM, to add to an already overloaded list, they at least better address my 3 references. Because you cannot dismiss the incredible theoretical advances of the past 30+ years as being an "obvious" derivation of the SE. And in fact, the SE is not mentioned in any of these references. You really wouldn't expect it too, either, as the well-discussed limitations of the SE as it can be applied to the photon does not naturally lead to the usual Bell states and their quantum nonlocality in the first place.
A. High-fidelity entanglement swapping with fully independent sources
Rainer Kaltenbaek, Robert Prevedel, Markus Aspelmeyer, Anton Zeilinger (2008)
Abstract: Entanglement swapping allows to establish entanglement between independent particles that never interacted nor share any common past. This feature makes it an integral constituent of quantum repeaters. Here, we demonstrate entanglement swapping with time-synchronized independent sources with a fidelity high enough to violate a Clauser-Horne-Shimony-Holt inequality by more than four standard deviations. The fact that both entangled pairs are created by fully independent, only electronically connected sources ensures that this technique is suitable for future long-distance quantum communication experiments as well as for novel tests on the foundations of quantum physics.
B. Experimental delayed-choice entanglement swapping
Xiao-song Ma, Stefan Zotter, Johannes Kofler, Rupert Ursin, Thomas Jennewein, Časlav Brukner, Anton Zeilinger (2012)
Abstract: Motivated by the question, which kind of physical interactions and processes are needed for the production of quantum entanglement, Peres has put forward the radical idea of delayed-choice entanglement swapping. There, entanglement can be "produced a posteriori, after the entangled particles have been measured and may no longer exist". In this work we report the first realization of Peres' gedanken experiment. Using four photons, we can actively delay the choice of measurement-implemented via a high-speed tunable bipartite state analyzer and a quantum random number generator-on two of the photons into the time-like future of the registration of the other two photons. This effectively projects the two already registered photons onto one definite of two mutually exclusive quantum states in which either the photons are entangled (quantum correlations) or separable (classical correlations). This can also be viewed as "quantum steering into the past".
C. Bell's Theorem Without Inequalities
Daniel M. Greenberger; Michael A. Horne; Abner Shimony; Anton Zeilinger (1990)
Abstract: It is demonstrated that the premises of the Einstein–Podolsky–Rosen paper are inconsistent when applied to quantum systems consisting of at least three particles. The demonstration reveals that the EPR program contradicts quantum mechanics even for the cases of perfect correlations. By perfect correlations is meant arrangements by which the result of the measurement on one particle can be predicted with certainty given the outcomes of measurements on the other particles of the system. This incompatibility with quantum mechanics is stronger than the one previously revealed for two‐particle systems by Bell’s inequality, where no contradiction arises at the level of perfect correlations. Both spin‐correlation and multiparticle interferometry examples are given of suitable three‐ and four‐particle arrangements, both at the gedanken and at the real experiment level.
I am not debating the importance of SE to QM. What I am saying is that modern entanglement theory requires additional theory that cannot be directly traced back to the SE. And I am using what I consider the farthest possible elements of modern entanglement theory to demonstrate how far away the SE is. Those elements being:
i) Application of SE to polarization states of spin 1 photons;
ii) Creation of entangled photons pairs via parametric down conversion;
iii) Entanglement swapping by use of a Bell State Measurement (BSM) apparatus (requiring indistinguishable photon detections);
iv) Polarization entangling photons from independent sources;
v) Polarization entangling photons by a distant BSM operation;
vi) Polarization entangling photons after they cease to exist; and
vii) Creation of GHZ states (a bonus requirement).
Basically, I am disputing there is any direct derivation or connection of any of these well known and well tested phenomena with the SE. And in fact, since most of these were discovered prior to 2000, I would ask for references that precede this date. Here is a chapter from a 2023 book, entirely about the SE, which contains a chapter on the SE for photons:
A Schrödinger Equation for Light (Daniel R.E. Hodgson)
None of the above 7 items are discussed. However, there are numerous references to Maxwell's equations. Further, there are some basic derivations of an SE for the photon in his E25. That might count for i) above.
But I don't think there exists pre-2000 references reasonably connecting the SE to the experimental results of references A, B or C above. I am asking for those. If the authors of my references were able to deduce everything in their papers from the earlier works using the SE, where are those references?
For example: How do you get the 4 two-particle Bell states (with their Entangled polarization correlations) from the SE? That would be a good start. Bell didn't need anything like that in his 1964 paper: "With the example advocated by Bohm and Aharonov [1957], the EPR argument [1935] is the following. Consider a pair of spin one-half particles formed somehow in the singlet spin state and moving freely in opposite directions. ... " Presto, here's a Bell state, and no SE required.
So what is the point of even asking this question in the first place? It has been argued by @PeterDonis and others in another thread (and we have discussed off and on at various times) that any new interpretation that recreates the basic SE must naturally lead to predictions fully consistent with all existing entanglement experiments - without any need to explain how. That deduction doesn't really follow, because the entire point of a novel interpretation is to ADD "something" to existing canon in the way of explanation. Maybe that novel explanation itself contradicts an experiment! It should be clear that in the year 2000, the SE had long been left behind as a basis for most entanglement research. Things like quantum nonlocality (remote entanglement swapping) and quantum causality (delayed choice) have no practical analog in the various forms of the SE. So I'm not sure how anyone can make the proposed leap that I am criticizing.
So if someone wants to put forth a new interpretation of QM, to add to an already overloaded list, they at least better address my 3 references. Because you cannot dismiss the incredible theoretical advances of the past 30+ years as being an "obvious" derivation of the SE. And in fact, the SE is not mentioned in any of these references. You really wouldn't expect it too, either, as the well-discussed limitations of the SE as it can be applied to the photon does not naturally lead to the usual Bell states and their quantum nonlocality in the first place.