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Many future directions of scientific endeavors depend on quantum theory and the precise interpretation and significance of the entanglement of quantum-particles. This interpretation depends in turn on the physical meaning of so called Bell-tests that are mostly performed using entangled photons and randomly switched polarizers to measure their polarization at distant locations. This paper presents a detailed critique of the well known theory of Bell tests given by Clauser-Horne-Shimony-Holt (CHSH). It is demonstrated that several important steps of the CHSH derivations contain serious inaccuracies of the underlying physics and probability theory and even a calculus error. As a consequence, the Bell-CHSH theory cannot be used to demonstrate extreme and opposite interpretations of entanglement such as super-luminal influences or alternatively super-determinism that cast aspersions on Einstein’s concepts of locality and separability.

If one asks for a list of significant problems in branches of current science, one is bound to find pointers toward developments of quantum mechanics that include the concept of quantum entanglement. Quantum computing, quantum teleportation and even topics in biology are using quantum entanglement for their basic considerations. The concept of quantum entanglement was defined and described by Schroedinger and has been shown to represent a main feature of quantum theory itself.

Quantum entanglement of isolated and distant pairs has been experimentally demonstrated by Kocher and Commins [

The most intriguing questions related to the Bell theorem emerged from measurements by Aspect [

The basic question of the possible existence of superluminal influences is actually contained in many a scientific theory, for example that of Newton, and has seen many discussions and opposing views (of Leibnitz, in Newtons case). Since the event of Einstein’s relativity, ideas of superluminal influences became unthinkable, but have been revived in the last decades based on Bell’s Theorem and the experimental Bell-tests. Recently a sensational Bell-test has been performed by Zeilinger and related groups [

To be sure, no direct proof has ever been provided by any experiments. We do not have any measurement equipment available that can claim to transmit information faster than the speed of light in vacuum and thus we cannot measure superluminal influences in one single shot, as is well known from Einstein’s special theory of relativity. The recent ideas of superluminal influences are based on the statistical results underlying the Aspect-Zeilinger type of experiments. These researchers claim that the absolute randomness and ultrafast switching between their distant measurements provides the definite proof for their assertions. This fact has even been discussed in popular TV-shows such as “Einstein’s Quantum Riddle”—NOVA, which describes the Einstein-Podolsky-Rosen-type (EPR) experiments that are the basis for the work of Aspect [

I show in this paper, that among other factors there are certain aspects of the random switching that render Bell-tests questionable. In fact, such switching was not included in any direct way into the theories that describe Bell tests, but has only been recommended to the experimenters in order to support Einstein locality. To demonstrate these facts, I discuss in great detail and in fairly elementary mathematical terms, the important theoretical framework of Clauser, Horne, Shimony and Holt (CHSH) [

Each of the following sections starts with verbatim-quotes or at least extremely faithful descriptions of the most relevant definitions, assumptions, inequalities and corollaries given in the original CHSH work. The criticisms and comments follow.

It is demonstrated that the main results of CHSH are based on assumptions lacking generality and accuracy and that their mathematical and physical steps contain several serious problems and even a calculus error. Their results are further invalidated by their lack of use of modern probability theory and particularly the work of Vorob’ev [

My criticism (of the CHSH theorem that has been scrutinized for more than 50 years) may appear too harsh and even suspect to some, because physically speaking, the theorem is based on innocuous and plausible assumptions. Furthermore, the theorem is undoubtedly correct within certain mathematical frameworks. The physical consequences of the theorem, however, are such that only the extremes of super-luminal effects and/or super-determinism appear as possible explanations. This fact opens the question whether the physical assumptions to derive the theorem are really that innocuous and whether the mathematical premises correspond to the physics of actual experiments (see also [

The seriousness of this question is demonstrated below by explicit counter-examples to the CHSH theory, including one that invalidates the reasoning in the TV-show “Einstein’s Quantum Riddle”—NOVA.

“—Consider an ensemble of correlated pairs of particles moving so that one enters apparatus I a and the other apparatus I I b , where a and b are adjustable apparatus parameters. In each apparatus a particle must select one of two channels labeled +1 and −1. Let the result of these selections be represented by A ( a ) and B ( b ) , each of which equals ±1 according as the first or second channel is selected.”

To work within the aims of Bell-CHSH, we are bound to use Einstein-type space-time (or, in approximation, space and time) physics. Thus, Bell-CHSH have replaced the operators and eigenvalues of quantum theory by functions A ( a ,... ) , B ( b , ... ) with the “ ... ” being not yet fully specified, but later related to the information λ from a source (see below).

The choice of two integer numbers to define two channels and the codomain of the corresponding functions A , B = ± 1 is innocuous and contradiction-free if indeed only one pair of apparatus parameters (fixed a , b ) is in discussion. However, the identical choice of +1 or −1 for all possible equipment (apparatus) settings and in particular the 4 different equipment settings used by CHSH (see below) represents an inaccuracy that leads to inconsistencies, because channels pointing into different directions are denoted by the same integer. The application of integer algebra leads, in fact, to direct contradictions, as is shown in expression (5) below.

The inaccuracy of CHSH (and Bell) to deal with only 2 equipment settings, while the bulk of their paper deals with 2 settings in each station, is further aggravated by the random switching between the settings in each station: a , a ′ in I a and b , b ′ in I I b . (Please note that we are using throughout the symbols a , a ′ and b , b ′ for the polarizer or magnet settings, as is usual in more recent publications. CHSH have used different symbols in their original paper.) The random switching had been suggested to the experimenters already by Bell and was realized by Aspect and coworkers [

However, the possibility of random switching has not been included into the mathematical formalism of the theories of Bell and CHSH. From the viewpoint of probability theory, they needed to introduce random variables j , j ′ with the possible outcomes j = a , a ′ and j ′ = b , b ′ in the respective stations. Thus, it is nontrivial to write the functions A , B in terms of these random variables and to equate all possible outcomes to ±1: A ( j ,... ) = ± 1 and B ( j ′ ,... ) = ± 1 , because the +1 or −1 may then indeed describe channels that point in different directions, depending on the actual setting outcome. That inconsistency is hidden in the Bell-CHSH-type theories, because they only deal with the actual outcomes a , a ′ ; b , b ′ and leave the switching reserved for the experimenters.

We, therefore, ask why different geometric equipment-arrangements need only be described by two integer numbers and follow their algebra? In the authors’ opinion, this oversimplification has been accepted by almost everyone, because of the illusion that we deal with something analog to the eigenvalues in quantum mechanics, while the Bell and CHSH formalism must not be quantum mechanical as emphasized by both Bell and CHSH (see next section below).

Experiments with polarized photons are usually characterized by descriptions such as [horizontal, a, …] instead of just +1 and [vertical, a, …] instead of −1 for a given setting a and analogous notations for the other settings. Thus, the experimenters imply a connection between the definition of horizontal or vertical to the equipment setting directions a (or b etc.). A more precise theoretical notation would, therefore, use horizontal^{a} and vertical^{a} and similar notations (such as horizontal^{b}) for the other settings, if one wishes to recognize the fact that the polarizer direction co-determines what is meant by horizontal and vertical.

Wigner [

Strictly speaking, one may only use the judgements “equal” and “not-equal” for parallel polarizers or Stern-Gerlach magnets in both stations. It is still possible to introduce different definitions such as horizontal^{a} and vertical^{b}^{'} in the respective separate stations. However, a precise notation would then also use superscripts such as equal^{a}^{, b'} or not-equal^{a}^{, b'} and similar superscripts for other settings. The use of superscripts from both stations is completely acceptable, because the notions of equal and not-equal can only be introduced after merging the data from both stations. Thus, one cannot exclude probability measures for the results equal and not-equal that are functions of the polarizer-settings of both stations and even of the angle between those settings. The standard objection that experimenters Alice and Bob in the respective stations know nothing about each other does simply not apply to the theoretician who deals with the merged data from both EPRB stations and compares them.

Similarities with relativity theory do surface here. If we have two spaceships with pilots Alice and Bob, respectively, who know absolutely nothing of each other, no correlation of any physical processes in the spaceships can ever be found. The times displayed by their respective clocks are unknown until investigated, for example, by light-beams tracking the spaceships; alternatively the clocks may be compared when the spaceships are brought together. Only in these ways may their clocks be correlated and found to depend on the difference of their velocity-histories (see also [

As done with the velocities in relativity, one may also fix the polarizer in one station and vary the angle between the polarizers settings (see Appendix and references [

Summarizing, one can state that the Bell-CHSH choice of A , B = ± 1 , implying that the function values can be handled as two integer numbers for all possible equipment settings, oversimplifies the actual physical facts of the Einstein-Podolsky-Rosen (EPR) type experiments. The extensive repair work of Wigner and d’Espagnat represents a major improvement, but did not demonstrate a general validity of the CHSH work, particularly not for pair measurements with multiple random polarizer settings on both sides (as shown in detail in sections below).

“—Suppose now that the statistical correlation of A ( a ) and B ( b ) is due to information carried by and localized within each particle, and that at some time in the past the particles constituting one pair were in contact and communication regarding this information. The information, which emphatically is not quantum mechanical, is part of the content of a set of hidden variables, denoted collectively by λ . The results of the selections are then to be deterministic functions A ( a , λ ) and B ( b , λ ) . Locality reasonably requires A ( a , λ ) to be independent of the parameter b and B ( b , λ ) to be likewise independent of a, since (sic) the two selections may occur at an arbitrary great distance from each other.”

We only note a minor inaccuracy: λ is defined as a “set of hidden variables” and certainly may be used as such. However, in most of what follows in the CHSH paper, the same symbol λ is used for the possible values of that hidden variable, which represent Einstein’s elements of physical reality. This twofold meaning of λ has led to some confusions in the literature. We attempt to present all the following explanations in a way that avoids confusion. However, we still continue to use λ with the dualistic meaning that it has in the CHSH paper (variable as well as value of variable), in order not to deviate too much from their notation.

“—Finally, since the pair of particles is generally emitted by a source in a manner physically independent of the adjustable parameters a and b, we assume that the normalized probability distribution ρ ( λ ) characterizing the ensemble is independent of a and b.”

The possible equipment settings a , b are still regarded as “adjustable parameters” that somehow also encompass the random switching. However a , b as well as all other equipment settings are used in the equations below as given. As mentioned, the introduction of random variables j = a , a ′ ; j ′ = b , b ′ is a necessity if random switching ought to be included. Furthermore we need to introduce a probabilistic tool that accounts for the physical fact that measurements with different setting pairs in any given station cannot occur simultaneously. The kinematics of random switching and any dynamics of the many body physics involved in the interactions between incoming particles and measurement equipment (see also reference [

The only way to cover such a situation consistently with a classical probability theory, such as the framework of Kolmogorov, is by use of stochastic processes [

This latter fact becomes visible in the immediately following mathematical steps of CHSH. They use in all their algebraic expressions the identical value of λ , but now for different pair-functions that correspond to different pair measurements as well as different polarizer setting-pairs. This procedure has been justified in two ways. First, by counterfactual reasoning of the kind “had we measured with a different setting pair, we would have encountered the same λ . We discuss this way in our criticism following the mathematical steps and the second justification in more detail afterwards.

Defining the correlation function

P ( a , b ) = ∫ Γ A ( a , λ ) B ( b , λ ) ρ ( λ ) d λ , (1)

where Γ is the total λ space, we have

| P ( a , b ) − P ( a , b ′ ) |

≤ ∫ Γ | A ( a , λ ) B ( b , λ ) − A ( a , λ ) B ( b ′ , λ ) | ρ ( λ ) d λ (2)

= ∫ Γ | A ( a , λ ) B ( b , λ ) | [ 1 − B ( b , λ ) B ( b ′ , λ ) ] ρ ( λ ) d λ (3)

= ∫ Γ [ 1 − B ( b , λ ) B ( b ′ , λ ) ] ρ ( λ ) d λ (4)

The steps from Equation (2) to Equation (4) use the axioms of integer numbers as well as the concept of the absolute value that have no obvious validity for the more general outcomes of horizontal and vertical and “products” of them. This fact does not matter for Equation (1), because we may adopt a convention to just subtract the numbers of equal and not-equal products as Wigner did. However, the algebraic steps from Equations (2) to (4) lead to the product:

B ( b , λ ) B ( b ′ , λ ) (5)

that now exhibits identical λs for two elements of reality that must be, generally and physically speaking, different, because both functions B symbolize measurements in the same station for different settings. Here we encounter a spectacular failure of the counterfactual reasoning and the assumption that the same λ may be used in the mathematical expressions above. Expression (5) is definitely a red flag for the basic assumptions that govern the domain and co-domain of the Bell-CHSH functions and their products.

Bell, CHSH and their followers have attempted to circumvent some criticism of the counterfactual arguments in the following way, which agrees also with the main reasoning in references [

Because λ represents the possible outcome-value of measurements, the claim is made that one can reorder these possible outcomes in such a way that about all the actual outcomes may be arranged in quadruples, each with the same value λ n to obtain the following inequality:

− 2 ≤ A ( a , λ n ) B ( b , λ n ) − A ( a , λ n ) B ( b ′ , λ n ) + A ( a ′ , λ n ) B ( b , λ n ) + A ( a ′ , λ n ) B ( b ′ , λ n ) ≤ + 2. (6)

where n = 1 , 2 , 3 , ⋯ , N , with N being a large number. Inserting all possible values of ±1 for the functions A , B supplies immediate verification. CHSH correctly have deduced from the random switching that Γ , the set of all possible λ n , must be independent of the equipment-settings, because of Einstein locality. They maintain, as the majority of experts do, that this fact justifies the reordering of data into a large number of quadruples each with the same outcome-value λ n . We will see below that this type of reordering indeed leads to an inequality that is only slightly different from the one derived by CHSH. As and aside, the possibility of reordering is actually mathematically only guaranteed for countable values of λ n . If the variable λ represents a continuum of some form, reordering may not be a valid procedure [

The additional reasons will be discussed in detail when connecting the CHSH-Bell-type inequalities to quantum theory and the actual experiments after inequality (11) below. These reasons follow from the findings of the mathematician Vorob’ev and are also explained in the Appendix. We first proceed, however, with the derivation of the CHSH inequalities.

CHSH use the following assumptions and equations to derive their original inequality from the inequality derived in Equations (1) - (4).

CHSH assume P ( a ′ , b ) = 1 − δ with 0 ≤ δ ≤ 1 and deduce

∫ Γ − ρ ( λ ) d λ = δ 2 (7)

with Γ − representing the set of all λ for which A ( a ′ , λ ) = − B ( b , λ ) . In addition CHSH imply

δ = − 2 ∫ Γ − A ( a ′ , λ ) B ( b ′ , λ ) ρ ( λ ) d λ , (8)

CriticismEquation (8) is only valid if also P ( a ′ , b ′ ) = 1 − δ . CHSH assume Γ − to be independent of the setting-pairs, which is incorrect. In this way they derive the following inequality.

“And therefore

| P ( a , b ) − P ( a , b ′ ) | ≤ 2 − P ( a ′ , b ) − P ( a ′ , b ′ ) ” (9)

Although a calculus-error was made to derive this original CHSH inequality (9), the error is largely inconsequential, because it is removed by the additional precondition that P ( a ′ , b ′ ) = 1 − δ , which is just more restrictive. This original CHSH inequality does, however, still suffer from the problems with the product (5) given above.

The nowadays mostly used variation of the CHSH inequality is not encumbered by the latter problem and is only somewhat “weaker” than (9):

| P ( a , b ) − P ( a , b ′ ) + P ( a ′ , b ) + P ( a ′ , b ′ ) | ≤ 2. (10)

This inequality follows immediately from inequality (6) by summation over all n with 1 ≤ n ≤ N . It does involve the reordering discussed above.

CHSH made the connection of their inequality to quantum theory by noting that P ( a , b ) is a function of b − a . This function depends on the actual entanglement (pair-correlations) and is typically given by − cos ( b − a ) and similar functions for the pairs a , b ′ , a ′ , b and a ′ , b ′ , which thus are functions of the angle Δ between the polarizer settings; a result that is obtained by quantum theory and also corroborated experimentally. CHSH further note that Equation (9) can be written by using only three differences resulting in three numbers that commonly are called Bell- or CHSH-angles. This fact follows from the cyclical arrangement of the CHSH polarizer settings, which means that three setting pairs fully determine the fourth. CHSH arbitrarily chose α = b − a , β = b ′ − b and γ = b − a ′ to obtain CHSH Equation (1b):

| P ( α ) − P ( α + β ) | ≤ 2 − P ( γ ) − P ( β + γ ) (11)

Seen from the viewpoint of rotational invariance, the angles between the polarizer settings indeed appear as the important physical variables, while the setting directions for themselves do not [

Vorob’ev’s work [

The term “cyclicity” expresses the precise appearance and recurrence of the equipment settings in the different terms of inequalities such as (10), which according to Vorob’ev are a sine qua non for the constraints that can be deduced in form of inequalities or otherwise. As a consequence of the cyclicity only three of the Ps in inequality (10) (e.g. P ( a , b ) , P ( a , b ′ ) , P ( a ′ , b ) ) may be chosen freely within their given codomain − 1 ≤ P ≤ + 1 , the fourth, P ( a ′ , b ′ ) , cannot be freely chosen, which is the exact reason for the constraints that are expressed by the CHSH inequality.

CHSH were obviously not aware of the work of Vorob’ev [

This cyclicity, necessary for any constraint on the expectation values, is usually not mentioned in discussions of Bell-type and CHSH-type inequalities, because most of these discussions stop at inequality (10) and do not continue to describe the link with quantum theory and experiment in any detail. Inequality (10) contains the cyclicity automatically. When the step to use Bell- and CHSH-angles is taken, this is no longer the case and the inequality (11) is then invalid for the following reasons.

The choice of the three CHSH angles α , β , γ to obtain inequality (11) is arbitrary and a multitude of other choices could have been made to obtain inequalities different from (11). Their choice also does not guarantee the cyclicity of the original equipment settings. In fact, going back from inequality (11) to inequality (10), one can choose for each term an infinity (cardinality of the real numbers) of non-cyclical setting arrangements [ a ″ , b ″ ; a ‴ , b ‴ ; a i v , b i v ; a v , b v ] that express the same four angles:

b ″ − a ″ = b − a ; b ‴ − a ‴ = b ′ − a ; b i v − a i v = b − a ′ and b v − a v = b ′ − a ′ . (12)

For these modified equipment settings, a CHSH inequality does not exist, because of the lacking cyclicity.

The claim of using completely random polarizer settings in references [

Based on the findings in the section “Removal of the Vorob’ev cyclicity”, it will be shown immediately that measurements with large numbers of random polarizer settings leave only negligibly few setting combinations for which inequality (11) remains indeed valid and we will discuss in the remarks at the end of this section how even these few exceptions may be dealt with to avoid any vestige of hints toward instantaneous influences between islands.

Note that the following counterexamples to the validity of inequality (11) do not contest the independence of the set Λ of all λs from the polarizer settings. The counterexamples are merely based on the use of a much larger number of random settings and in some cases on the fact that the correlation functions P are by law of nature invariant to rotations of the polarizer-pairs involved in any specific pair-measurement, while the Vorob’ev cyclicity represents a mathematical abstraction that is not subject to laws of nature.

First, use a large number of completely random polarizer settings in both measurement stations (wings). In this case we encounter, with only negligible probability, measurement-pairs that exhibit CHSH angles. We may select these measurements-pairs in order to form a CHSH-quadrupel. However, even among these selected quadruples, it is only a negligible number that can be arranged into a Vorob’ev cyclicity. Thus the necessary cyclicity that validates (11) is rarely encountered (with probability close to 0). All of this follows immediately from the algebra discussed in the subsection “Removal of the Vorob’ev cyclicity”. We further discuss in the remarks below, how even this negligible set of measurements that form a Vorob’ev cyclicity may be dealt with.

Second, use again a large number (instead of just two as the Aspect- and Zeilinger-groups do) of completely random polarizer settings in one of the EPRB wings and use corresponding settings in the other wing that conserve (with equal frequency of occurrence) the 4 CHSH angles between the two polarizer directions and thus the 4 pair correlations P. The overwhelming majority of the corresponding CHSH-quadruples will again not exhibit any Vorob’ev cyclicity as explained above and may thus violate inequality (11). Large numbers of such measurements may indeed be performed by using the techniques of Giustina et al. [

As mentioned, two polarizer settings are indeed switched randomly on each island in the NOVA—TV-show and in references [

It is informative in this context, to consider how the equipment settings for the measurements in ordinary space are entering the operators that act on the Hilbert-state-vectors of quantum theory. For EPRB experiments with spin 1 2 particles, we require a tensor product of two Pauli matrices acting on the tensor product of spinors. One Pauli matrix (related to the measurements performed with apparatus I) may be chosen corresponding to an arbitrarily defined coordinate system that describes an arbitrary magnet-setting in ordinary space. The second Pauli matrix (related to apparatus II) is not entirely arbitrary but must account for the experimentally given Bell-CHSH angle. These facts demonstrate the Achilles heel of the work of Bell and CHSH: The validity of their inequality requires a particular cyclicity of the equipment settings in ordinary space. The choice of the quantum operators in relation to these equipment settings is, on the other hand, to a large extent arbitrary and requires only the conservation of certain vector products that result in the same Bell-CHSH angles but do not necessarily correspond to cyclical equipment settings. This fact opens the possibility of violations of the Bell-CHSH type inequalities.

As another counterexample that violates (11), consider the use of a fixed setting in one measurement station (wing) and arbitrary random settings in the other, as described in more detail in Appendix. This experimental arrangement permits us to obtain setting pairs that have the same Bell-CHSH angles but no cyclicity that imposes any restrictions whatsoever [

It is important to note that the quantum results for the pair correlations P as well as the corresponding experimental results are invariant under rotations in ordinary three-dimensional space. The specific Vorob’ev cyclicity used by CHSH for the four measurement pairs is not invariant under rotations of the separate setting pairs. In addition, the four-pair inequality (6) represents, as mentioned above, a mathematical construct that includes reordering of the λs and does not follow any natural symmetry-law. This latter fact permits the removal of the Vorob’ev cyclicity by the following plausible counterexample.

Link the frame of reference to the distant stars, and consider the rotation of the polarizer settings with the rotation of the earth. This rotation will also remove the cyclical arrangement of the terms in (6) and, therefore, any CHSH constraint, while it will leave the pair correlations P unchanged. The NOVA—TV-show does not discuss the rotation of the earth relative to the stars.

We may ask ourselves what it means when the quadruple-cyclicity indeed exists for some subset of the data or even for about all of them?

Counterexample 3 relates to the most precise EPRB-measurements ever performed to the authors’ knowledge. However, due to the fixing of the polarizer setting on one side, the cyclicity is completely removed and inequality (11) is, therefore, not valid.

Counterexample 4 applies directly to the Aspect-Zeilinger-type of experiments. Rotation of the polarizer settings does certainly remove some of the cyclicity. It does also leave the possibility for some remaining cyclical or almost cyclical rearrangements of CHSH quadruples. However, a typical experimental run lasts for about one hour, which leads to significant angular changes in a system rotating with Earth. That rotation (or any other relevant rotation) together with the need of reordering the λs and the need to use consistent definitions of horizontal and vertical (as emphasized in Subsection 2.2) may lead to considerable violations of the cyclicity. Inequalities (11) and (9) have, thus, lost their theorem-character and become rather a multivariate Monte Carlo approximation problem. This fact means, in turn, that the experiments and measurements need not only be investigated with respect to how much they deviate from the originally fixed upper limit 2, but need also be investigated with respect to their, often significant, deviation from the results of quantum theory that have usually been ignored.

There are important (with respect to clarification and explanation) experiments that have not yet been performed. Assume, for example, that we have 4 Aspect-Zeilinger-type experiments with four setting pairs a , b ; a , b ′ ; a ′ , b and a ′ , b ′ and also four sources of entangled pairs that may all be run simultaneously. Select from the runs of the 4 pair-experiments the subset C of data for which indeed the simultaneous quadruple measurement-outcomes are equal for all measurements with equal polarizer settings. This subset C fulfills then inequalities (9) as well as (11). The quantum result for this subset must obviously also fulfill the inequalities because otherwise it would contradict algebra and the measurements (see [

Last but not least, I would like to comment about the fact that for the experiments of the Aspect-Zeilinger-type, the “closure of the cyclical arrangement is not guaranteed by the simultaneity of the measurements of CHSH quadruples, but only involves sequential measurements of pairs collected with synchronized clock-pair-readings. For such sequential pair-measurements, many variations of possible violations have been suggested in the past. For example, the two-dimensional vector stochastic processes from Subsection 4.2 remove, at least in principle, any cyclicity, because the pair measurements are performed at different times and any dependency of the relative pair-outcomes on measurement times will remove the cyclicity. Violations are particularly easy to construct, when only small subsets of the totality of measurements can be arranged in cyclical form, as is the case for all of the above counterexamples.

The possibility of geometric phases that also prevent the closure of the cyclicity (as shown in FigureA1 of the Appendix) was recently added as an additional option to the previously existing extensive list of possible violations [

In summary, the reported violations of CHSH inequality (1b) (identical to (11) above), are actually no violations at all for all the experiments and measurements that do not exhibit a Vorob’ev cyclicity as clearly shown in counterexample 3. The measurements by Kwiat and coworkers (see Appendix) represent the most accurate Bell-test yet performed. However, these measurements exhibit no cyclicity and, therefore, are not subject to any constraint.

Furthermore, the CHSH constraints are, generally speaking, diminished as demonstrated in counterexamples 1, 2, 4, because of the limited presence of cyclicities that are a necessary condition for CHSH inequality 1b. This fact adds many more possibilities to the already previously published deficiencies of CHSH-Bell-type inequalities when applied to actual experiments (see also the work of Kupczynski [

The well known CHSH results [

The author declares no conflicts of interest regarding the publication of this paper.

Hess, K. (2021) What Do Bell-Tests Prove? A Detailed Critique of Clauser-Horne-Shimony-Holt Including Counterexamples. Journal of Modern Physics, 12, 1219-1236. https://doi.org/10.4236/jmp.2021.129075

The function products in all Bell-CHSH-type inequalities contain a cyclicity that the mathematician Vorob’ev [

It turns out that the cyclicity may rather easily be removed in view of Equation (11), because it is not the single polarizer settings that are important for the statistics of the outcomes but only the angle between them.

The most straightforward removal of the Vorob’ev cyclicity is accomplished by the experimental choice of a fixed polarizer setting in one wing as shown in FigureA2. For purposes of illustration, imagine again that the different lengths of the lines between the functions relate to the joint pair probability-distributions. Because they may now all be different and because of the lack of a cyclicity, there exists no constraint in form of a CHSH inequality (see also [

The fact that such a rather straightforward removal of the cyclicity removes also all restrictions that the CHSH inequality and all other related inequalities impose, has received little attention by the majority of researchers in this field. Instead they have concentrated on other conditions to derive the inequalities,

conditions such as “Bell locality” or the “complete randomness” and the “free will” related to setting choices, conditions that are neither necessary nor sufficient for validations or violations of the inequalities.

Experiments corresponding to this precise situation, experiments that violate the CHSH inequality with extremely high precision (probably the highest yet achieved), have been performed by Kwiat and coworkers [

The agreement with the quantum result, corresponding to the very high visibility of V = 99.6 ± 0.3 % is, however, not surprising. There exists, in this case, no valid CHSH inequality that would put any constraints on the measurement results. The explicit proof of this fact is straightforward: just insert the settings of FigureA2 into inequalities (10) or (11), while conserving the CHSH angles and notice that the sum of all function pairs may now violate the CHSH inequalities, because the cyclicity has vanished.

It is important to realize that the wing with variable polarizer setting may also be subjected to rapid switching in this particular experiment. Rapid switching in both wings from positive to negative polarizer direction may be performed in addition, all without changing any expectation values (the correlations P).

Rapid switching of the Kwiat and coworker experiment would be useful to test Einstein’s separation principle. It also would guarantee, now in a consistent way, the independence of the sets Λ from the polarizer-setting-pairs. Therefore, conspiracy-theory loopholes would be excluded as they have been excluded in the work that uses human and cosmic random number generators [