Abstract
The ontological models framework distinguishes ψontic from ψepistemic wavefunctions. It is, in general, quite straightforward to categorize the wavefunction of a certain quantum theory. Nevertheless, there has been a debate about the ontological status of the wavefunction in the statistical interpretation of quantum mechanics: is it ψepistemic and incomplete or ψontic and complete? I will argue that the wavefunction in this interpretation is best regarded as ψontic and incomplete.
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1 Introduction
In their recent article, Oldofredi and López [50] claim that Harrigan and Spekkens [33] define the ontic state \(\lambda\) in too restrictive a way so that it does not properly capture the statistical interpretation of quantum mechanics. Furthermore, they argue that Harrigan and Spekkens [33] put the wavefunction in the statistical interpretation in the wrong category: instead of being ψepistemic (and incomplete) the wavefunction is ψontic (and complete). They support their argument by historic evidence from Albert Einstein and Leslie Ballentine, who are the most prominent proponents of the statistical interpretation. I want to challenge all three claims and argue for the following: (i) the ontic state in the sense of Harrigan and Spekkens [33] is general enough to capture a statistical interpretation of the wavefunction, (ii) the wavefunction can be interpreted as ψepistemic as perceived by Einstein and Ballentine (although it does not merely represent an observer’s knowledge), and (iii) the statistical interpretation is more compatible with an ontic state as described by Harrigan and Spekkens [33] than as redefined by Oldofredi and López [50].
I will argue that both interpretations face different kinds of problems: the interpretation of Harrigan and Spekkens [33] runs into the PBRtheorem, and the interpretation of Oldofredi and López [50] is in fact incomplete itself and conceptually unclear. Ultimately, the status of the wavefunction in the statistical interpretation depends on the particular completion of this theory. Yet, I will argue that the wavefunction in the statistical interpretation is most plausibly ψontic and incomplete.
2 The Ontological Models Framework
Let me first explain where the notion of ψepistemic comes from and what it means. Harrigan and Spekkens [33] introduce it within a certain formal framework for quantum mechanics, which they call the ontological models framework. The main question they ask is, “Does the quantum state represent reality or only our knowledge of reality?” One option is to sidestep this question and take an operational approach to quantum mechanics: all one is interested in is predicting the behavior of quantum systems without recourse to unobservable objects and processes. The ideal case would be an operational quantum theory that describes all predictions of the theory in terms of preparation and measurement procedures. In doing so, it needs to say what kinds of measurements M and preparation procedures P yield an outcome k. An operational quantum theory specifies a probability \(\mathbb{P}\) for k, given M and P, that is, \(\mathbb{P}(k\vert M,P)\).
Often a physical theory tells us more about the world than how certain manipulations on a physical system lead to certain empirical results: it may tell us what the measured system is made of, what a measurement device is made of, and how measurement and preparation devices interact with the constituents of the measured system [37]. In particular, the physical theory should (ideally) specify a complete description of the system’s properties. This complete description is often denoted \(\lambda\). A theory that gives such an ontological story to operational quantum theory is an ontological model of operational quantum theory.
Again, an ontological model of an operational theory of quantum mechanics provides more information about the physical system beyond an operational level; it describes the complete physical state \(\lambda\) of the system. Although measurement and preparation devices can be described with their own ontic state \(\lambda\) in an ontological theory, they are not reduced to these \(\lambda\)’s in the ontological models framework. The main problem that the ontological models framework aims to tackle is how much an observer can know about the ontic state of the physical system if she prepares and measures the system in a certain way. For example, a preparation procedure may not uniquely fix the ontic state but rather a probability distribution \({\mathbb{P}}(\lambda \vert P)\) for ontic states given a preparation procedure. If the observer prepares the system in a state \(\lambda\), this ontic state determines the result k once measured, that is, the ontological models framework provides this probability distribution \({\mathbb{P}}(k \vert \lambda , M)\). We can now explain the predictions of the operational theory \({\mathbb{P}}(k\vert M,P)\) with the machinery of the ontological theory:
We integrate over all the possible ontic states, where \({\mathbb{P}}(\lambda \vert P)\ne 0\) singles out the ontic states that are compatible with the state procedure P.
It is often implied that the ontological model framework is a strong constraint on a physical theory (for instance [31]). In my opinion, it is rather a formalization of how physics has been ever done until recently with the development of quantum physics by identifying the complete physical state of a system and investigating the time evolution of this state. One may still agree with me here and still claim that the ontological models framework is too restrictive for quantum physics (I thank an anonymous reviewer for this remark). Nevertheless, the ontological models framework reaches a large set of quantum theories that does not face the physical, conceptual, and ontological problems as theories that do not fit into this model (see, for instance [18, 48]).
Oldofredi and López [50] seem to mischaracterize the relation between an operational theory and its corresponding ontological model:
It is worth noting that the authors define ontological models employing an operational setting, i.e. the primitive notions of such models consist exclusively in preparations procedures of physical systems in certain states and measurements performed on them. A complete specification of the properties of a given physical system is provided by \(\lambda\), the ontic state of the system under scrutiny. [50, pp. 1318–1319]
As we have seen, ontological models consider operational procedures to prepare the state of a quantum system in a certain manner as primitive notions. Such procedures are associated with some observable properties, whose values will be then revealed by the performance of a set of measurements on the physical system under scrutiny. [50, pp. 1321]
It is not the ontological model that treats the operational procedures as primitive notions. Rather, the ontological model provides the tools for explaining these procedures and reduce them to the behavior of the ontic state \(\lambda\). More precisely, ”In an ontological model of an operational theory, the primitives of description are the properties of microscopic systems,” [33, p. 128] and these properties encoded in \(\lambda\) determine the probabilities and outcomes in preparation and measurement procedures. Of course, the ontological model itself does not tell us exactly how the operational procedures look like, but it demands, in contrast to an operational theory, that the probabilities derive from the interaction with the ontic state of the system. It is only on the level of the operational quantum theory, where the operational procedures are taken as primitive. Therefore, the relation between the operational theory and the corresponding ontological model is indeed similar to the relation between thermodynamics and statistical mechanics.
In quantum mechanics, the wavefunction has a double role: it determines the probabilities of measurement outcomes via the Born rule, and it also (at least partially) describes the ontic state of the physical system. This is also reflected in the ontological models framework. The probabilities of the operational theory are determined by the wavefunction \({\mathbb{P}}(k\vert M,P)={\mathbb{P}}_{\psi }(k\vert M,P)\). The ontological models framework zooms in on the relation between the ontic state \(\lambda\) and the corresponding wavefunction describing this state. If the system is prepared to have a certain wavefunction ψ, the system may be in one of many possible ontic states compatible with this ψ. The corresponding probability distribution would be \({\mathbb{P}}(\lambda \vert P=\psi )\).
Having introduced the ontic state \(\lambda\), one can try to answer the original question “Does the quantum state represent reality or our knowledge of reality?”. In other words, does the wavefunction represent objective properties of the ontic state (the complete physical description of the system), or does it rather represent an agent’s knowledge about properties of this state?
Harrigan and Spekkens [33] introduce an ingenious and rather general formal distinction to make this question more precise. If we prepare two systems with different wavefunctions, a natural question arises of how the ontic states corresponding to these wavefunctions are related. The ontological models framework distinguishes between two cases:

(i)
If the probability distributions \({\mathbb{P}}(\lambda \vert P=\psi_A)\) and \({\mathbb{P}}(\lambda \vert P=\psi_B)\) of two different wavefunctions \(\psi_A\) and \(\psi_B\) do not overlap, as depicted in Fig. 1a), the wavefunction is called ψontic.

(ii)
If the probability distributions \({\mathbb{P}}(\lambda \vert P=\psi_A)\) and \({\mathbb{P}}(\lambda \vert P=\psi_B)\) of two different wavefunctions \(\psi_A\) and \(\psi_B\) do overlap, as depicted in Fig. 1b), the wavefunction is called \(\psi\)epistemic.
For every wavefunction, there is a set of ontic states \(\lambda\) compatible with this wavefunction, that is, there is a onetomany relation from the wavefunction to the underlying ontic states. If we pick an ontic state, then it depends on the wavefunction whether the relation from the ontic state to the wavefunction is onetoone or onetomany. More precisely, if the wavefunction is \(\psi\)ontic, fixing an ontic state \(\lambda\), there is only one wavefunction associated with it. If the wavefunction is \(\psi\)epistemic, there are ontic states which are associated with at least two wavefunctions—namely, the ones in the overlap region.
The definition of \(\psi\)ontic and \(\psi\)epistemic was up to now only about whether or not a wavefunction can be uniquely associated with an ontic state. On this level, \(\psi\)ontic and \(\psi\)epistemic are merely formal notions. Nevertheless, these definitions have been introduced to clarify and make more precise in what way the wavefunction is ontic or epistemic; that is, in what way the wavefunction represents objective features or knowledge about the world. But we will shortly encounter certain caveats regarding the ontological and epistemic status of \(\psi\)ontic and \(\psi\)epistemic wavefunctions. \(\psi\)ontic and \(\psi\)epistemic carve up the ontic and epistemic landscape of the wavefunction a bit differently than the notions themselves may suggest.
2.1 How Ontological are \(\psi\)Ontic WaveFunctions?
Let us first discuss in which way a \(\psi\)ontic wavefunction is ontological. If an ontic state is uniquely associated with a wavefunction, then and only then can we interpret the wavefunction as representing certain objective properties of \(\lambda\) (what these properties exactly are is left open).
We can introduce further definitions that show how a \(\psi\)ontic wavefunction can objectively represent these properties (see Fig. 2a). First, the wavefunction alone can completely describe the state of the system. In this case, we call the wavefunction \(\psi\)complete. The probability distributions of \(\psi\)complete wavefunctions are sharply peaked around \(\lambda\), as shown in Fig. 3.
If the wavefunction does not completely describe \(\lambda\), then it is called \(\psi\)supplemented. A \(\psi\)supplemented wavefunction would need additional variables to provide such a complete description (what these variables are is left open in the ontological models framework).
We can also describe \(\psi\)ontic wavefunctions in a different way, as done in Fig. 2b). If the wavefunction represents properties of \(\lambda\) because it is itself a physical object (or rather the object it represents is a physical object), then we call it \(\psi\)physical. If the wavefunction represents an abstract entity that still determines the behavior of \(\lambda\), we call it \(\psi\)nomological.^{Footnote 1}
We can now build a matrix for the different combinations of \(\psi\)ontic wavefunctions (see Fig. 4), as the ontological models framework merely provides a general categorization of the wavefunction that needs to be filled in by specific interpretations of quantum mechanics. Example of theories or interpretations that construe the wavefunction as \(\psi\)complete and \(\psi\)physical are wavefunction realism [47], probably the Copenhagen interpretation, and different versions of the manyworlds interpretation [16]. Examples of \(\psi\)supplemented and \(\psi\)physical are the multifield interpretation within the de Broglie–Bohm theory [38, 52], spacetime state realism in the manyworlds theory [58], the manyworlds theory with matter density [3], and the original version of Albert’s marvelous point interpretation [1]. Examples of theories or interpretations with a \(\psi\)supplemented and \(\psi\)nomological wavefunction would be Humean interpretations of the de Broglie–Bohm theory (also called Bohumianism, [12, 14, 20, 25, 26, 46]), the dispositional interpretation of the wavefunction in the de Broglie–Bohm theory [25, 26, 56], the wavefunction as a nomological entity in the de Broglie–Bohm theory [32], wavefunctionalism [2], a Humean version of Albert’s marvelous point interpretation [42], and the GRW theory with a flash or matter ontology [22, 23, 43].^{Footnote 2} A \(\psi\)nomological interpretation with a \(\psi\)complete wavefunction has not been proposed, since it is hard to grasp how the wavefunction can completely represent the ontic state with it being a mere nomological entity.
2.2 How Epistemic Are \(\psi\)Epistemic WaveFunctions?
Now let us turn to \(\psi\)epistemic wavefunctions. These are the ones where some ontic states \(\lambda\) are associated with more than one wavefunction. How can that happen? One obvious way is when two agents have different knowledge about the same system and disagree on the the wavefunction, as in Fig. 5. It would be a mistake to say that the wavefunction in this case is purely epistemic; rather, agents would learn something about the system if they assign to the system one of the (correct) wavefunctions that are associated with the ontic state.^{Footnote 3} This kind of \(\psi\)epistemic wavefunction emphasizes the relational character between the objective properties of \(\lambda\) and the agents’ knowledge about \(\lambda\) represented in the wavefunction. We could call such a wavefunction \(\psi\)credal, as there is another way to interpret \(\psi\)epistemic wavefunctions (see [44, Ch. 3]).
Oldofredi and López [50] assume that all \(\psi\)epistemic wavefunctions are \(\psi\)credal:
If a model is \(\psi\)epistemic, then it cannot in any case be \(\psi\)ontic, since it does not describe any underlying physical reality, but only the agents’ knowledge of it. [50, pp. 1320]^{Footnote 4}
Even if a \(\psi\)epistemic wavefunction were to represent an agent’s knowledge, the wavefunction would be referring to the ontic state. So if I assign a correct \(\psi\)epistemic wavefunction to a quantum system, I would indeed know some aspects of the underlying physical reality, even if another agent may assign a different wavefunction to the same system.
It is indeed possible to interpret a \(\psi\)epistemic wavefunction in a completely nonepistemic way.^{Footnote 5} Imagine we prepare two beams of particles, one with wavefunction \(\psi_A\) and the other with wavefunction \(\psi_B\). Let us assume that a particle have wavefunction \(\psi_A\) is primarily a matter of whether it is part of the ensemble being prepared to have \(\psi_A\) as its wavefunction. If the wavefunction is \(\psi\)epistemic there are some of the particles in the \(\psi_A\) ensemble that may be also correctly described by another wavefunction, say \(\psi_B\). This means that these particles can be correctly associated with either beam, the \(\psi_A\) beam or the \(\psi_B\) beam. In this case, the wavefunction, although \(\psi\)epistemic, does not represent an agent’s knowledge but rather whether a particle is part of a certain ensemble. Maudlin [44, Ch. 3] calls such a wavefunction \(\psi\)statistical (see Fig. 6).
This counterexample challenges two arguments by Oldofredi and López [50]: (i) that a \(\psi\)epistemic wavefunction is necessarily epistemic, and (ii) that the wavefunction in the statistical interpretation has to be \(\psi\)ontic. Having replied to (i), I will discuss (ii) in Sect. 4, but before doing so, I shall introduce the PBRtheorem, which will be important to answer more completely whether the statistical interpretation of quantum mechanics can be \(\psi\)epistemic. This will in particular affect how Harrigan and Spekkens [33] understand the statistical interpretation.
3 The PBRTheorem
The PBRtheorem starts with two crucial assumptions:

Assumption 1 (Reality Criterion): Every physical system has an underlying ontic state that completely describes its physical properties, which is objective and independent from observers.^{Footnote 6}

Assumption 2 (Preparation Independence): Two preparation devices run independently from each other.
The first assumption is essential to the ontological models framework, whereas the second is added for methodological reasons. The reality criterion basically says that we consider a theory that fits into the ontological models framework. Preparation independence adds to the ontological models framework that the statistical distributions of ontic states that are generated in one preparation device do not depend on the statistical distributions of ontic states that are generated in another preparation device.^{Footnote 7}
The general argument of the PBRtheorem is the following: if the wavefunction is \(\psi\)epistemic and the two assumptions hold, then we get a contradiction with the (wellconfirmed) predictions of quantum mechanics. Since the two assumptions are reasonable, the wavefunction cannot be \(\psi\)epistemic and must therefore be \(\psi\)ontic. It is indeed possible to question the validity of the two assumptions and explore how such a quantum theory would look like.^{Footnote 8} I just want to emphasize here that it is impossible to violate the Reality Criterion and retain a \(\psi\)epistemic wavefunction, as is often claimed. For the definition of \(\psi\)epistemic hinges on the ontological models framework and thus on the existence of \(\lambda\).
Let us now discuss the experimental setup of the PBRtheorem. Two preparation devices are used to generate particles either in a zspin up or an xspin up state (see Fig. 7). Alice and Bob can choose in which state the system should be prepared. Since it is assumed that the wavefunction is \(\psi\)epistemic, some of the wavefunctions in Alice’s ensemble can be correctly associated with another wavefunction. For simplicity, we assume that if such a system is in an zspin up state the other correct wavefunction would be xspin up and vice versa. The same is the case for Bob’s systems. To have a concrete number, we say that these ontic states with double wavefunctions appear q times in such an ensemble.
Now, Alice and Bob shoot their quantum systems into a measuring device that is set up to measure pairs of particles, where one system of the pair comes from Alice and the other from Bob. Certain pairs are of particular interest, because these are the ones that ultimately yield a contradiction with the predictions of quantum mechanics. A fraction of q systems on Alice’s and on Bob’s side are associated with two wavefunctions: \(\vert \uparrow_z \rangle\) and \(\vert \uparrow_x \rangle\). Due to preparation independence, the ontic states with such double wavefunctions on Alice’s side are independent from (or uncorrelated with) the ontic states with double wavefunctions on Bob’s side. Therefore, \(q^2\) times a pair of particles is associated with four wavefunctions (each in a product state): \(\vert \uparrow_z \rangle \vert \uparrow_z \rangle\), \(\vert \uparrow_z \rangle \vert \uparrow_x \rangle\), \(\vert \uparrow_x \rangle \vert \uparrow_z \rangle\), and \(\vert \uparrow_x \rangle \vert \uparrow_x \rangle\).
The subsequent measurement is set up in such a way to yield one of four possible measurement outcomes: A, B, C, or D. What are the probabilities for either outcome if a pair in a product state is measured? The device is prepared that a \(\vert \uparrow_z \rangle \vert \uparrow_z \rangle\) state will not get measured as A, that is, the probability for yielding A given this product state is zero: \(P_{z,z}(A)=0\). Similarly, for the other product states: \(P_{z,x}(B)=0\), \(P_{x,z}(C)=0\), \(P_{x,x}(D)=0\).^{Footnote 9} It is now easy to see why these ontic states that are associated with all these product states are problematic. If we shoot these states into the measurement device, the theory tells us that the measurement will not give us either of the four possible results. On the other hand, the measurement apparatus by construction will measure something and will yield one of the four possible outcomes.^{Footnote 10} Overall, it happens \(q^2\) times that the measurement device will show a result that is prohibited by quantum mechanics if the wavefunction is \(\psi\)epistemic.
One can now react in three different ways to the result of the PBRtheorem:

1.
Our best choice of wavefunctions is to interpret them as \(\psi\)ontic.

2.
We may deny the preparation independence assumption. These theories would fit into the ontological models framework, they would also have a \(\psi\)epistemic wavefunction, but they would not lead to the contradiction indicated in the PBRtheorem.^{Footnote 11}

3.
We may deny the reality criterion. Then the entire setup of the ontological models framework would be undermined; in particular, the PBRtheorem would say nothing about these kinds of quantum theories.
I do not want to argue for or against either of these strategies in this paper. Instead, this overview will give us a scheme for evaluating the status of the wavefunction in the statistical interpretation of quantum mechanics.
4 The Statistical Interpretation of Quantum Mechanics
For Harrigan and Spekkens [33], the wavefunction in the statistical interpretation is \(\psi\)epistemic and \(\psi\)incomplete, while Oldofredi and López [50] claim it to be \(\psi\)ontic and \(\psi\)complete. I will argue that Einstein and Ballentine regard the wavefunction in the statistical interpretation as \(\psi\)epistemic and \(\psi\)incomplete. I will also discuss whether the wavefunction in the statistical interpretation can be \(\psi\)statistical. I will conclude, however, that the wavefunction in the statistical interpretation needs to be \(\psi\)ontic and \(\psi\)incomplete.
Let us first start to introduce the statistical interpretation of quantum mechanics. One of the clearest descriptions of it can be found in Einstein’s 1949 Reply to Critics in Paul Schilpp’s volume Albert Einstein: Philosopher–Scientist:
Within the framework of statistical quantum theory there is no such thing as a complete description of the individual system. More cautiously it might be put as follows: The attempt to conceive the quantumtheoretical description as the complete description of the individual systems leads to unnatural theoretical interpretations, which become immediately unnecessary if one accepts the interpretation that the description refers to ensembles of systems and not to individual systems. In that case the whole ‘eggwalking’ performed in order to avoid the ‘physically real’ becomes superfluous. There exists, however, a simple psychological reason for the fact that this most nearly obvious interpretation is being shunned. For if the statistical quantum theory does not pretend to describe the individual system (and its development in time) completely, it appears unavoidable to look elsewhere for a complete description of the individual system; in doing so it would be clear from the very beginning that the elements of such a description are not contained within the conceptual scheme of the statistical quantum theory. With this one would admit that, in principle, this scheme could not serve as the basis of theoretical physics. Assuming the success of efforts to accomplish a complete physical description, the statistical quantum theory would, within the framework of future physics, take an approximately analogous position to the statistical mechanics within the framework of classical mechanics. I am rather firmly convinced that the development of theoretical physics will be of this type; but the path will be lengthy and difficult. [54, pp. 671–672]
I want to take home three important points from this passage:

1.
The wavefunction in the statistical interpretation describes ensembles instead of individual quantum systems.

2.
Therefore individual systems are not completely described by the wavefunction.

3.
To describe an individual system completely, one would need to go beyond the statistical interpretation to search for such a completion.
The statistical interpretation, as Einstein describes it, is a peculiar form of interpretation. Normally, one would seek an interpretation of quantum mechanics that is in some sense complete. Even if one were to support an operational or pragmatist interpretation of quantum mechanics [34], one would argue that such an interpretation does not need a completion—for example, because one is skeptical that we can discover the true nature of unobservable objects. The statistical interpretation, on the other hand, rather says that, for all practical purposes, one can think of the wavefunction describing ensembles, but this is not the complete story of reality. In his last words on the statistical interpretation, Einstein emphasized in a letter to A. Lamouche just a month before he died on March 20, 1955, that the statistical interpretation is incomplete:
The \(\psi\)function is not to be considered as a complete description of an individual state of affairs, rather only as a representation of what we can know about a particular state of affairs from an empirical point of view. Then the \(\psi\)function is a representation of an “ensemble”, not the complete characterization of individual states of affairs. One has thereby renounced the latter in principle.^{Footnote 12} (quoted in [28, p. 9])
We can find the same attitude in Ballentine [5,6,7], who is probably the most famous modern advocate of the statistical interpretation:
The Statistical Interpretation, according to which a pure state provides a description of certain statistical properties of an ensemble of similarly prepared systems, but need not provide a complete description of an individual system. [5, p. 360]
We see that a quantum state is a mathematical representation of the result of a certain state preparation procedure. Physical systems that have been subjected to the same state preparation will be similar in some of their properties, but not in all of them [...]. [5, p. 361]
The Statistical Interpretation, which regards quantum states as being descriptive of ensembles of similarly prepared systems, is completely open with respect to hidden variables. It does not demand them, but it makes the search for them entirely reasonable [(]this was the attitude of Einstein (1949)[)]. [5, p. 374]
The Statistical Interpretation does not prejudice the possibility of introducing hidden variables which would determine (in principle) the outcome of each individual measurement (Sec. 6). [5, p. 379]
For both Einstein and Ballentine, the wavefunction does indeed give an incomplete description of physical systems and would need a completion to provide such a description, as Ballentine’s statements “The Statistical Interpretation does not prejudice the possibility of introducing hidden variables” and that the statistical interpretation “is completely open with respect to hidden variables” confirm. On the one hand, it seems that Ballentine regards the statistical interpretation as a viable interpretation for all practical purposes, but, on the other hand, this interpretation is incomplete and can be completed by hidden variables. The statistical interpretation is a useful interpretation of quantum mechanics, especially for physicists, and it gives a clear statistical interpretation of the predictions of quantum mechanics. This interpretation does therefore provide a richer picture of the world than pure operationalism and a less obscure metaphysics than the Copenhagen interpretation, even if the wavefunction is \(\psi\)incomplete.
4.1 \(\psi\)Epistemic and Incomplete?
Is the wavefunction in this interpretation \(\psi\)ontic or \(\psi\)epistemic? Einstein does not explicitly answer this question in the above quotation. But since the wavefunction describes ensembles instead of individual quantum systems, it seems plausible that an individual system can be associated with two different wavefunctions. Einstein mentions such a case in his 1935 correspondence with Schrödinger (see [36] Sect. 2 and [33], Sect. 4.3):
Now what is essential is exclusively that \(\psi_{B}\) and \(\psi_{\underset{\bar{}}{B}}\) are in general different from one another. I assert that this difference is incompatible with the hypothesis that the \(\psi\) description is correlated onetoone with the physical reality (the real state). After the collision, the real state of (AB) consists precisely of the real state of A and the real state of B, which two states have nothing to do with one another. The real state of B thus cannot depend upon the kind of measurement I carry out on A [...] But then for the same state of B there are two (in general arbitrarily many) equally justified \(\psi_B\), which contradicts the hypothesis of a onetoone or complete description of the real states. (Einstein to Schrödinger in 1935, quoted in [36, p. 180])
Einstein concocted several arguments throughout his career to prove that quantum mechanics is incomplete. The only option Einstein saw in making sense of quantum mechanics was to interpret it as an incomplete statistical theory. So when Einstein concludes that quantum mechanics is incomplete, we can also understand this to say that the statistical interpretation is incomplete. His arguments also show what this incompleteness amounts to. In the above quote, Einstein talks about an entangled twoparticle system AB, presumably in this state: \(\psi =\frac{1}{\sqrt{2}}\left( \psi_A\psi_B+\psi_{\underset{\bar{}}{A}}\psi_{\underset{\bar{}}{B}}\right)\). We can think of two electrons in the singlet state, for example. Einstein presupposed that each particle is prepared in an ontic state \(\lambda_{A}\) and \(\lambda_{B}\) respectively. Whether or not we measure particle A, this measurement cannot have any physical influence on the other particle, since Einstein strongly believed in locality. Therefore, the ontic state of particle B remains the same before and after measurement, and the wavefunction representing this state cannot change either. Thus, the ontic state \(\lambda_{B}\) is correctly described by both \(\psi_{B}\) and \(\psi_{\underset{\bar{}}{B}}\). Thus quantum mechanics, as well as the statistical interpretation, is \(\psi\)epistemic and \(\psi\)incomplete.^{Footnote 13} Einstein deduces the incompleteness from the issue that several wavefunctions can be associated with the same ontic state; a complete theory, on the other hand, would uniquely associate a wavefunction to an ontic state. Harrigan and Spekkens also interpret this passage of Einstein’s as arguing for a \(\psi\)epistemic interpretation of the wavefunction. They conclude:
By characterizing his 1935 argument as one that merely established the incompleteness of quantum theory on the assumption of locality, Einstein did it a great disservice. For in isolation, a call for the completion of quantum theory would naturally have led many to pursue hidden variable theories that interpreted the fundamental mathematical object of the theory, the wave function, in the same manner in which the fundamental object of other physical theories were customarily treatedas ontic. But such a strategy was known by Einstein to be unable to preserve locality. Thus it is likely that the force of Einstein’s 1935 argument from locality to the epistemic interpretation of \(\psi\) was not felt simply because the argument was not sufficiently well articulated. [33, p. 152]
Ballentine’s answer as to whether the statistical interpretation is \(\psi\)epistemic or \(\psi\)ontic is encrypted in his second quote: “Physical systems that have been subjected to the same state preparation will be similar in some of their properties, but not in all of them.” This sounds like he regards the wavefunction as \(\psi\)statistical. An individual system has a certain wavefunction solely in virtue of being part of an ensemble that has been prepared in the same quantum state, but some of these systems within this ensemble may differ with respect to their physical properties. If these systems can be described by another wavefunction, they would have a \(\psi\)statistical wavefunction, and then the wavefunction would be \(\psi\)epistemic.
If Ballentine would advocate for such a statistical interpretation, it would not be able to make correct empirical predictions according to the PBR theorem. The only way out would be a \(\psi\)epistemic completion of the statistical interpretation that violates the assumption of preparation independence, which would lead to some form of superdeterminism (see [40, 55], for such a model).^{Footnote 14}
Let me briefly explain why one needs to violate preparation independence to rescue \(\psi\)epistemic wavefunctions.^{Footnote 15} Remember the PBR setting in Fig. 8 from Sect. 3. Two preparation devices (blue boxes) send a beam of particles to a measurement device (orange box). The particles are either prepared in a spin xup or spin zup state. Since it is assumed that the wavefunction is \(\psi\)epistemic, a fraction q of the particles in each beam are described by both the spin xup and spin zup wavefunctions (double wavefunctions). Due to preparation independence, the ontic states of the left beam are independently distributed from the ontic states in the right beam; therefore, \(q^2\) of times, a pair of particles (one from the left and one from the right beam) are associated with four wavefunctions. These simultaneous four wavefunctions lead to a contradiction with the predictions of quantum mechanics. A violation of preparation independence would not yield any twoparticle system that is correctly described by these four wavefunctions. That is, whenever a particle in the left beam has a double wavefunction the corresponding particle in the right beam will only have one correct wavefunction, and vice versa. Thus, the distribution of double wavefunctions in each beam are correlated such that a particle with a double wavefunction in one beam will not be paired with a particle in the other beam having also a double wavefunction.
There are a couple of problems with violating preparation independence. First, how could the ontic states of the two beams be correlated in the first place? This becomes particularly problematic when we isolate each preparation device from each other—for example, by spacelike separation and special isolation materials round them. There are two ways to do that, which are both implausible. Either these correlations happen by pure chance. If that were the case, there needs to be some case (even only in principle) where chance is not in our favor and would match two systems with a double wavefunction. This would, however, undermine the empirical predictions of the theory. Another way to explain these correlations would be to postulate special finetuned initial conditions in the past before the preparation (and the measurement) were conducted. These finetuned initial conditions are ultimately traced back to finetuned initial conditions of the universe...and these finetuned initial conditions demand further explanation. Especially, when experimentalists do not do anything particularly special with the preparation devices, such special initial conditions have a mysterious character.
Second, the correlation of the ontic states after preparation is sensitive to the future measurement. If we change the measurement device and conduct a different kind of measurement, this would necessitate that the particles become differently correlated if this measurement is similarly prepared as in the PBRtheorem—otherwise, we would run into another contradiction. One may explain the influence of the measurement device again by special initial conditions, but this would make the setup even more finetuned. And if the future measurement is not specially designed as in the PBRtheorem, does this mean that the particles would be still correlated, or are they uncorrelated?
Third, connected to the previous point, a violation of preparation independence depends on operational procedures, like measurement and preparation. It is unclear where to draw the line between measurement and nonmeasurement procedures and between preparation and nonpreparation procedures. It is, therefore, illdefined in which situations one has correlations and in which one does not. Following the argument by Peter Lewis [41], we can call this a measurementproblemlikeproblem.
If the statistical interpretation is \(\psi\)epistemic and incomplete as claimed by Harrigan and Spekkens [33], it has to violate preparation independence and rely on some superdeterministic mechanism, otherwise it would not be an empirically adequate theory. To avoid a violation of preparation independence, you may seek an interpretation of the wavefunction as \(\psi\)ontic. Oldofredi and López [50] go along this route but for different reasons. I present and evaluate their arguments in the next subsection.
4.2 \(\psi\)Ontic and Complete?
The biggest problem Oldofredi and López [50] identify in Harrigan and Spekkens’s classification of the statistical interpretation is that this interpretation demands a different kind of ontic state:
In the second place, another crucial point to highlight is that the ontic space of the statistical interpretation is not one of individuals, but of ensembles. This allows for an alternative reading of the ontic state: it provides a complete description of the properties of an ensemble, not of individuals. And there is nothing else to know about ensembles that is not provided by the quantum state. The upshot of the present discussion is that the sort of \(\lambda\) that the statistical interpretation poses is completely different in nature with respect to that employed by Harrigan and Spekkens. [50, p. 1330]
According to Oldofredi and López [50], the ontic state that underlies the statistical interpretation is not the one that is presupposed in the ontological models framework (which refers to individual systems), but one that only refers to an ensemble of systems. With this kind of ensemble\(\lambda\), one may interpret the wavefunction in the statistical interpretation to be \(\psi\)ontic and also \(\psi\)complete. Since, in the usual definition, a \(\psi\)ontic wavefunction requires an ontic state for individual systems, Oldofredi and López [50] would need an “ensemble ontological model”, in which the wavefunction uniquely refers to the ensemble\(\lambda\).
Oldofredi and López [50] do not argue that a \(\psi\)epistemic wavefunction is troublesome because of the PBRtheorem, that is, there are physical reasons to construe the wavefunction differently; rather, they mention historical reasons for their take on the wavefunction and the corresponding ontic state. They argue that Ballentine thought the wavefunction in the statistical interpretation to provide a complete description of physical systems. Since any \(\psi\)complete wavefunction is necessarily \(\psi\)ontic (see Lemma 6 in [33, p. 133]), the wavefunction in the statistical interpretation is \(\psi\)ontic.
Their historic argument is quite confusing. First, they present three sources in which Einstein explicitly argues that the wavefunction has to be incomplete (to not violate locality).^{Footnote 16} Then they say that “Hence, it is fair to establish a strong theoretical continuity between Ballentine’s presentation of the ensemble view and Einstein’s interpretation of quantum mechanics.” (p. 1330) That is, Ballentine agrees with Einstein on what the statistical interpretation tells us about quantum systems ([6], see also).^{Footnote 17} In particular, Ballentine is supposed to agree with Einstein that this theory is incomplete. As I discussed above, Ballentine sometimes appears to be indecisive as to whether his interpretation is complete or incomplete, but he certainly considers that his theory can be completed by another quantum theory, but whether it needs such a completion is left open. Oldofredi and López seem to suggest that Ballentine breaks with Einstein and advocates an interpretation that is complete necessitating a different ontic state \(\lambda\) that only refers to entire ensembles and not to individual systems.
In my reading of Ballentine, I rather think that he considers his theory “complete for all practical purposes” to make successful predictions and to apply quantum mechanics without dealing with a mysterious metaphysics à la Copenhagen. But to get a truly complete theory that tells us what quantum systems really are, Ballentine seems to embrace such a completion of the statistical interpretation.
Hence, it is Oldofredi and López’s proposal of an ensemble\(\lambda\), which renders the statistical interpretation a complete theory, and therefore it is them who break with both Einstein’s and Ballentine’s view of how the statistical interpretation refers to the physical world.^{Footnote 18} I see the following problems with their suggestion. First, as I said, Einstein and Ballentine explicitly mention that their interpretation is incomplete. For all practical purposes, one can use the statistical interpretation to have a sufficiently clear picture of what quantum physics tells us about the world, but for a complete picture one would need to supplement this interpretation. Second, the statistical behavior of an ensemble is generated by its individual constituents. A natural question is how these constituents do that. How is the ensemble\(\lambda\) related to the individual \(\lambda\)s? Third, and connected to the previous point, even if the wavefunction provides the complete description of an ensemble, it is unclear how the wavefunction could not be \(\psi\)statistical. Such a statistical interpretation of the wavefunction would not provide the means to exclude that some particles can be swapped between two ensembles. One may respond that it is impossible to talk about the individual ontic states since all there is in this statistical interpretation is the ensemble\(\lambda\). This response is problematic, because the individual systems do exist, and it is unclear why we are not supposed to completely describe them or why the properties of the individual systems do not contribute to the complete description of the ensemble. Fourth, ensembles are usually defined to be series or copies of infinitely many systems. In the real world, we only deal with finite series. It is not clear how an ontic state that is about the properties of infinitely many systems is related to the properties of finitely many systems.
4.3 \(\psi\)Ontic and Incomplete!
Because of the just mentioned conceptual problems with an \(\psi\)ontic and complete wavefunction for the statistical interpretation and the challenges of the PBRtheorem faced by a \(\psi\)epistemic and incomplete wavefunction, I conclude that a \(\psi\)ontic and incomplete wavefunction is the best option.
One may argue that a \(\psi\)ontic and incomplete wavefunction would restrict the relation between the ontic state \(\lambda\) and \(\psi\) more strictly than the formulation of the statistical interpretation justifies, because although the wavefunction in the statistical interpretation only describes ensembles, we would need to believe in (a not yet specified) completion that would describe individual systems. This description of individual systems would make it impossible that an electron can be swapped from an xup beam into a zup beam. Even if the statistical interpretation does not seem to a priori prohibit such a swap of particles, this constraint follows from the wavefunction being \(\psi\)ontic. That is, a particle is in a certain quantum state \(\psi\) not because it happens to be prepared to be part of an ensemble, but because properties of its ontic state \(\lambda\) make it to be in the quantum state \(\psi\)!
Although it is correct that the statistical interpretation allows for different ways the wavefunction could be, I have presented several arguments that uncover the problems of a \(\psi\)epistemic or a complete wavefunction. These arguments are similar in kind to arguments that have been made about the contextuality [39] and nonlocality of quantum mechanics [8]. The KochenSpecker theorem concludes that a \(\psi\)incomplete wavefunction can only be supplemented by contextual variables (that is, variables that lead to different empirical results depending on how they are measured); Bell’s theorem says that as long as a certain kind of statistical independence is fulfilled the theory cannot explain certain correlations by a local mechanism. So even if a certain interpretation of quantum mechanics is incomplete, one can discover certain hidden structures of the theory or certain features of a possible completion. The same is the case for my defense of a \(\psi\)ontic and \(\psi\)incomplete wavefunction for the statistical interpretation.
This reading of the statistical interpretation would indeed break with Einstein’s view of assigning several wavefunctions to the same system but seems to back up my understanding of Ballentine of using the statistical interpretation for all practical purposes, while being open to a possible completion. Such an interpretation would also make the statistical interpretation fit into the ontological models framework without a revisionary interpretation of the ontic state \(\lambda\).
5 Conclusion
Is the statistical interpretation of quantum mechanics \(\psi\)epistemic? It could be. The core tenets of the interpretation do not settle the question as to whether the wave function is \(\psi\)epistemic or \(\psi\)ontic. That is left open, to be decided by deeper physics. If the statistical interpretation allows for the swap of some particles prepared with different wavefunctions, the wavefunction would be \(\psi\)epistemic, but then it would be ruled out by the PBR theorem, unless one is willing to violate preparation independence and support a quantum theory that invokes some form of superdeterminism. The wavefunction would be \(\psi\)onic, if the statistical interpretation is completed by a quantum theory that describes the state of individual systems.
The way the statistical interpretation is formulated by Ballentine would paradoxically make both the \(\psi\)epistemic and the \(\psi\)ontic path viable. The underlying issue is that this interpretation in its very definition is incomplete.
Notes
An anonymous reviewer challenged my distinction, in the following way (I thank the reviewer for this argument). First, Harrigan and Spekkens [33] had in mind a \(\psi\)physical wavefunction when defining a \(\psi\)ontic wavefunction; therefore, \(\psi\)nomological wavefunctions cannot be \(\psi\)ontic. I could not retrieve this presupposition in Harrigan and Spekkens’ paper. Harrigan and Spekkens are rather indifferent to the metaphysical status of the wavefunction. Instead, they propose a formal relationship between the ontic state and the wavefunction elucidating how the properties of a physical system are represented by the wavefunction. Maudlin [45, p. 8] also regards nomological wavefunctions as examples of \(\psi\)ontic wavefunctions and mentions even more subcategories of \(\psi\)ontic wavefunctions than I do. Second, if the wavefunction is \(\psi\)nomological it cannot represent the physical properties of the ontic state \(\lambda\) qua abstract entity. I suppose that underlying this argument is too strict a reading of the word ”physical” in the definition of the reality criterion. A \(\psi\)nomological wavefunction can still represent parts of the complete physical properties of the quantum system, even if it is an abstract nomological entity. The wavefunction does not need to be a physical object, like a field, to be included in the physical properties of the quantum system.
The philosophical literature on the GRW theories seems to imply that the universal wavefunction is \(\psi\)nomological. It still needs to be worked out what a \(\psi\)physical wavefunction amounts to for collapse theories.
I thank Travis Norsen for this insight.
They say the same also on p. 1318 and 1328.
It is also possible to have an epistemic interpretation of the wavefunction without it being \(\psi\)epistemic. Therefore, the distinction between \(\psi\)ontic and \(\psi\)epistemic wavefunctions does not cover all the ways one can interpret the wavefunction. Pace Oldofredi and López [50, pp. 1320], the wavefunction in QBism would be such an example, as this theory denies the existence of \(\lambda\), which is necessary for a wavefunction to be \(\psi\)epistemic. What the ontology of QBism actually is is still debated (see, for instance [13]). On the other hand, Oldofredi and López [50, p. 1341] classify relational quantum mechanics to be \(\psi\)epistemic because: “For RQM, by contrast, the quantum state is merely a useful tool for calculation and prediction, and because of this it is \(\psi\)epistemic.”
One may think that in order to assign an ontic state to a physical system, one needs to presuppose that the system is sufficiently isolated from the environment. For example, if one entangles two electrons in the singlet state, neither electron has an ontic state, because we cannot assign a (pure) wavefunction to either electron. I think this example confuses the ontic state \(\lambda\) with the wavefunction \(\psi\), which is supposed to describe or represent properties of the ontic state. The ontic state is independent of a physical theory, and it captures all the physical properties of the system. Therefore, both electrons have their own ontic state. The ontological model framework investigates whether a purestate wavefunction gives a complete or partial physical description of the ontic state of the system. According to quantum mechanics, neither electron in the singlet state can be assigned a purestate wavefunction, but this does not mean that there is no complete physical description of them. One may criticize the ontological models framework, however, that it ignores density matrices as representations of the ontic state [15]. But this criticism is rather about the representation of \(\lambda\) than of \(\lambda\) itself. It would be a worthwhile project to investigate the implications for density matrix realism [17], if one generalizes the ontological models framework and the PBR theorem. (I thank Charles Sebens and Eddy Chen for helpful discussions on these issues.)
One may reason that the preparation devices need to be spacelike separated to run independently. That is just one way to justify that they have to run independently. Even if the preparation devices are not spacelike separated assumption 2 may still hold if there is no causal relation between the devices.
Theories that deny the reality assumption are QBism [29, 30], radical epistemicism [9,10,11], relational quantum mechanics [21, 49, 50, 53], and pragmatist interpretations of quantum mechanics [34]. Theories that deny preparation independence are Spekken’s toy model [55] and different proposals for superdeterministic theories [19, 35, 51, 57]. An excellent critical review of this approach is Chen [18].
For our purposes it is not important to explain the details of this measurement procedure. The product states get projected onto a certain entanglement basis that gives rise to these probabilities.
The precise argument why the measurement apparatus has to show a result is a bit technical. Roughly speaking it goes like this. We deal here with a fourdimensional Hilbert space. Each outcome of the measurement device is associated with a basis vector in this Hilbert space. These basis vectors span the complete Hilbert space. So upon measurement any vector in this Hilbert space gets projected on one of these basis vectors and yields the corresponding value with a certain probability. In particular, the product states \(\vert \uparrow_z \rangle \vert \uparrow_z \rangle\), \(\vert \uparrow_z \rangle \vert \uparrow_x \rangle\), \(\vert \uparrow_x \rangle \vert \uparrow_z \rangle\), and \(\vert \uparrow_x \rangle \vert \uparrow_x \rangle\) are part of this Hilbert space. So it is impossible that the measurement device will yield nothing if fed with one of the problematic ontic states.
It is, in principle, a further option to have a \(\psi\)ontic wavefunction and deny preparation independence. Ciepielewski et al. [19] present such a model, although they do not defend it.
I thank Maaneli Derakhshani for this reference.
Fano et al. [27] contest that this is Einstein’s line of argument. According to them, Einstein argued only that if locality holds standard quantum mechanics must be \(\psi\)epistemic. It’s not so clear whether Einstein had a coherent view of what the statistical interpretation actually is. Sometimes Einstein can be read to advocate a \(\psi\)ontic interpretation but also a \(\psi\)epistemic interpretation in other contexts.
Ballentine could also deny the reality criterion (I thank an anonymous reviewer for raising this option). Then the statistical interpretation would not fit into the ontological models framework; it would be neither \(\psi\)ontic nor \(\psi\)epistemic; and the PBR theorem would not be applicable. The biggest problem I see here is that it becomes unclear what the statistical interpretation is about and how the statistical pattern is generated in the first place. If there is no ontological underpinning in terms of some objective properties, it is not obvious what a quantum system is and how this (nonexisting?) quantum system can interact with a measurement device. Oldofredi and López [50] will take a similar but less radical approach by revising instead of abolishing the reality criterion (see Sect. 4.2).
In their analysis of the statistical interpretation, Fano et al. [27] interpret the PBRtheorem to make such an interpretation impossible. Violation of preparation is in fact a way, although problematic, to retain a \(\psi\)epstemic wavefunction.
Fine [28] also discusses how Einstein interpreted quantum mechanics.
I also think that Oldofredi and López cite the wrong reason for why Harrigan and Spekkens consider the statistical interpretation to be \(\psi\)epistemic:
How do Harrigan and Spekkens reinforce their conclusion that the ensemble view is a \(\psi\)epistemic model? They answer it by saying that the notion of ‘ensemble” in Einstein’s jargon is nothing but a way to talk about probabilities reflecting an observer’s knowledge[.] [50, p. 1328]
Harrigan and Spekkens do not make the mistake of identifying \(\psi\)epistemic wavefunctions with epistemic interpretations of the wavefunction. Instead, they conclude that the wavefunction in the statistical interpretation to be \(\psi\)epistemic on two grounds. First, it is incomplete (according to Einstein and Ballentine). Second, Einstein gives an argument for associating two different wavefunctions to the same quantum system in his 1935 correspondence to Schrödinger.
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Hubert, M. Is the Statistical Interpretation of Quantum Mechanics ψOntic or ψEpistemic?. Found Phys 53, 16 (2023). https://doi.org/10.1007/s10701022006510
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DOI: https://doi.org/10.1007/s10701022006510