Counterfactual Definiteness and Bell’s Inequality

Counterfactual definiteness must be used as at least one of the postulates or axioms that are necessary to derive Bell-type inequalities. It is considered by many to be a postulate that not only is commensurate with classical physics (as for example Einstein’s special relativity), but also separates and distinguishes classical physics from quantum mechanics. It is the purpose of this paper to show that Bell’s choice of mathematical functions and independent variables implicitly includes counterfactual definiteness. However, his particular choice of variables reduces the generality of his theory, as well as the physics of all Bell-type theories, so significantly that no meaningful comparison of these theories with actual Einstein-Podolsky-Rosen experiments can be made.

1. Introduction

Bell’s theorem [1] has an unusual standing among mathematical-physical theorems. No other theorem has ever been discussed with respect to so many “loopholes”, physical situations that make it possible to escape the mathematical strictures of the theorem. It is shown that the reason for this fact is that Bell’s theorem is based on the postulate of counterfactual definiteness. The postulate of counterfactual definiteness to derive Bell-type inequalities is clearly asserted in the books of Peres [2] and Leggett [3] .

Some of Einstein’s reasoning regarding Einstein-Podolsky-Rosen (EPR) experiments also contain counterfactual realism and Einstein’s special relativity is counterfactually definite in the mathematical sense presented below. This fact may have contributed to the opinion that counterfactual realism is the major defining trait of “classical” theories. It will be shown, however, that great care must be exercised with respect to the choice of independent variables in the argument of the functions that are used to formulate a counterfactually definite physical theory. It will also be shown that the particular choice of variables, used for the derivation of Bell’s inequality and Bell’s theorem, imposes significant restrictions to the physical situations that can be described by Bell’s functions and excludes dynamic processes of classical physics, no matter whether deterministic or stochastic. To show this fact, we first repeat the main features of Bell’s functions that describe Einstein-Podolsky-Rosen-Bohm (EPRB) experiments and then connect them to a precise definition of counterfactual definiteness.

2. EPRB Experiments and Bell’s Functions Representing Them

EPRB experiments have been described extensively in the literature [4] [5] and measure the spins of entangled particle pairs at two space-like separated locations. The two particles of each pair are emanating from a source and propagate toward the space-like separated locations. The properties of these particles are measured by instruments that are described by a “setting” such as the direction of a polarizer or magnet which is characterized by a unit vector of three dimensional space denoted by j = a, b, c, ∙∙∙. Measurements of this type have been performed by a number of researchers and have had a checkered history with respect to the results. These, at first, contradicted and then confirmed quantum theory [4] . There are still significant deviations from quantum theory in current experiments, which are, however, mostly ignored [6] . We proceed here by just stipulating that indeed these experiments showed a violation of the, by now, famous Bell inequality and describe in the following only Bell’s postulates and assumptions, thereby focusing on the simplest case involving only three settings and not four, as used in actual experiments, see also [7] . Bell’s postulates and assumptions are considered by many researchers to be entirely general and valid for all EPR like experiments and Gedanken-experiments as long as they can be described by classical physics such as Einstein’s relativity.

Bell’s classical-physics model for the system of measurement equipment and entangled pairs of the EPRB experiments is constructed as follows (see page 8 of [1] ). He assumed that all experimental results, all data, can be described by using functions A that map the independent measurement results onto ±1 which symbolizes the two possible outcomes of the spin measurements. The variables in the argument of the function always include the settings j = a, b, c, ∙∙∙ and another variable, or set of variables, that Bell denoted by λ. Bell then proceeded to present a proof of his now celebrated inequality:

(1)

where indicates the average over many measurements. The left and right factor of each term correspond to the data taken at the two corresponding space like separated measurement stations. The events of measurements and corresponding data are linked to clock times of two synchronized laboratory clocks. Therefore, the functions A as well as the variables j and λ must, for each of the products, correspond to pairs of clock times where n is the measurement number. These clock times are not explicitly included as indexes or variables of Bell’s functions.

Note that Bell’s original paper (see page 7 of [1] ) assigned to λ only properties of the entangled pair. It is now generally assumed [8] that λ may stand for a set of arbitrary physical variables including space and time coordinates or even Einstein’s space-time st. Therefore, λ may also describe some properties of the measurement equipment (in addition to the magnet or polarizer orientation j), such as dynamical effects arising from many-body interactions of the entangled pair with the constituent particles and fields of the measurement equipment. Bell agreed with this assumption in his later work [1] .

It is the purpose of this paper to show that the postulate of counterfactual definiteness in conjunction with the use of a setting variable j does not permit the introduction of general space and time related variables that describe the said many body dynamics. Therefore, Bell’s assumptions are not general enough to describe classical theories of EPRB experiments that include dynamic processes involving the measurement equip- ment.

3. Counterfactual Reasoning and EPRB Experiments

Peres [2] gave the following definition of counterfactual realism, which roughly agrees with the definition of Leggett [3] . Peres claims, as does Leggett, not to use traditional concepts of mathematics and physics to start with, but only “what could have possibly been the results of unperformed experiments” and bases his definition of counterfactual realism on the following statement:

It is possible to imagine hypothetical results for any unperformed test, and to do calculations where these unknown results are treated as if they were numbers.

We agree that it is possible, as a purely intellectual activity, to imagine hypothetical results for any unperformed tests. However, without significant additional assumptions, it is not possible “to do calculations where these unknown results are treated as if they were numbers”. Here we encounter the so often unrecognized gulf between sense im- pressions, even just imagined ones, and conceptual frame-works such as the axiomatic system of numbers or the probability theory of Kolmogorov. Peres, Leggett and a majority of quantum information theorists did not and do not recognize that giant gulf, that giant separation, between events of nature, recorded as data, and the axiomatic edifices of human thought.

Take any set of data derived from measurements on spin-1/2 particles with Stern- Gerlach magnets, that lists the measured spins as “up” or “down” together with magnet settings j = a, b, c, ∙∙∙. Can we replace “up” with +1 and “down” with −1 and expect that the so obtained set follows the axioms of integers? The “trespass” to deal with tests as if they were numbers has been committed by several textbook authors, in particular by Peres [2] and Leggett [3] . This point appears in clear relief, if we write down the data according to the way in which they are imagined to be taken in testing e.g. the Bell-type inequality. The data are recorded in pairs corresponding to detector-events that are re- gistered together with equipment settings and the clock times of synchronized labora- tory clocks. Thus we obtain data lists of the kind: the representing the randomly chosen setting pair and denoting the times of measurement. Here the D’s are symbols that represent the measured up/down spin in the example above but may as well represent the red/green color of a flash of light, etc. For numerical processing of this list of symbols, it is expedient to introduce new symbols taking values +1 and −1 that are in one-to-one correspondence with the original symbols. The number of times that the setting (a, b), (a, c), and (b, c) was chosen is denoted by Na,b, Na,c, and Nb,c, respectively. The total number of pairs is then M = Na,b + Na,c + Nb,c. One cannot do justice to the number of different data-pairs by using models with three pairs of mathematical symbols such as Aa, Ab, Aa, Ac, and Ab, Ac as they are used in Bell-type proofs. One runs into problems even if one regards these mathematical symbols as “variables” (such as Boolean variables [11] ) and not just as numbers; the reason being that one cannot cover all the different possible correlations of the data by such few variables. If we admit the two values +1 and −1 for the’s at different times of the same experiment, then we obtain Na,b + 1 different values for the sum of the pair product. If we have three such sums with all independent variables, the number of possibilities is for M sufficiently large. In contrast, we have for the Bell type variables Aa, Ab, Aa, Ac, and Ab, Ac only about independent choices of all possible different correlations of possible outcomes of these variables. This fact arises from Bell’s description of 3 M different pairs of measurements (6 M measurements) by only 3 different variables and represents another typical trespass that is explicitly made in both the book of Peres [2] and Leggett [3] : they use a model with a severe restriction of choices before any physics is introduced and thus”overburden” their variables in a way which cannot do justice to the complexity of the data. In real EPRB experiments, one uses four not three different randomly chosen settings [12] [13] but the above argument equally holds for this case, with and being replaced by and for 4 M different pairs (8 M measurements), respectively.

To describe EPRB experiments in the general way that Bell intended and purported to actually have done, we need to introduce functions A with variables additional to j in their argument (or indexes, see below). We need to have variables such as tn, sn, stn, ∙∙∙ that are taken out of the realm of Einsteinian physics and do indeed guarantee the one to one correspondence to the data. For example, we may need to include tn, the time of measurement at one location and sn representing any property of the objects emanating from the source. It may also be necessary to include a more general four dimensional space-time vector stn instead or in addition to the measurement time tn and we include it here just for completeness. This way we obtain functions.

Some may ask whether that is not precisely what Bell used by introducing his λ that, as he claimed [1] , can stand for any set of variables and, therefore, also for the set. We thus may have. Indeed it is true that this is what Bell claimed. However, as we will see below his claim is incorrect, because he and followers have postulated complete independence of λ and j and thus postulated counterfactual definiteness in conjunction with the setting variable j according to the precise definition given in the next section. Einstein locality does not require independence of λ of the local setting (see Section 5).

Note that quantum mechanics does not use any setting-type of variable as independent variable in the argument of the wave-function. There, the setting-type variables label the operators. A helpful discussion of explicit and implicit assumptions of Bell, with emphasis of the mathematical structure and consistency, was given by Khrennikov [14] .

4. Mathematical Definition of Counterfactual Definiteness and Bell’s Inequality

Counterfactual definiteness requires the following. We must be able to describe a measurement or test by using a given set of variables in the argument of the function A, and thus for example a setting j = b. Then, we must also be able to reason that we could have used instead of setting b the setting c and would have obtained the outcome corresponding to the value of A, now calculated with setting c and all other variables in its argument unchanged. Although this type of reasoning is not permitted in the courts of law, its mathematical restatement looks natural and general enough:

A counterfactually definite theory is described by a function (or functions) that map(s) tests onto numbers. The variables of the function(s) argument(s) must be chosen in a one to one correspondence to physical entities that describe the test(s) and must be independent variables in the sense that they can be arbitrarily chosen from their respective domains.

This definition means that the outcomes of measurements must be described by functions of a set of independent variables. The definition applies, of course, to the major theories of classical physics, including Einstein’s special relativity. Counterfactual definiteness appears, therefore, as a reasonable and even necessary requirement of classical theories. However, most importantly, counterfactual definiteness restricts the use of variables to those that can be independently picked from their respective domains. However, a magnet- or polarizer-orientation, mathematically represented by the variable j, cannot be picked independently of the measurement times, which are mathematically represented by tn and registered by the clocks of the measurement stations. Once a setting is picked at a certain space-time coordinate, no other setting can be linked to that coordinate, because of the relativistic limitations for the movement of massive bodies and the fact that Bell’s theory is confined to the realm of Einsteinian physics and, therefore, excludes quantum superpositions. Thus any measurement is related to spatio-temporal equipment changes and the mathematical variables that describe the measurement need to represent the possible physical situations.

Enter probability theory and we certainly cannot use the setting j as a random variable and the measurement time t as another independent random variable on the same probability space. The reason for this fact is rooted in the above explanation and can be further crystallized as follows. It is possible to define the setting j as a random variable on one probability space meaning that we may regard j as a function which assigns to each elementary event ω of a sample space Ω a so called realization of j e.g.. It is also possible, at least under very general circumstances, to formulate the measurement times as another random variable, where is an elementary event of a second sample space Ω'. Again, given some specific we obtain a realization e.g..

However, the formation of a product probability space on which both random variables j and t are defined presents now a problem. That space would necessarily contain impossible events (such as different settings for the same measurement times) with a non-zero product probability measure assigned to them. These facts can actually be formulated as a theorem stating that setting and time variables of EPRB experiments cannot be defined on one probability space [15] .

Thus, the postulate of counterfactual definiteness in conjunction with the use of a setting variable restricts the independent variables additional to j in the argument of Bell’s functions A to a, physically speaking, narrow subset of variables that we denote by NB. This subset permits the physical description of static properties but cannot handle dynamic properties expressed by space-time dependencies.

As a consequence, the choices that can be made for variables in addition to the setting variable j in Bell’s theory are extremely limited, particularly if these variables are related to space-time (or space and time). This limitation is so severe that it is impossible to describe general dynamic processes of classical physics with Bell’s independent variables. The way to describe general dynamic processes in Kolmogorov’s framework is by using stochastic processes.

To describe a dynamics of EPRB experiments one needs to use two dimensional vector stochastic processes, which involves several subtleties that, if neglected, lead to incorrect conclusions. A general vector stochastic process is in essence a vector of random variables, such a (A1(tn), A2(tn), A3(tn), ∙∙∙), whose statistical properties change in time (we use here discrete time only). A precise mathematical definition can be found in Ref. [16] , pp. 11-15. In relation to EPRB experiments we thus consider vectors such as (A1(tn), A2(tn)).

A first difficulty that is usually encountered is related to the physics of spin mea- surements. According to Bohr, the outcomes of measurements on each separate side of the EPRB experiment are spin-up or spin down with equal likelihood, which appears to suggest stationarity or time-independence of the random variables A1(tn) and A2(tn). Bohr’s postulate, however, does not necessitate a time-independence of the statistical correlations between the random variables. This fact has been explained on the basis of a mathematical model involving time in Ref. [5] (pp. 55-60) and demonstrated by actual EPRB related computer experiments [7] .

A second difficulty arises from the fact, explained in detail above, that the time and setting related variables of EPRB experiments cannot be treated as independent. This difficulty can be resolved by use of the following two-dimensional system of functions (vector stochastic process) on a probability space W:

(2)

Settings and times are now included as indexes that are not independent. jn = a, b represents the randomly chosen settings at one measurement place and at the second. tn as well as are the respective measurement times. n = 1, 2, 3, ∙∙∙ indicates just the number of the experiment. Only one setting can occur at one given time in order to avoid physical contradictions and incorrect assignments of probability measures. (Note that a generalization of the time-indexes to space-time stn is straight- forward.)

Bell’s inequality then transforms to:

(3)

where the labels n, k, m are the appropriate, all different, experiment numbers for which the particular settings have been chosen. Equation (3) puts no restrictions on the correlations of EPRB experiments, because the actual experiments may now be represented by a countable infinite number of different functions instead of the three or four functions used by Bell.

There do exist theorems that appear to prove the validity of Bell’s inequality for stochastic processes (the Martingales discussed in [17] are just special forms of stochastic processes). These theorems, however, do not use two-dimensional vector stochastic processes as used in Equation (2). They use, instead, counterfactual de- finiteness in conjunction with setting variables to arrive at three-, four- or higher dimensional stochastic processes (Martingales). Thus these theorems cannot encom- pass dynamic measurement processes [18] and time- (space-time-) related variables, because they would then imply the existence of events with more than one setting at a given measurement time and, therefore, involve impossible events with non-zero probability measure. Such theorems apply, therefore, only to the set of variables NB as defined above and do not apply to EPRB types of experiments that may involve dynamical processes in the measurement equipment.

It is, therefore, imperative to view EPRB experiments in a different light. A violation of Bell-type inequalities need not be seen as crossing the border between the reasoning of classical Einstein type of physics and quantum mechanics, but indicating a possible dynamics in the interactions of particles and measurement equipment. This possible dynamics is what needs to be investigated, particularly as contrasted to the charac- terization of the measurement equipment by a completely static symbol [19] .

5. Einstein Locality and Bell’s Reasoning Revisited

Up to now, experimentalists have not used Bell’s theorem and its implications to search for a many body dynamics of local equipment. Instead, they have attempted to “uncover” the instantaneous dynamic influences of remote measurements, the so called quantum non-localities. Some consider these non-localities to be the most profound development of modern physics [5] . They maintain that the measurement of the entangled partner causes instantaneous influences over arbitrary distances.

This search for influences due to distant events is based on the conviction, dating back to Bell’s original paper, that Einstein locality is necessary to derive Bell’s inequality. However, this is not the case. Bell’s assumption that λ is independent of the setting variable j is already contained in the postulate of counterfactual definiteness. The postulate of Einstein locality is not only redundant because of this fact, but does not require at all that λ be independent of all settings. Variables dependent on the local setting and describing local many body interactions with the incoming particles are entirely permitted and necessary. It is counterfactual definiteness that requires that all additional variables represented by λ be independent of the setting variable. But why does our classical theory need to involve the setting variable in the way Bell has included it? One can use the setting variable as an index together with another index related to or representing space-time. These indexes are, of course not independent as was pointed out above for stochastic processes.

From these facts, we can deduce that Einstein locality is not a necessary condition for Bell’s derivation, rather the opposite. Its correct implementation prevents the deriva- tion of Bell to go forward, as shown in Equation (3).

6. Conclusion

The major premise for the derivation of Bell’s inequality is counterfactual definiteness, which in connection with Bell’s use of setting variables restricts the domain of the variables in the argument of Bell’s functions A to a subset NB of general physical independent variables. NB does not encompass the variables that are necessary to describe a general dynamics of many body interactions with the measurement equip- ment. Using only the independent variables defined by NB, it is impossible to find a violation of Bell’s inequality, which therefore represents a demarcation between possible and impossible experience [9] , not between classical and quantum physics. For a wider parameter space that permits the description of dynamic processes and includes space-time coordinates, the validity of Bell-type inequalities cannot be and has not been derived. This situation is reminiscent of that with the last theorem of Fermat before 1984. There existed only rather trivial proofs of Fermat’s theorem for subsets of conditions, while a general proof was not known until Andrew Wiles supplied it in 1984. Such more complicated and general proofs of Bell’s theorem have not been presented and, in the authors opinion, are not likely to be presented in the future, because they would need to remove the use of the setting variable j.

Conflicts of Interest

The authors declare no conflicts of interest.

Cite this paper

Hess, K. , Raedt, H. and Michielsen, K. (2016) Counterfactual Definiteness and Bell’s Inequality. Journal of Modern Physics, 7, 1651-1660. doi: 10.4236/jmp.2016.713150.

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