Part of a series of articles about 
"Quantum mechanics 

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Historically, in "physics, hidden variable theories were espoused by some "physicists who argued that the "state of a physical system, as formulated by "quantum mechanics, does not give a complete description for the system; i.e., that quantum mechanics is ultimately incomplete, and that a "complete theory would provide descriptive categories to account for "all observable behavior and thus avoid any "indeterminism. The existence of indeterminacy for some measurements is a characteristic of prevalent interpretations of quantum mechanics; moreover, bounds for indeterminacy can be expressed in a quantitative form by the "Heisenberg uncertainty principle.
"Albert Einstein, the most famous proponent of hidden variables, objected to the fundamentally probabilistic nature of quantum mechanics,^{[1]} and famously declared "I am convinced God does not play dice".^{[2]} Einstein, "Podolsky, and "Rosen argued that "elements of reality" (hidden variables) must be added to quantum mechanics to explain "entanglement without "action at a distance.^{[3]}^{[4]} Later, "Bell's theorem suggested that "local hidden variables of certain types are impossible, or that they evolve nonlocally. A famous nonlocal theory is "De Broglie–Bohm theory.
Under the "Copenhagen interpretation, quantum mechanics is nondeterministic, meaning that it generally does not predict the outcome of any measurement with certainty. Instead, it indicates what the probabilities of the outcomes are, with the indeterminism of observable quantities constrained by the "uncertainty principle. The question arises whether there might be some deeper reality hidden beneath quantum mechanics, to be described by a more fundamental theory that can always predict the outcome of each measurement with certainty: if the exact properties of every subatomic particle were known the entire system could be modeled exactly using deterministic physics similar to classical physics.
In other words, it is conceivable that the standard interpretation of quantum mechanics is an incomplete description of nature. The designation of variables as underlying "hidden" variables depends on the level of physical description (so, for example, "if a gas is described in terms of temperature, pressure, and volume, then the velocities of the individual atoms in the gas would be hidden variables"^{[5]}). Physicists supporting De Broglie–Bohm theory maintain that underlying the observed probabilistic nature of the universe is a deterministic objective foundation/property—the hidden variable. Others, however, believe that there is no deeper deterministic reality in quantum mechanics.^{["citation needed]}
A lack of a kind of "realism (understood here as asserting independent existence and evolution of physical quantities, such as position or momentum, without the process of measurement) is crucial in the Copenhagen interpretation. Realistic interpretations (which were already incorporated, to an extent, into the physics of Feynman^{[6]}), on the other hand, assume that particles have certain trajectories. Under such view, these trajectories will "almost always be continuous, which follows both from the finitude of the perceived speed of light ("leaps" should rather be precluded) and, more importantly, from the principle of least action, as "deduced in quantum physics by Dirac. But continuous movement, in accordance with the "mathematical definition, implies deterministic movement for a range of time arguments;^{[7]} and thus realism is, under modern physics, one more reason for seeking (at least certain limited) determinism and thus a hidden variable theory (especially that such theory exists: see "De Broglie–Bohm interpretation).
Although determinism was initially a major motivation for physicists looking for hidden variable theories, nondeterministic theories trying to explain what the supposed reality underlying the quantum mechanics formalism looks like are also considered hidden variable theories; for example "Edward Nelson's "stochastic mechanics.
In June 1926, "Max Born published a paper, "Zur Quantenmechanik der Stoßvorgänge" ("Quantum Mechanics of Collision Phenomena") in the scientific journal "Zeitschrift für Physik, in which he was the first to clearly enunciate the probabilistic interpretation of the quantum "wavefunction, which had been introduced by "Erwin Schrödinger earlier in the year. Born concluded the paper as follows:
Here the whole problem of determinism comes up. From the standpoint of our quantum mechanics there is no quantity which in any individual case causally fixes the consequence of the collision; but also experimentally we have so far no reason to believe that there are some inner properties of the atom which conditions a definite outcome for the collision. Ought we to hope later to discover such properties ... and determine them in individual cases? Or ought we to believe that the agreement of theory and experiment—as to the impossibility of prescribing conditions for a causal evolution—is a preestablished harmony founded on the nonexistence of such conditions? I myself am inclined to give up determinism in the world of atoms. But that is a philosophical question for which physical arguments alone are not decisive.
Born's interpretation of the wavefunction was criticized by Schrödinger, who had previously attempted to interpret it in real physical terms, but "Albert Einstein's response became one of the earliest and most famous assertions that quantum mechanics is incomplete:
Quantum mechanics is very worthy of regard. But an inner voice tells me that this is not yet the right track. The theory yields much, but it hardly brings us closer to the Old One's secrets. I, in any case, am convinced that He does not play dice.^{[8]}^{[9]}
"Niels Bohr reportedly replied to Einstein's later expression of this sentiment by advising him to "stop telling God what to do."^{[10]}
Shortly after making his famous "God does not play dice" comment, Einstein attempted to formulate a deterministic counterproposal to quantum mechanics, presenting a paper at a meeting of the "Academy of Sciences in Berlin, on 5 May 1927, titled "Bestimmt Schrödinger's Wellenmechanik die Bewegung eines Systems vollständig oder nur im Sinne der Statistik?" ("Does Schrödinger's wave mechanics determine the motion of a system completely or only in the statistical sense?").^{[11]} However, as the paper was being prepared for publication in the academy's journal, Einstein decided to withdraw it, possibly because he discovered that, contrary to his intention, it implied "nonseparability of "entangled systems, which he regarded as absurd.^{[12]}
At the "Fifth Solvay Congress, held in Belgium in October 1927 and attended by all the major theoretical physicists of the era, "Louis de Broglie presented "his own version of a deterministic hiddenvariable theory, apparently unaware of Einstein's aborted attempt earlier in the year. In his theory, every particle had an associated, hidden "pilot wave" which served to guide its trajectory through space. The theory was subject to criticism at the Congress, particularly by "Wolfgang Pauli, which de Broglie did not adequately answer. De Broglie abandoned the theory shortly thereafter.
Also at the Fifth Solvay Congress, Max Born and "Werner Heisenberg made a presentation summarizing the recent tremendous theoretical development of quantum mechanics. At the conclusion of the presentation, they declared:
[W]hile we consider ... a quantum mechanical treatment of the electromagnetic field ... as not yet finished, we consider quantum mechanics to be a closed theory, whose fundamental physical and mathematical assumptions are no longer susceptible of any modification.... On the question of the 'validity of the law of causality' we have this opinion: as long as one takes into account only experiments that lie in the domain of our currently acquired physical and quantum mechanical experience, the assumption of indeterminism in principle, here taken as fundamental, agrees with experience.^{[13]}
Although there is no record of Einstein responding to Born and Heisenberg during the technical sessions of the Fifth Solvay Congress, he did challenge the completeness of quantum mechanics during informal discussions over meals, presenting a "thought experiment intended to demonstrate that quantum mechanics could not be entirely correct. He did likewise during the Sixth Solvay Congress held in 1930. Both times, "Niels Bohr is generally considered to have successfully defended quantum mechanics by discovering errors in Einstein's arguments.
The debates between Bohr and Einstein essentially concluded in 1935, when Einstein finally expressed what is widely considered his best argument against the completeness of quantum mechanics. "Einstein, Podolsky, and Rosen had proposed their definition of a "complete" description as one that uniquely determines the values of all its measurable properties. Einstein later summarized their argument as follows:
Consider a mechanical system consisting of two partial systems A and B which interact with each other only during a limited time. Let the ψ function [i.e., "wavefunction ] before their interaction be given. Then the Schrödinger equation will furnish the ψ function after the interaction has taken place. Let us now determine the physical state of the partial system A as completely as possible by measurements. Then quantum mechanics allows us to determine the ψ function of the partial system B from the measurements made, and from the ψ function of the total system. This determination, however, gives a result which depends upon which of the physical quantities (observables) of A have been measured (for instance, coordinates or momenta). Since there can be only one physical state of B after the interaction which cannot reasonably be considered to depend on the particular measurement we perform on the system A separated from B it may be concluded that the ψ function is not unambiguously coordinated to the physical state. This coordination of several ψ functions to the same physical state of system B shows again that the ψ function cannot be interpreted as a (complete) description of a physical state of a single system.^{[14]}
Bohr answered Einstein's challenge as follows:
[The argument of] Einstein, Podolsky and Rosen contains an ambiguity as regards the meaning of the expression "without in any way disturbing a system." ... [E]ven at this stage [i.e., the measurement of, for example, a particle that is part of an "entangled pair], there is essentially the question of an influence on the very conditions which define the possible types of predictions regarding the future behavior of the system. Since these conditions constitute an inherent element of the description of any phenomenon to which the term "physical reality" can be properly attached, we see that the argumentation of the mentioned authors does not justify their conclusion that quantummechanical description is essentially incomplete."^{[15]}
Bohr is here choosing to define a "physical reality" as limited to a phenomenon that is immediately observable by an arbitrarily chosen and explicitly specified technique, using his own special definition of the term 'phenomenon'. He wrote in 1948:
As a more appropriate way of expression, one may strongly advocate limitation of the use of the word phenomenon to refer exclusively to observations obtained under specified circumstances, including an account of the whole experiment."^{[16]}^{[17]}
This was, of course, in conflict with the definition used by the EPR paper, as follows:
If, without in any way disturbing a system, we can predict with certainty (i.e., with probability equal to unity) the value of a physical quantity, then there exists an element of physical reality corresponding to this physical quantity. [Italics in original]^{[3]}
In 1964, "John Bell showed through "his famous theorem that if local hidden variables exist, certain experiments could be performed involving "quantum entanglement where the result would satisfy a "Bell inequality. If, on the other hand, statistical correlations resulting from "quantum entanglement could not be explained by local hidden variables, the Bell inequality would be violated. Another "nogo theorem concerning hidden variable theories is the "Kochen–Specker theorem.
Physicists such as "Alain Aspect and Paul Kwiat have performed "experiments that have found violations of these inequalities up to 242 standard deviations^{[18]} (excellent scientific certainty). This rules out local hidden variable theories, but does not rule out nonlocal ones. Theoretically, there could be "experimental problems that affect the validity of the experimental findings.
"Gerard 't Hooft has disputed the validity of Bell's theorem on the basis of the "superdeterminism loophole and proposed some ideas to construct local deterministic models.^{[19]}
Assuming the validity of Bell's theorem, any deterministic hiddenvariable theory that is "consistent with "quantum mechanics would have to be "nonlocal, maintaining the existence of instantaneous or fasterthanlight relations (correlations) between physically separated entities. The currently bestknown hiddenvariable theory, the "causal" interpretation of the physicist and philosopher "David Bohm, originally published in 1952, is a nonlocal hidden variable theory. Bohm unknowingly rediscovered (and extended) the idea that Louis de Broglie had proposed in 1927 (and abandoned) – hence this theory is commonly called "de BroglieBohm theory". Bohm posited both the quantum particle, e.g. an electron, and a hidden 'guiding wave' that governs its motion. Thus, in this theory electrons are quite clearly particles—when a "doubleslit experiment is performed, its trajectory goes through one slit rather than the other. Also, the slit passed through is not random but is governed by the (hidden) guiding wave, resulting in the wave pattern that is observed.
Such a view does not contradict the idea of local events that is used in both classical atomism and "relativity theory as Bohm's theory (and quantum mechanics) are still locally causal (that is, information travel is still restricted to the speed of light) but allow nonlocal correlations. It points to a view of a more "holistic, mutually interpenetrating and interacting world. Indeed, Bohm himself stressed the holistic aspect of quantum theory in his later years, when he became interested in the ideas of "Jiddu Krishnamurti.
In Bohm's interpretation, the (nonlocal) "quantum potential constitutes an implicate (hidden) order which organizes a particle, and which may itself be the result of yet a further implicate order: a superimplicate order which organizes a field.^{[20]} Nowadays Bohm's theory is considered to be one of many "interpretations of quantum mechanics which give a "realist interpretation, and not merely a "positivistic one, to quantummechanical calculations. Some consider it the "simplest theory to explain quantum phenomena.^{[21]} Nevertheless, it is a hidden variable theory, and necessarily so.^{[22]} The major reference for Bohm's theory today is his book with "Basil Hiley, published posthumously.^{[23]}
A possible weakness of Bohm's theory is that some (including Einstein, Pauli, and Heisenberg) feel that it looks contrived.^{[24]} (Indeed, Bohm thought this of his original formulation of the theory.^{[25]}) It was deliberately designed to give predictions that are in all details identical to conventional quantum mechanics.^{[25]} Bohm's original aim was not to make a serious counterproposal but simply to demonstrate that hiddenvariable theories are indeed possible.^{[25]} (It thus provided a supposed counterexample to the famous proof by "John von Neumann that was generally believed to demonstrate that no deterministic theory reproducing the statistical predictions of quantum mechanics is possible.) Bohm said he considered his theory to be unacceptable as a physical theory due to the guiding wave's existence in an abstract multidimensional configuration space, rather than threedimensional space.^{[25]} His hope was that the theory would lead to new insights and experiments that would lead ultimately to an acceptable one;^{[25]} his aim was not to set out a deterministic, mechanical viewpoint, but rather to show that it was possible to attribute properties to an underlying reality, in contrast to the conventional approach to quantum mechanics.^{[26]}
In August 2011, Roger Colbeck and Renato Renner published a proof that any extension of quantum mechanical theory, whether using hidden variables or otherwise, cannot provide a more accurate prediction of outcomes, assuming that observers can freely choose the measurement settings.^{[27]} Colbeck and Renner write: "In the present work, we have ... excluded the possibility that any extension of quantum theory (not necessarily in the form of local hidden variables) can help predict the outcomes of any measurement on any quantum state. In this sense, we show the following: under the assumption that measurement settings can be chosen freely, quantum theory really is complete".
In January 2013, "GianCarlo Ghirardi and Raffaele Romano described a model which, "under a different free choice assumption [...] violates [the statement by Colbeck and Renner] for almost all states of a bipartite twolevel system, in a possibly experimentally testable way".^{[28]}
The general class, Λ, of hidden variables is composed of two subclasses Λ_{R} (Recurrent) and Λ_{N} (Nonrecurrent) such that Λ_{R}∪Λ_{N}=Λ and Λ_{R}∩Λ_{N}={}. The class Λ_{N} is very large and contains random variables whose domain is the continuum, the reals ^{[29]}. There are an uncountable infinite number of reals. Every instance of a real random variable is unique. The probability two instances are equal is zero, exactly zero^{[30]}. Λ_{N} induces sample independence. All correlations are context dependent but not in the usual sense. There is no "spooky action at a distance". That fact can be captured by using random variables which, for Λ_{N} , are independent from one experiment to the next. The existence of the class Λ_{N} makes it impossible to derive any of the standard inequalities used to define quantum entanglement. Attempting to derive Bell's inequality when the hidden variables belong to Λ_{N} blocks the step assuming A of AB and A of AC are equal. Those experiments occur at different times and hence share no continuous hidden variable instances. AB and AC are independent, the expected value of their product is the product of their expected values: <(AB)(AC)>=<AB><AC>. That leads to a different inequality from Bell's. The nonrecurrent inequality places no constraints on the correlations. Those correlations can violate Bell's inequality even though they arise from a local model.
Examples of Λ_{N} distributions are:
Uniform
Normal (Gaussian)
Exponential
...
any piecewise continuous density