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Vatarescu, A. Quantum Rayleigh Annihilation of Entangled Photons and Quantum Local Realism. Encyclopedia. Available online: https://encyclopedia.pub/entry/94 (accessed on 16 June 2024).

Vatarescu A. Quantum Rayleigh Annihilation of Entangled Photons and Quantum Local Realism. Encyclopedia. Available at: https://encyclopedia.pub/entry/94. Accessed June 16, 2024.

Vatarescu, Andre. "Quantum Rayleigh Annihilation of Entangled Photons and Quantum Local Realism" *Encyclopedia*, https://encyclopedia.pub/entry/94 (accessed June 16, 2024).

Vatarescu, A. (2019, July 26). Quantum Rayleigh Annihilation of Entangled Photons and Quantum Local Realism. In *Encyclopedia*. https://encyclopedia.pub/entry/94

Vatarescu, Andre. "Quantum Rayleigh Annihilation of Entangled Photons and Quantum Local Realism." *Encyclopedia*. Web. 26 July, 2019.

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The interpretation of published experimental results intended to prove the existence of a quantum phenomenon of non-locality involving photonic entangled states did not take into consideration the existence of the quantum Rayleigh conversion of photons in dielectric media. This phenomenon leads to the existence of high levels of correlations between two independent photonic and linearly polarized quantum states generated after the entangled photons have been absorbed through the quantum Rayleigh conversion. Both pure and mixed individual states of polarization result in expressions normally associated with entangled photonic states, providing support for the view that the physical reality of quantum non-locality is highly questionable.

quantum
optcs
Rayleigh spontaneous emission
polarization states
correlations
locality

Over the past half-century, large amounts of resources have been invested in experiments based on photonic devices in order to prove the existence of the quantum non-locality by measuring expectation values of detected polarized photons that comply with various versions of Bell inequalities ^{[1]}^{[2]}^{[3]}^{[4]}^{[9]}^{[10]}^{[11]}^{[12]}^{[13]}^{[14]}. For some unexplained reason, from a scientific perspective, it has always been assumed that no other external or additional physical processes could take place in the experimental configurations. Yet, over the years, questions have emerged about the validity of the experimental model, from different directions ^{[5]}^{[6]}. The supporters of the theory of quantum non-locality ^{[7]} choose to ignore or denigrate these objections without addressing them directly ^{[8]}.

The concept of quantum non-locality in the context of photonic systems would cause a measurement carried out at location A to influence a measurement performed at location B. The requirement for this effect to take place is that the two photons – measured separately – had a joint interaction which left them correlated or in an entangled state. This combination of quantum non-locality and entanglement of photons would, allegedly, result in strongly correlated measurement outcomes ^{[1]}.

The relatively strong correlations between the detected states of polarizations of the two space-time separated photons ^{[1]} were considered to be a clear indication of an instantaneous collapse into an eigenstate of the wave function describing the two apparently entangled photons and, as a result, it was concluded that a non-local mechanism - of an yet unknown origin and nature - brings about a mutual influence between the two distant measurements. Overall, it is argued that those correlations disprove beyond any doubt the paradox pointed out by Einstein, Podolsky and Rosen (EPR), while complying with the uncertainty principle for each subsystem which would not allow simultaneous sharp values for two incompatible variables linked to the Pauli spin operators which do not commute.

The measured events of correlated pairs of photons are “extremely rare” ^{[1]}, with typical values of “slightly more than one event-ready signal per hour” ^{[2]}*.* Nevertheless, the interpretation of the experimental results of ^{[1]}^{[2]}^{[3]}^{[4]} failed to take into account the role played by the quantum Rayleigh conversion of photons ^{[9]}^{[10]}^{[11]}^{[12]}^{[13]}^{[14]} in their propagation through the dielectric media of optical fibers, beam splitters, polarization rotating devices and other dielectric elements comprising the experimental setups. While the classical Rayleigh scattering induced by perturbations of the refractive index is the major loss factor in optical fibers ^{[15]}, the quantum Rayleigh conversion of photons has been practically ignored although documented in early textbooks ^{[9]}^{[10]}.

In the case of only one photon propagating through a dielectric medium, the only process occurring is that of absorption of the photon by an oscillating dipole and spontaneous emission of one photon, which corresponds to the quantum Rayleigh conversion of photons (QRCP) which is outlined in Appendix A.

This article analyses the physical process of quantum Rayleigh scattering of photons through spontaneous emission which is bound to affect the propagation of the single photons originating from the same source and forming the components of entangled states ^{[1]}^{[2]}^{[3]}^{[4]} . Correlation functions - evaluated in Section 2 - are associated with the two independently and separately emitted qubits of photons, and deliver the same degree of high correlations for pure states and variable outcomes for mixed states. Additionally, each term of the commutative relations between the relevant Pauli operators in the context of the individual and separated photonic state vectors will vanish leading to the possibility of simultaneous measurements and the absence of an EPR paradox. The implications of replacing the physically eliminated entangled states of photons with individual and independent qubits are discussed in Section 3 and support the view of reference ^{[14]} objecting to the existence of quantum nonlocality. The conclusions summarizing the main results of this article point out the feasibility of explaining the published experimental - apparently supporting the concept of quantum nonlocality- by adopting a fully local approach based on a well-established physical process.

**2. Correlation functions**

As a photon enters a birefringent crystal and interacts with electric dipoles, the photon needs to be re-emitted into a polarization eigenstate so it can propagate in the same forward direction to reach the intended photodetector. If each of the individual photons of the initial pair is re-emitted into their original state of polarization and reaches its respective detector within the designated time interval for a coincidence count to be registered, then this physical process can be mistaken for the physically impossible case of the entangled photons having survived their propagation through the dielectric media without interacting with electric dipoles. Nevertheless, as photons acquire a phase shift as a results of their propagation, the probability of no dipole-photon interactions taking place even for a short distance of millimetres, is nil.

** ****2.1 Pure states of polarization **

Although the conventional definition of the correlation function – see ^{[16]} (Eq.13) – involves the same state of polarization reaching the two separate detectors, in the case of quantum Rayleigh spontaneous emission additional correlations can be defined between different states of polarization – possibly boosting the detection counts – for two different angles *φ** _{1}* and

*E _{c}* = ⟨ Ψ (

where the initial state vector of spontaneous emission │Ψ (*φ ** _{j}* )⟩ =

( *θ** _{j}* ) = │

where * _{1}* = │

( *θ _{1}* ) ⊗ ((

By inserting Eqs. (3) and (A3), along with the equalities ⟨ Ψ ( *φ** _{1}* ) │ Ψ (

*E _{c}*

*E _{c}* =

For *φ ** _{1}* =

The detection of photons having a polarization direction *e*_{k }* _{µ}* which is not aligned with the polarization filter

For initially identical states of photon polarization, that is *φ ** _{1}* =

**2.2 Mixed states of polarization**

The overall correlation for one step of spontaneous emission will be found by adding up probability-weighted correlation functions of Eq. (4) as the ensemble of polarizations states generated over a time interval corresponds to a mixed quantum state described by the density matrix elements *ρ _{m n}* (

The correlation function for the mixed state of an ensemble is evaluated similarly to Eq. (1) after using the transformation │Ψ (* φ* ) ⟩ → *p* (*φ*)] ^{1/2} │Ψ (* φ* ) ⟩ to obtain:** **

*E _{c}* =

where the first term reproduces the result for identical and independent qubits, i.e., *φ*_{ 1}_{ =}*φ ** _{2}* , with

As the expectation values of the operator products of Eq. (3) are found to vanish for identical pure states of Eq. (A3), │ Ψ (* φ *) ⟩ =* cos* *φ* │ *x * ⟩ + *sin* *φ * │ *y * ⟩, namely ⟨ Ψ (*φ* ) │_{1}* _{3}* │ Ψ (

⟨ Ψ (*φ* ) │[* _{1}* ,

The eigenstates of * _{1}* are superpositions of the eigenvectors of

3. **Physical aspects of simultaneous measurements of independent photons **

Since the same correlation functions are derived for independent and single qubits generated through quantum Rayleigh conversion of photons - from initially entangled polarized photons - as for the initially entangled photons, it follows that the violations of any type of relevant Bell inequalities will also take place in the same way. Yet, the correlations result from similar, if not identical, distributions of polarization states as opposed to what is conceptually believed to be a non-local quantum effect which has an unspecified nature but is being pursued because of vested interests.

Once the same correlation functions are derived using only states of polarizations emitted spontaneously by the quantum Rayleigh conversion of photons, no other physical processes is required to explain the experimental results.

Let us now consider a few characteristics associated with local realism ^{[6]} of quantum measurements in the context of quantum Rayleigh conversion of photons:

__Locality__ of measurements is supported by the use of single and independent photonic qubits emitted separately to explain the experimental results of apparently enhanced correlations of outcomes.

__Randomness __of experimental parameters stems from the quantum Rayleigh spontaneous emission that generates the projection from the polarization state │* x *⟩ of the input photons to the rotated polarization state │ Ψ (*φ* )⟩ = *cos* *φ** _{ }*│

__Realism __of values carried by the detected photons is indicated by the physical effect of the measuring operators on the detected photons in quantum states │ Ψ (*φ** _{ j }*) ⟩ of Eq. (A3) for which the two commutator terms of the two Pauli operators of Eqs. (6) vanish independently of each other. Thus, a physically meaningful identification of wavefunctions will enable simultaneous measurements of well-defined values.

The common view ^{[7]} holds that “the measurement of one component of the entangled state collapses the total wave function into a certain value which, in turn, affects instantaneously the second measured value.” Nonlocality is associated with the instantaneous collapse of the wave function. The “remarkable” correlation is revealed by a comparison of the two lists of measured data compiled at the two detection points as ethereal influences are said to be associated with the collapse of the wave function upon measurement. Yet, the experimental results can be explained without entangled states of photons which are destroyed by propagating through a dielectric medium and replaced by independent qubits of photon polarization.

The presentation of ^{[17]} (Ch.19) describes the Einstein, Podolsky and Rosen (EPR) view suggesting that there is no such thing as an uncaused random event, and the characteristic randomness of the quantum world originates at the very beginning of each macroscopic event. By contrast, the conventional view [1] would have a quantum description in which the state vector evolves in a perfectly deterministic way from its initial value, and randomness enters only at the time of measurements. The quantum Rayleigh spontaneous emission is, in fact, a random process at the generating stage followed by evolution described by the Schrödinger equation, thereby supporting the EPR view.

It is emphasized in ^{[5]} that “Bell violation has less to do with quantum theory than previously thought, but everything to do with entanglement.” Actually, there is no need for entangled states to measure strong correlations of polarization between spontaneously emitted photons detected far apart from each other or non-locally.

It is claimed in ^{[16]} that “… the violation of Bell inequalities can be seen as a detector of entanglement that is robust to any experimental imperfection: as long as a violation is observed, we have the guarantee, independently of any implementation details, that the two systems are entangled.” Yet, this is not the case with single and independent qubits which can reproduce the same results.

For the entangled state of two polarized photons shown in the inset of ^{[1]} (Fig. 1), quantum mechanics predicts that the polarization measurements performed at the two distant stations will be strongly correlated ^{[1]}*. *But the same prediction also applies to two independent, single qubits which are generated through quantum Rayleigh spontaneous emission from initially identical photons propagating in different directions through dielectric media such as optical fibers.

Additionally, reference ^{[18]} “…rules out outcome-dependent causal models without additional assumptions in any scenario with more than two settings. A direct causal influence from one outcome to the other can therefore not explain quantum correlations.”

The analysis presented in this article is based on physically meaningful interactions of quantum Rayleigh conversion of photons and supports reference [6] in its statement that “There is no mystery. There is no quantum nonlocality”. It is the physical process that gives rise to a wave function. The opposite approach of relying on mathematical complexities to conjure up physical processes is bound to generate “‘quantum mysteries”.

As for the quantum key distribution between the two measuring units ^{[19]}, it is determined by the local distribution of the mixed state of spontaneously emitted photons and the measurement setup of the dielectric devices involved in the polarization filtering with its eigenstates capturing the projected single qubits. However, errors will appear because of the statistical nature of the correlations between polarized photons.

The physical approach presented in this article can also explain the experimental results of reference [5] by invoking the quantum Rayleigh conversion of photons - see Appendix A below. This contrasts with the opinion article of reference ^{[20]} which dismisses the results of ^{[5]} as being irrelevant to the question of whether or not the quantum nonlocality is feasible.

**4. Conclusions**

Quantum Rayleigh conversions of photons in dielectric media provide a physically meaningful explanation for experimental results of statistical and “nonlocal” quantum correlations supposedly associated with entangled states of photons. Single and independent qubits replace the annihilated entangled states and provide identical correlation functions between two sets of polarization-related measurements carried out far apart from each other. This physically meaningful analysis raises significant doubts about the existence of photonics-based quantum nonlocality processes.

**Appendix A-** **Spontaneous emission and polarization rotation induced by quantum Rayleigh conversion of photons**

The probability of emitting a photon with momentum ** k** and polarization

*γ _{sp} *(

with ** d** denoting the electric dipole moment vector which is excited by an optical field of the same polarization,

The angular distribution of an accumulated number of spontaneously emitted photons *N _{s p}* (D

*N _{s p}* ( Δ

with *φ _{ e m} * the emission angle between the dipole

For *e*_{k }* _{µ}* •

The generic eigenstates of polarization associated with spontaneous emission through quantum Rayleigh conversion of photons on the two-dimensional Hilbert space ℋ will take the form of single and independent qubits │ Ψ (* φ ** _{ e m}* ) ⟩ identified as:

│ Ψ (* φ ** _{e m}* ) ⟩ =

These state vectors with polarization angles *φ** _{ e m}* in the range -π / 2 ≤

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