Holism and Nonseparability in Physics

First published Thu Jul 22, 1999; substantive revision Thu Mar 3, 2022

It has sometimes been suggested that quantum phenomena exhibit a characteristic holism or nonseparability, and that this distinguishes quantum from classical physics. One puzzling quantum phenomenon arises when one performs measurements on certain separated quantum systems. The results of some such measurements regularly exhibit patterns of statistical correlation that resist traditional causal explanation. Some have held that it is possible to understand these patterns as instances or consequences of quantum holism or nonseparability. Just what holism and nonseparability are supposed to be has not always been made clear, though, and each of these notions has been understood in different ways. Moreover, while some have taken holism and nonseparability to come to the same thing, others have thought it important to distinguish the two. Any evaluation of the significance of quantum holism and/or nonseparability must rest on a careful analysis of these notions and their physical applications.

1. Introduction

Holism has often been taken as the thesis that the whole is more than the sum of its parts. Several different interpretations of this epigram prove relevant to physics, as we shall see. Here is a correspondingly vague initial statement of nonseparability: The state of the whole is not constituted by states of its parts. It is already apparent both that holism and nonseparability are related notions and that their exact relation needs to be clarified.

In one interpretation, holism is a methodological thesis (Section 2), to the effect that the best way to study the behavior of a complex system is to treat it as a whole, and not merely to analyze the structure and behavior of its component parts. Alternatively, holism may be taken as a metaphysical thesis (Section 3): There are some wholes whose natures are simply not determined by the nature of their parts. Methodological holism stands opposed to methodological reductionism, in physics as well as in other sciences. But it is a certain variety of metaphysical holism that is more closely related to nonseparability. What is at issue here is the extent to which the properties of the whole are determined by the properties of its parts: property holism (Section 4) denies such determination, and thereby comes very close to a thesis of nonseparability. In turn, nonseparability can be analyzed either as state nonseparability (Section 5), or as spatiotemporal nonseparability (Section 6). By and large, a system in classical physics can be analyzed into parts, whose states and properties determine those of the whole they compose (Section 7). But all hands agree that the state of a system in quantum theory resists such analysis. The quantum state of a system specifies its chances of exhibiting various properties on measurement. In ordinary quantum mechanics, the most complete such specification is given by what is called a pure state. Even when a compound system has a pure state, some of its subsystems may not have their own pure states. Emphasizing this characteristic of quantum mechanics, Schrödinger described such component states as “entangled” (Section 8). Superficially, such entanglement of states already demonstrates nonseparability. At a deeper level, it has been maintained that the puzzling statistics that arise from measurements on entangled quantum systems either demonstrate, or are explicable in terms of, holism or nonseparability rather than any problematic action at a distance (Sections 8, 9). The Aharonov-Bohm effect (Section 10) also appears to exhibit action at a distance, as the behavior of electrons is modified by a magnetic field they never experience. But this effect may be understood instead as a result of the local action of nonseparable electromagnetism. And indeed, this type of holism is not rooted in quantum mechanics or entanglement: though the measurement of the Aharonov-Bohm effect uses quantum ingredients, it builds on the existence of non-separable quantities in classical gauge theory (e.g. electromagnetism) in a vacuum. But even focussing on theories without gauge symmetry, we can obtain puzzling correlations between distant simultaneous measurements in the vacuum, according to quantum field theory (Section 12). A form of quantum theory used to study them represents systems by algebras of operators with new kinds of states defined on them, thereby making room for failures of state and system separability with no analogs in ordinary quantum mechanics. String theory (Section 13) is an ambitious research program in the framework of quantum field theory. According to string theory, all fundamental particles can be considered to be excitations of underlying non-pointlike entities in a multi-dimensional space. The particles’ intrinsic charge, mass and spin may then arise as nonseparable features of the world at the deepest level.

2. Methodological Holism

Methodologically, holism stands opposed to reductionism, somewhat as follows.

Methodological Holism: An understanding of a certain kind of complex system is best sought at the level of principles governing the behavior of the whole system, and not at the level of the structure and behavior of its component parts.
Methodological Reductionism: An understanding of a complex system is best sought at the level of the structure and behavior of its component parts.

This seems to capture much of what is at stake in debates about holism in social and biological science. In social science, societies are the complex systems, composed of individuals; while in biology, the complex systems are organisms, composed of cells, and ultimately of proteins, DNA and other molecules. A methodological individualist maintains that the right way to approach the study of a society is to investigate the behavior of the individual people that compose it. A methodological holist, on the other hand, believes that such an investigation will fail to shed much light on the nature and development of society as a whole. There is a corresponding debate within physics. Methodological reductionists favor an approach to (say) condensed matter physics which seeks to understand the behavior of a solid or liquid by applying quantum mechanics (say) to its component molecules, atoms, ions or electrons. Methodological holists think this approach is misguided: As one condensed matter physicist put it “the most important advances in this area come about by the emergence of qualitatively new concepts at the intermediate or macroscopic levels—concepts which, one hopes, will be compatible with one’s information about the microscopic constituents, but which are in no sense logically dependent on it.” (Leggett 1987, p.113)

It is surprisingly difficult to find methodological reductionists among physicists. The elementary particle physicist Steven Weinberg, for example, is an avowed reductionist. He believes that by asking any sequence of deeper and deeper why-questions one will arrive ultimately at the same fundamental laws of physics. But this explanatory reductionism is metaphysical in so far as he takes explanation to be an ontic rather than a pragmatic category. On this view, it is not physicists but the fundamental laws themselves that explain why “higher level” scientific principles are the way they are. Weinberg (1992) explicitly distinguishes his view from methodological reductionism by saying that there is no reason to suppose that the convergence of scientific explanations must lead to a convergence of scientific methods.

3. Metaphysical Holism

The metaphysical holist believes that the nature of some wholes is not determined by that of their parts. One may distinguish three varieties of metaphysical holism: ontological, property and nomological holism.

Ontological Holism: Some objects are not wholly composed of basic physical parts.
Property Holism: Some objects have properties that are not determined by physical properties of their basic physical parts.
Nomological Holism: Some objects obey laws that are not determined by fundamental physical laws governing the structure and behavior of their basic physical parts.

All three theses require an adequate clarification of the notion of a basic physical part. One way to do this would be to consider objects as basic, relative to a given class of objects subjected only to a certain kind of process, just in case every object in that class continues to be wholly composed of a fixed set of these (basic) objects. Thus, atoms would count as basic parts of hydrogen if it is burnt to form water, but not if it is converted into helium by a thermonuclear reaction. But this way excludes consideration of time-slices and point events (for example) as basic (spatio)temporal parts of an object. What counts as a part, and what parts are basic, are matters best settled in a particular context of enquiry.

Weinberg’s (1992) reductionism is opposed to nomological holism in science. He claims, in particular, that thermodynamics has been explained in terms of particles and forces, which could hardly be the case if thermodynamic laws were autonomous. In fact thermodynamics presents a fascinating but complex test case for the theses both of property holism and of nomological holism. One source of complexity is the variety of distinct concepts of both temperature and entropy that figure in both classical thermodynamics and statistical mechanics. Another is the large number of quite differently constituted systems to which thermodynamics can be applied, including not just gases and electromagnetic radiation but also magnets, chemical reactions, star clusters and black holes. Both sources of complexity require a careful examination of the extent to which thermodynamic properties are determined by the physical properties of the basic parts of thermodynamic systems. A third difficulty stems from the problematic status of the probability assumptions that are required in addition to the basic mechanical laws in order to recover thermodynamic principles within statistical mechanics. (An important example is the assumption that the micro-canonical ensemble is to be assigned the standard, invariant, probability distribution.) Since the basic laws of mechanics do not determine the principles of thermodynamics without some such assumptions (however weak), there may well be at least one interesting sense in which thermodynamics establishes nomological holism. The related entry philosophy of statistical mechanics contains further discussion of these difficulties, especially in Section 6.

4. Property/Relational Holism

While some form of ontological holism has occasionally been considered, the variety of metaphysical holism most clearly at issue in quantum mechanics and in gauge theory is property holism. But to see just what the issue is we need a more careful formulation of that thesis.

First the thesis should be contextualized to physical properties of composite physical objects. We are interested here in how far a physical object’s properties are fixed by those of its parts, not in some more general determinationist physicalism. Next, to arrive at an interesting formulation of property holism we must accept that this thesis is not only concerned with properties, and not concerned with all properties. The properties of a whole will typically depend upon relations among its proper parts as well as on properties of the individual parts. But if we are permitted to consider all properties and relations among the parts, then these trivially determine the properties of the whole they compose. For one relation among the parts is what we might call the complete composition relation—that relation among the parts which holds just in case they compose this very whole with all its properties.

Let us call a canonical set of properties and relations of the parts which may or may not determine the properties and relations of the whole the supervenience basis. To avoid trivializing the theses we are trying to formulate, only certain properties and relations can be allowed in the supervenience basis. The intuition as to which these are is simple—the supervenience basis is to include just the qualitative intrinsic properties and relations of the parts, i.e., the properties and relations which these bear in and of themselves, without regard to any other objects, and irrespective of any further consequences of their bearing these properties for the properties of any wholes they might compose. Unfortunately, this simple intuition resists precise formulation. It is notoriously difficult to say precisely what is meant either by an intrinsic property or relation, or by a purely qualitative property or relation. And the other notions appealed to in expressing the simple intuition are hardly less problematic. But, imprecise as it is, this statement serves already to exclude certain unwanted properties and relations, including the complete composition relation, from the supervenience basis.

Finally, we arrive at the following opposing theses:

Physical Property Determination: Every qualitative intrinsic physical property and relation of a set of physical objects from any domain D subject only to type P processes supervenes on qualitative intrinsic physical properties and relations in the supervenience basis of their basic physical parts relative to D and P.
Physical Property Holism: There is some set of physical objects from a domain D subject only to type P processes, not all of whose qualitative intrinsic physical properties and relations supervene on qualitative intrinsic physical properties and relations in the supervenience basis of their basic physical parts (relative to D and \(P)\).

If we take the real state of a set of physical objects to be given by their qualitative intrinsic physical properties and relations, then physical property determination says (while physical property holism denies) that the real state of wholes is determined by the real state of their parts.

There is some residual unclarity in the notion of supervenience that figures in these theses. The idea is familiar enough—that there can be no relevant difference in objects in D without a relevant difference in their basic physical parts. I take it that the modality involved here is not logical but broadly physical. One might try to explicate the notion of supervenience here in terms of models of a true, descriptively complete, physical theory. At issue is whether such a physical theory has two models which agree on the qualitative intrinsic physical properties and relations of the basic parts of one or more objects in D but disagree on some qualitative intrinsic property or relation of these objects.

Teller (1989) has introduced the related idea of what he calls relational holism.

Relational Holism: There are non-supervening relations—that is, relations that do not supervene on the nonrelational properties of the relata. (p. 214)

Within physics, this specializes to a close relative of physical property holism, namely:

Physical Relational Holism: There are physical relations between some physical objects that do not supervene on their qualitative intrinsic physical properties.

Physical property holism entails physical relational holism, but not vice versa. For suppose that F is some qualitative intrinsic physical property or relation of one or more elements of D that fails to supervene on qualitative intrinsic physical properties and relations in the supervenience basis of their basic physical parts. We may define a (non-intrinsic) physical relation \(R_{F}\) to hold of the basic physical parts of elements of D if and only if F holds of these elements. Clearly \(R_{F}\) does not supervene on the qualitative intrinsic physical properties of these parts. So physical property holism entails physical relational holism. But the converse entailment fails. For let \(R_{G}\) be a physical relation that holds between the basic parts of some elements in D when and only when those elements are in the relation \(S_{G}\). \(R_{G}\) may fail to supervene on the qualitative intrinsic physical properties of these basic parts, even though all qualitative intrinsic physical properties and relations of elements of D (including \(S_{G}\)) supervene on the qualitative intrinsic physical properties and relations of their basic parts.

Physical relational holism seems at first sight too weak to capture any distinctive feature of quantum phenomena: even in classical physics the spatiotemporal relations between physical objects seem not to supervene on their qualitative intrinsic physical properties. But when he introduced relational holism Teller (1987) maintained a view of spacetime as a quantity: On this view spatiotemporal relations do in fact supervene on qualitative intrinsic physical properties of ordinary physical objects, since these include their spatiotemporal properties.

5. State Nonseparability

Physics treats systems by assigning them states. The thermodynamic state of a gas specifies its pressure, volume and temperature. The state of a system of classical particles is represented as a point in a phase space coordinatized by their positions and momenta. One expects that if a physical system is composed of physical subsystems, then both the composite system and its subsystems will be assigned states by the relevant physical theory. One further expects that the state of the whole will not be independent of those of its parts, and specifically that if a system is composed of two subsystems, A and B, then it will satisfy a principle formulated by Einstein (1935). Howard (1985, p.180) gives the following translation of this principle, which I’ll call the

Real State Separability Principle: The real state of the pair \(AB\) consists precisely of the real state of A and the real state of B, which states have nothing to do with one another.

But the assignment of states to systems in quantum mechanics seems not to conform to these expectations (see related entry quantum mechanics). Recall that the quantum state of a system specifies its chances of exhibiting various properties on measurement. At least in ordinary quantum mechanics, the mathematical representative of this state is an object defined in a Hilbert space—a kind of vector space. This is analogous in some ways to the representation of the state of a system of particles in classical mechanics in a phase space. Let us formulate a principle of

State Separability: The state assigned to a compound physical system at any time is supervenient on the states then assigned to its component subsystems.

This principle could fail in one of two ways: the subsystems may simply not be assigned any states of their own, or else the states they are assigned may fail to determine the state of the system they compose. Interestingly, state assignments in quantum mechanics have been taken to violate state separability in both ways.

The quantum state of a system may be either pure or mixed (see related entry quantum mechanics). In ordinary quantum mechanics a pure state is represented by a vector in the system’s Hilbert space. On one common understanding, any entangled quantum systems violate state separability in so far as a vector representing the state of the system they compose does not factorize into a product of vectors, one in the Hilbert space of each individual subsystem, that could be taken to represent their pure states. On the other hand, in such a case each subsystem may be uniquely assigned what is called a mixed state represented in its Hilbert space not by a vector but by a more general object—a so-called von Neumann density operator. But then state separability fails for a different reason: the subsystem mixed states do not uniquely determine the compound system’s state. A failure of state separability may not occasion much surprise if states are thought of merely in their role of specifying a system’s chances of exhibiting various possible properties on measurement. But it becomes more puzzling if one believes that a system’s quantum state also has a role in specifying some or all of its categorical properties. For that role may connect a failure of state separability to metaphysical holism and nonseparability.

6. Spatial and Spatiotemporal Nonseparability

The idea is familiar (particularly to Lego enthusiasts!) that if one constructs a physical object by assembling its physical parts, then the physical properties of that object are wholly determined by the properties of the parts and the way it is put together from them. A principle of spatial separability tries to capture that idea.

Spatial Separability: The qualitative intrinsic physical properties of a compound system are supervenient on those of its spatially separated component systems together with the spatial relations among these component systems.

If we identify the real state of a system with its qualitative intrinsic physical properties, then spatial separability is related to a separability principle stated by Howard (1985, p. 173) to the effect that any two spatially separated systems possess their own separate real states. It is even more closely related to Einstein’s (1935) real state separability principle. Indeed, Einstein formulated this principle in the context of a pair \(A, B\) of spatially separated systems.

Spatial nonseparability —the denial of spatial separability—is also closely related to physical property holism. At least classically, spatial relations are the only clear examples of qualitative intrinsic physical relations required in the supervenience basis for physical property determination/holism: other intrinsic physical relations seem to supervene on them, while any instance of physical property holism due to the spatial separation of basic physical parts would entail spatial nonseparability. But if one thought a spatially localized object has a determinate value for a magnitude like mass only by virtue of its mass relations to other such objects elsewhere then one might decide to include those relations in the supervenience basis also (see Dasgupta (2013)).

If we take a spacetime perspective, then spatial separability naturally generalizes to

Spatiotemporal Separability: Any physical process occupying spacetime region R supervenes upon an assignment of qualitative intrinsic physical properties at spacetime points in R.

Spatiotemporal separability is a natural restriction to physics of David Lewis’s (1986, p. x) principle of Humean supervenience. It is also closely related to another principle formulated by Einstein (1948, pp. 233–234 of Howard’s (1989) translation) in the following words: “An essential aspect of [the] arrangement of things in physics is that they lay claim, at a certain time, to an existence independent of one another, provided these objects ‘are situated in different parts of space’” (the context of the quote suggests that Einstein intended his principle to apply to objects provided they occupy spacelike separated regions of spacetime).

As Healey (1991, p. 411) shows, spatiotemporal separability entails spatial separability, and so spatial nonseparability entails spatiotemporal nonseparability. Because it is both more general and more consonant with a geometric spacetime viewpoint, it seems reasonable to consider spatiotemporal separability to be the primary notion. Accordingly, separability without further qualification will mean spatiotemporal separability in what follows, and nonseparability will be understood as its denial.

Nonseparability: Some physical process occupying a region R of spacetime is not supervenient upon an assignment of qualitative intrinsic physical properties at spacetime points in R.

It is important to note that nonseparability entails neither physical property holism nor spatial nonseparability: a process may be nonseparable even though it involves objects without proper parts. But this section has explained that either of the latter principles entails nonseparability under quite weak assumptions.

7. Holism and Nonseparability in Classical Physics

Classical physics presents no definitive examples of either physical property holism or nonseparability. As section 6 explained, almost any instance of physical property holism would demonstrate nonseparability. This justifies restricting attention to the latter notion. Now the assumption that all physical processes are completely described by a local assignment of magnitudes forms part of the metaphysical background to classical physics. In Newtonian spacetime, the kinematical behavior of a system of point particles under the action of finite forces is supervenient upon ascriptions of particular values of position and momentum to the particles along their trajectories. This supervenience on local magnitudes extends also to dynamics if the forces on the particles arise from fields defined at each spacetime point.

The boiling of a kettle of water is an example of a more complex physical process. It consists in the increased kinetic energy of its constituent molecules permitting each to overcome the short range attractive forces which otherwise hold it in the liquid. It thus supervenes on the assignment, at each spacetime point on the trajectory of each molecule, of physical magnitudes to that molecule (such as its kinetic energy), as well as to the fields that give rise to the attractive force acting on the molecule at that point.

As an example of a process in Minkowski spacetime (the spacetime framework for Einstein’s special theory of relativity), consider the propagation of an electromagnetic wave through empty space. This is supervenient upon an ascription of the electromagnetic field tensor at each point in the spacetime.

But it does not follow that classical processes like these are separable. For one may question whether an assignment of basic magnitudes at spacetime points amounts to or results from an assignment of qualitative intrinsic properties at those points. Take instantaneous velocity, for example: this is usually defined as the limit of average velocities over successively smaller temporal neighborhoods of that point. This provides a reason to deny that the instantaneous velocity of a particle at a point supervenes on qualitative intrinsic properties assigned at that point. Similar skeptical doubts can be raised about the intrinsic character of other “local” magnitudes such as the density of a fluid, the value of an electromagnetic field, or the metric and curvature of spacetime (see Butterfield (2006)).

One response to such doubts is to admit to a minor consequent violation of separability while introducing a weaker notion, namely

Weak Separability: Any physical process occupying spacetime region R supervenes upon an assignment of qualitative intrinsic physical properties at points of R and/or in arbitrarily small neighborhoods of those points.

Along with a correspondingly strengthened notion of

Strong Nonseparability: Some physical process occupying a region R of spacetime is not supervenient upon an assignment of qualitative intrinsic physical properties at points of R and/or in arbitrarily small neighborhoods of those points.

No holism need be involved in a process that is nonseparable, but not strongly so, as long as the basic parts of the objects involved in it are themselves taken to be associated with arbitrarily small neighborhoods rather than points. Versions of Weak Separability are offered by both Belot (1998, p. 540), whose term is Synchronic Locality, and by Myrvold (2011, p. 425), who calls it Patchy Separability. The idea is that the state of a region supervenes on assignments of intrinsic properties to patches of the region, where the patches may be taken to be arbitrarily small.

Any physical process fully described by a local spacetime theory will be at least weakly separable. For such a theory proceeds by assigning geometric objects (such as vectors or tensors) at each point in spacetime to represent physical fields, and then requiring that these satisfy certain field equations. But processes fully described by theories of other forms will also be separable. These include many theories which assign magnitudes to particles at each point on their trajectories. Of familiar classical theories, it is only theories involving direct action between spatially separated particles which involve nonseparability in their description of the dynamical histories of individual particles. But such processes are weakly separable within spacetime regions that are large enough to include all sources of forces acting on these particles, so that the appearance of strong nonseparability may be attributed to a mistakenly narrow understanding of the spacetime region these processes actually occupy.

The propagation of gravitational energy according to general relativity apparently involves strongly nonseparable processes, since gravitational energy cannot be localized (it does not contribute to the stress-energy tensor defined at each point of spacetime as do other forms of energy). But even a non-locally-defined gravitational energy will still be supervenient upon the metric tensor defined at each point of the spacetime, and so the process of its propagation will be weakly separable.

The definition of nonseparability becomes problematic in general relativity, since its application requires that one identify the same region R in possible spacetimes with different geometries. But while there is no generally applicable algorithm for making a uniquely appropriate identification, some identification may appear salient in a particular case. For example, one can meaningfully discuss whether or not the field is the same everywhere in the region outside the solenoid in the Aharonov-Bohm effect with an increased current flowing, even though the size of the current will have a (tiny) influence on the geometry of that region. Note that the definition of nonseparability does not require that one identify the same point in spacetimes of distinct geometries.

While strictly outside the domain of classical physics, quantum phenomena such as the Aharonov-Bohm effect may be considered manifestations of nonseparability and holism even in classical electromagnetism. Nonseparability would be a trivial notion if no qualitative intrinsic physical properties were ever assigned at spacetime points or in their neighborhoods. But this would require a thorough-going relationism that took not just geometric but all local features to be irreducibly relational (cf. Esfeld (2004)). We will return to this point in our discussion of the Aharonov-Bohm effect.

8. The Quantum Physics of Entangled Systems

Quantum entanglement is in the first instance a relation between not physical but mathematical objects representing the states of quantum systems. Different forms of quantum theory represent quantum states of various systems by different kinds of mathematical object. So the concept of quantum entanglement has been expressed by a family of definitions, each appropriate to a specific form and application of quantum theory (see Earman (2015)). The first definition (Schrödinger (1935)) was developed in the context of applications of ordinary non-relativistic quantum mechanics to pairs of distinguishable particles that have interacted, such as an electron and proton.

A hydrogen atom may be represented in ordinary non-relativistic quantum mechanics as a quantum system composed of two subsystems: an electron e and a nuclear proton p. When isolated, its quantum state may be represented by a vector \(\Psi\) in a space H constructed as a tensor product of spaces \(H_{p}\) and \(H_{e}\) used to represent states of \(e, p\) respectively. The states of \(e, p\) are then defined as entangled if and only if

\[ \Psi \ne \Psi_{p} \otimes \Psi_{e}\]

for every pair of vectors \(\Psi_{p}, \Psi_{e}\) in \(H_{p}\), \(H_{e}\) respectively. This definition naturally generalizes to systems composed of n distinguishable particles. But alternative definitions seem preferable for a collection of indistinguishable particles—of electrons or of photons for example (see Ghirardi et al. (2002), Ladyman et al. (2013)).

It follows that the states of electron and proton in an isolated hydrogen atom are entangled. But one may also represent the hydrogen atom as composed of a center-of-mass subsystem C and a relative subsystem R represented by vector states \(\Psi_{C}\), \(\Psi_{R}\) in \(H_{C}, H_{R}\) respectively such that

\[ \Psi = \Psi_{C} \otimes \Psi_{R}\]

If the state of the hydrogen atom is represented by \(\Psi\) then the states of quantum subsystems \(C, R\) are not entangled but the states of quantum subsystems \(p, e\) are entangled. This illustrates the important point that one cannot draw metaphysical conclusions from a mathematical condition of quantum entanglement without first deciding which quantum systems are physical parts composing some physical whole. It may seem natural to take the physical parts of a hydrogen atom to be an electron and a proton. But note that the state of an isolated hydrogen atom is usually represented by \(\Psi_{R}\), and not by \(\Psi\) or \(\Psi_{e}\).

Viewed as basic physical parts of a hydrogen atom represented by state \(\Psi\), its electron and proton may be considered entangled physical parts since \(\Psi\) cannot be expressed as a product of vectors representing the state of each. The electron and the proton may each be assigned a mixed state, but these do not uniquely determine the state \(\Psi\): state separability is violated. This may occasion no surprise if a system’s state merely specifies its chances of exhibiting various possible properties on measurement. But it may have metaphysical significance if a system’s quantum state plays a role in specifying its categorical properties—its real state, so that the real state separability principle is threatened. His commitment to this principle is one reason why Einstein denied that a physical system’s real state is given by its quantum state (though it’s not clear what he thought its real state consisted in). But according to (one variant of) the rival Copenhagen interpretation, the quantum state gives a physical system’s real dynamical state by specifying that it contains just those qualitative intrinsic quantum dynamical properties to which it assigns probability 1. On this last interpretation, violation of state separability in quantum mechanics leads to physical property holism: it implies, for example, that a pair of fundamental particles may have the intrinsic property of being spinless even though this is not determined by the intrinsic properties and relations of its component particles.

If an entangled pure vector state of a pair of quantum systems violates state separability then there are measurements of dynamical variables (one on each subsystem) whose joint quantum probability distribution cannot be expressed as a product of probability distributions for separate measurements of each variable. Quantum theory predicts such a probability distribution for each of many types of spatially separated measurements of variables including spin and polarization components on a pair of entangled physical entities assigned such a state, and many of these distributions have been experimentally verified. If one thought that quantum theory treats each dynamical variable by replacing a precise real value assignment by a probability distribution for the results of measurements of that dynamical variable, one might take this already to violate the real state separability principle. But if one entertains a theory that supplements the quantum state by values of additional “hidden” variables, then the quantum probabilities would be taken to arise from averaging over many distinct hidden states. In that case, it would rather be the probability distribution conditional on a complete specification of the values of the hidden variables that should be taken to specify the underlying chances of system and subsystems exhibiting various possible properties on measurement. The real state might then include all these conditional probability distributions. The best known example of such a theory is the Bohm theory (see the entry on Bohmian mechanics), where the “hidden” variables are spatial positions. In each specific experimental context all conditional probabilities are 0 or 1, so the joint conditional probability distributions indeed factorize. But the outcome of a measurement of a chosen dynamical variable on one subsystem depends on what dynamical variable is chosen and measured on the other, no matter just when or how far apart these measurements are selected and made.

Bell (1964, [2004]) reasoned that any local hidden variable theory must yield conditional probabilities of 0 or 1 for each local outcome in order to reproduce all quantum predictions but could not permit these to depend on the choice of distant measurement. He then proved that the probabilistic predictions of any local hidden variable theory must satisfy particular inequalities violated by predictions of quantum theory for certain entangled state assignments (see entry Bell’s Theorem). In later work Bell (1990, [2004]) generalized this argument to apply to any theory of a certain type meeting a condition he called Local Causality which, he claimed, quantum mechanics does not meet. Howard (1989, 1992) took outcome independence — the probabilistic independence of the outcomes of a given pair of measurements, one on each of a pair of entangled systems, conditional on definite values for any assumed hidden variables on the joint system—as a separability condition. Outcome independence may be contrasted with parameter independence—the condition that, given a definite hidden variable assignment, the outcome of a measurement on one of a pair of entangled systems is probabilistically independent of what measurement, if any, is made on the other system. Together with parameter independence, outcome independence implies the factorization of conditional probabilities that leads to what are now called Bell inequalities. These inequalities constrain the patterns of statistical correlations to be expected between the results of measurements of variables such as spin and polarization on a pair of entangled systems in any quantum state. Quantum mechanics predicts, and experiment confirms, that such Bell inequalities do not always hold. The Bohm theory accommodates this fact by its violation of parameter dependence, and hence Local Causality. But Howard (1989), as well as Teller (1989), suggested that we appeal instead to a failure of outcome independence to understand why Bell inequalities do not always hold, and that this failure is associated rather with holism or nonseparability. Howard (1989) blamed the violation of Bell inequalities on the violation of his separability condition: Teller (1989) took it to be a manifestation of relational holism. They both acquit parameter independence of blame because they believe that (at least when the measurement events on the entangled systems are spacelike separated) parameter independence (unlike outcome independence) is a consequence of relativity theory: (note that the Bohm theory requires a preferred frame not provided by relativity theory).

Henson (2013) and others have questioned this line of reasoning, including the conclusion that its appeal to holism or nonseparability helps one to understand how these correlations involving entangled systems come about without any action at a distance that violates relativity theory, Local Causality or Einstein’s (1948)

Principle of Local Action: If A and B are spatially distant things, then an external influence on A has no immediate effect on B.

Howard’s (1989,1992) identification of outcome independence with a separability condition has proved controversial, as has Teller’s (1989) claim that violations of Bell inequalities are no longer puzzling if one embraces (physical) relational holism (Laudisa 1995; Berkowitz 1998; Henson 2013). Winsberg and Fine (2003) object that separability requires only that the conditional joint probabilities be determined as some function of the marginal probabilities, whereas outcome independence arbitrarily restricts this to be the product function. By allowing other kinds of functional dependence they are able to construct models of experiments whose results would exhibit violations of Bell inequalities. They claim that these models are both local and separable even though they violate outcome independence. But Fogel (2007) presents alternative formalizations of the separability condition, of which several indeed imply outcome independence. The view that violations of outcome independence are consistent with relativity theory, while violations of parameter independence are not, has also been criticized (Jones & Clifton 1993; Maudlin 2011). But Myrvold (2016) has responded by arguing that locally-initiated state-vector collapse in violation of outcome dependence may be perfectly compatible with relativity.

While diverging from the Copenhagen prescription mentioned above, some modal interpretations take real states of systems to be closely enough related to quantum states that entangled systems’ violation of quantum state separability implies some kind of holism or nonseparability. Van Fraassen (1991, p. 294), for example, sees his modal interpretation as committed to “a strange holism” because it entails that a compound system may fail to have a property corresponding to a tensor product projection operator \(P\otimes I\) even though its first component has a property corresponding to P. In fact, a clearer case of holism would arise in a modal interpretation that implied that the component lacked P while the compound had \(P\otimes I\): ceteris paribus, that would provide an instance of physical property holism. Healey (1989,1994) offered a modal interpretation and used it to present a model account of the puzzling correlations which portrays them as resulting from the operation of a process that violates both spatial and spatiotemporal separability. He argued that, on this interpretation, the nonseparability of the process is a consequence of physical property holism; and that the resulting account yields genuine understanding of how the correlations come about without any violation of relativity theory or Local Action. But subsequent work by Clifton and Dickson (1998) and Myrvold (2001) cast doubt on whether the account can be squared with relativity theory’s requirement of Lorentz invariance. More recently Healey (2016) has given a different account of how quantum theory may be used to explain violations of Bell inequalities consistent with Lorentz invariance and Local Action. This account involves no metaphysical holism or nonseparability.

Esfeld (2001) takes holism, in the quantum domain and elsewhere, to involve more than just a failure of supervenience. He maintains that a compound system is holistic in that its subsystems themselves count as quantum systems only by virtue of their relations to other subsystems together with which they compose the whole.

9. Ontological Holism in Quantum Mechanics?

As applied to physics, ontological holism is the thesis that there are physical objects that are not wholly composed of basic physical parts. Views of Bohr, Bohm and others may be interpreted as endorsing some version of this thesis. In no case is it claimed that any physical object has nonphysical parts. The idea is rather that some physical entities that we take to be wholly composed of a particular set of basic physical parts are in fact not so composed.

It was Bohr’s (1934) view that one can meaningfully ascribe properties such as position or momentum to a quantum system only in the context of some well-defined experimental arrangement suitable for measuring the corresponding property. He used the expression ‘quantum phenomenon’ to describe what happens in such an arrangement. In his view, then, although a quantum phenomenon is purely physical, it is not composed of distinct happenings involving independently characterizable physical objects—the quantum system on the one hand, and the classical apparatus on the other. And even if the quantum system may be taken to exist outside the context of a quantum phenomenon, little or nothing can then be meaningfully said about its properties. It would therefore be a mistake to consider a quantum object to be an independently existing component part of the apparatus-object whole.

Bohm’s (1980, 1993) reflections on quantum mechanics led him to adopt a more general holism. He believed that not just quantum object and apparatus, but any collection of quantum objects by themselves, constitute an indivisible whole. This may be made precise in the context of Bohm’s (1952) interpretation of quantum mechanics by noting that a complete specification of the state of the “undivided universe” requires not only a listing of all its constituent particles and their positions, but also of a field associated with the wave-function that guides their trajectories. If one assumes that the basic physical parts of the universe are just the particles it contains, then this establishes ontological holism in the context of Bohm’s interpretation. But there are alternative views of the ontology of the Bohm theory (see the entry Bohmian mechanics).

Some (Howard 1989; Dickson 1998) have connected the failure of a principle of separability to ontological holism in the context of violations of Bell inequalities. Howard (1989) formulates the following separability principle (pp. 225–6)

Howard Separability: The contents of any two regions of space-time separated by a nonvanishing spatiotemporal interval constitute separable physical systems, in the sense that (1) each possesses its own, distinct physical state, and (2) the joint state of the two systems is wholly determined by these separate states.

He takes Einstein to defend this as a principle of individuation of physical systems, without which physical thought “in the sense familiar to us” would not be possible. Howard himself contemplates the possible failure of this principle for entangled quantum systems, with the consequence that these could no longer be taken to be wholly composed of what are typically regarded as their subsystems. Dickson (1998), on the other hand, argues that such holism is not “a tenable scientific doctrine, much less an explanatory one” (p. 156).

One may try to avoid the conclusion that experimental violations of Bell inequalities manifest a failure of Local Action by invoking ontological holism for events. The idea would be to deny that these experiments involve distinct, spatiotemporally separate, measurement events, and to maintain instead that what we usually describe as separate measurements involving an entangled system in fact constitute one indivisible, spatiotemporally disconnected, event with no spatiotemporal parts. But such ontological holism conflicts with the criteria of individuation of events inherent in both quantum theory and experimental practice.

10. The Aharonov-Bohm Effect and Field Holonomies

Aharonov and Bohm (1959) drew attention to the quantum mechanical prediction that an interference pattern due to a beam of charged particles could be produced or altered by the presence of a constant magnetic field in a region from which the particles were excluded. This effect has since been experimentally demonstrated. At first sight, the Aharonov-Bohm effect seems to involve action at a distance. It seems clear that the (electro-)magnetic field acts on the particles since it affects the interference pattern they produce; and this must be action at a distance since the particles pass through a region from which that field is absent. But alternative accounts of the phenomenon are possible which portray it rather as a manifestation of (strong) nonseparability (Healey 1997). There need be no action at a distance if the behavior both of the charged particles and of electromagnetism are nonseparable processes. While such a treatment of electromagnetism (and other gauge theories) is increasingly common in physics, to treat the motion of the charged particles as a nonseparable process is to endorse a particular position on how quantum mechanics is to be interpreted.

An interpretation of quantum mechanics that ascribes a nonlocalized position to a charged particle on its way through the apparatus is committed to a violation of spatiotemporal separability in the Aharonov-Bohm effect, since the particle’s passage constitutes a nonseparable process. To see why the electromagnetism that acts on the particles during their passage may also be taken to be nonseparable it is necessary to consider contemporary representations of electromagnetism in terms of neither fields nor vector potentials.

Following Wu and Yang’s (1975) analysis of the Aharonov-Bohm effect, it has become common to consider vacuum electromagnetism to be completely and nonredundantly described neither by the electromagnetic field, nor by its vector potential, but rather by the so-called Dirac phase factor:

\[ \exp[(ie/\hbar) \oint_C A_{\mu}(x^{\mu}.dx^{\mu}] \]

where \(A_{\mu}\) is the electromagnetic potential at spacetime point \(x^{\mu}\), e is the particles’ charge, and the integral is taken over each closed loop C in spacetime. This can be seen as an instance of the more general notion of the holonomy of a closed curve, a notion that has come to the fore in contemporary formulations of gauge theories including electromagnetism in terms of fiber bundles (Healey (2007)). Applied to the Aharonov-Bohm case, this means that the constant magnetic field is accompanied by an association of a phase factor \(S(C)\) with all closed curves C in space, where \(S(C)\) is defined by

\[ S(C) = \exp[-(ie/\hbar) \oint_C \mathbf{A(r).}d\mathbf{r}] \]

(where \(\mathbf{A}(\mathbf{r})\) is the magnetic vector potential at point \(\mathbf{r}\) of space). This approach has the advantage that since \(S(C)\) is gauge-invariant, it may readily be considered a physically real quantity. Moreover, the effects of electromagnetism in the field-free region may be attributed to the fact that \(S(C)\) is nonvanishing for certain closed curves C within that region. But it is significant that, unlike the magnetic field and its potential, \(S(C)\) is not defined at each point of space at each moment of time.

Can \(S(C)\) at some time be taken to represent an intrinsic property of a region of space corresponding to the curve C? There are two difficulties with this suggestion. The first is that the presence of the quantity e in the definition of \(S(C)\) appears to indicate that \(S(C)\) rather codes the effect of electromagnetism on objects with that specific charge. If in fact all charges are multiples of some minimal value e, then this would no longer be a problem: the value of \(S(C)\) for this minimal charge could then be viewed as representing an intrinsic property of a region of space corresponding to the curve C. If not, one could rather take

\[ I(C) = \oint_C \mathbf{A(r).}d\mathbf{r} \]

to represent an intrinsic property of C. The second difficulty is that closed curves do not correspond uniquely to regions of space: e.g., circling the region in which there is a magnetic field twice on the same circle will produce a different curve from circling it once. But this does not prevent one from taking \(S(C)\) at some time to represent an intrinsic property of a loop—the oriented region of space traced out by a closed curve C that intersects itself only at its end-point.

Once these difficulties have been handled, it is indeed possible to consider electromagnetism in the Aharonov-Bohm effect as faithfully represented at a time by a set of intrinsic properties of loops in space (or more generally space-time). But if one does so, then electromagnetism itself manifests (strong) nonseparability. For these intrinsic properties do not supervene on any assignment of qualitative intrinsic physical properties at spacetime points in the region concerned, nor even in arbitrarily small neighborhoods of those points. Whether the magnetic field remains constant or changes, the associated electromagnetism constitutes a nonseparable process, and so the Aharonov-Bohm effect violates spatiotemporal separability. If the motion of the particles through the apparatus is a nonseparable process, then it is possible to account for the \(AB\) effect in terms of a purely local interaction between electromagnetism and this process. For the particles effectively traverse loops traced out by closed curves C on their nonlocalized “trajectories”, and so they interact with electromagnetism precisely where this is defined.

Assuming it exhibits nonseparability, does the Aharonov-Bohm effect involve some kind of holism? The states of the particles need not be entangled with each other. But the state of the field may be thought to be holistic, in so far as the electromagnetic properties of loops do not supervene on properties (such as electric and magnetic field strengths) at the points that make up those loops. Since these are classical fields, the Aharonov-Bohm effect may be taken to demonstrate holism as well as nonseparability even in classical physics. However, a loop may also be thought of as traced out by a curve composed by “stringing together” a set of curves that trace out smaller loops, and removing segments traversed by two such curves in opposite directions. In that case, in a simply-connected region, the holonomy properties of any loop will be determined by those of an arbitrary set of smaller loops that compose it in this way. But when spacetime is not simply connected, there are loops that cannot be decomposed in this way: e.g. the loop that encompasses “the hole” in space cannot be further decomposed.

Myrvold (2011) interprets this result as saying that Weak Separability (what he calls Global Patchy Separability) fails for non-simply connected spacetimes, even though locally—over simply-connected patches—separability holds. Moreover, he here sees a marked distinction between the holonomy and the field formalism for gauge theories: in which supposedly separability always holds.

But Gomes (2021) effaces this distinction: he argues that a field formalism maintains separability, but only at the cost of dealing with gauge variant field variables. Once we restrict attention to the gauge-invariant quantities, the nonseparability illustrated above (using the holonomy variables) is restored. Moreover, he argues that only in a vacuum is nonseparability conditional on the topology of spacetime. In the presence of charged matter, there may be gauge-invariant quantities that cannot be decomposed into smaller patches, even for simply-connected regions. And this is easy to illustrate: suppose that, instead of the phase factor \(S(C)\), for a closed loop C, we write \(S(I)\) for an open segment I, that begins at point x and ends at point y. For a (Klein-Gordon) charged scalar field \(\varphi\) that vanishes everywhere except at small neighborhoods \(\nu_x, \nu_y\), of x and y, the function:

\[ \bar\varphi(x)S(I)\varphi(y) \]

is gauge-invariant, and it cannot be further decomposed into quantities with support on patches that do not include the entirety of \(I. \)For instance, if there are two patches, each containing either \(\nu_x\) or \(\nu_y\), then that patch has insufficient charges to complete \(S(I)\) into a gauge-invariant function. This example is in line with the physics literature, which largely takes gauge-invariance (and in particular the existence of a generalized Gauss constraint), to signal some general type of nonlocality (cf. Strocchi (2013, Ch. 7)).

11. Alternative Approaches

This entry has focused mainly on metaphysical holism and its relation to nonseparability. That there is a variety of alternative ways of understanding holism in physics is illustrated by a special issue of the journal Studies in the History and Philosophy of Physics (2004) devoted to this topic.

Seevinck (2004) proposes an epistemological criterion of holism and illustrates its application to physical theories. A physical theory counts as holistic by this criterion if and only if it is impossible in principle to infer the global properties, as assigned in the theory, by local resources available to an agent, where these include (at least) all local operations and classical communication. To apply this criterion it is necessary to specify how a theory assigns properties, a matter on which different interpretations of the theory may disagree. Seevinck (2004) argues that neither classical physics nor Bohmian mechanics is holistic in this sense. Applying the eigenvalue-eigenstate link to a particular state of a bipartite quantum system he then shows that this manifests epistemological holism, even when the state of the system is not entangled.

Placek (2004) understands quantum state holism as involving a thesis about probabilities: that the probability of a joint result of a combined measurement on a pair of entangled quantum systems is not determined by the probabilities of the two results. But he takes this to be only one ingredient of a more complete conception, whose formulation and analysis requires a modal framework combining indeterminism, (rudiments of) relativistic space-time, and probability—Belnap’s (1992) theory of branching space-times.

Esfeld (2004) argues for a metaphysics of relations based on a characterization of quantum entanglement in terms of non-separability, thereby regarding entanglement as a sort of holism. He there characterizes non-separability as follows:

Non-separability: The states of two or more systems are non-separable if and only if it is only the joint state of the whole that completely determines the state-dependent properties of each system and the correlations among these systems (to the extent that these are determined at all).

He takes this to imply that any case of quantum entanglement is a case of non-separability, and non-separability is the reason why quantum entanglement is a sort of holism. (He discusses the relation between non-separability and holism in chapter 8 of Esfeld (2001).)

Lyre (2004) and Healey (2004) see electromagnetism and other gauge theories as manifesting nonseparability for reasons different from those arising from quantum entanglement (cf. The Aharonov-Bohm Effect). Lyre takes this to be a variant of spatiotemporal holism, and connects it to structural realism. Healey (2007) argues that general relativity does not manifest this kind of nonseparability even though it may be formulated as a gauge theory. Weatherall (2016) argues that a distinction exists, but it is not enough to rule out spatiotemporal holism in general relativity. If there are more than one spatial dimensions, an analogue of the Aharonov-Bohm effect in general relativity (using the directions of parallel-propagated vectors) theoretically exhibits a similar type of nonseparability as that observed in gauge theory.

12. Quantum Field Theory

Certain phenomena that arise within quantum field theory have been taken to challenge principles of separability or to involve holism. These have been analyzed most intensively by mathematical physicists and philosophers taking an algebraic approach to quantum theory, even though many empirical successes of quantum field theory have been achieved by following other approaches.

Algebraic quantum field theory (AQFT) represents the state in a region of spacetime by means of a function from an algebra of associated “field” or “observable” operators: the value of this function for a self-adjoint operator represents the expected result of a measurement of the corresponding observable on that region. A state is said to be decomposable (some say separable) across algebras \(R_{A}, R_{B}\) associated with regions \(A, B\) if its restriction \(\omega\) to the algebra \(R_{AB}\) generated by \(R_{A}, R_{B}\) is a product state—i.e. satisfies \(\omega(XY)=\omega(X)\omega(Y)\), for all \(X\in R_{A}, Y\in R_{B}\); or if \(\omega\) is a limit of convex combinations of product states: otherwise, it is said to be entangled across \(R_{AB}\) (see e.g. Valente 2010, pp. 1031–2). This is a natural reformulation of a generalization to mixed states of the first condition for entanglement given in section 8.

Entanglement is endemic in AQFT. Summers and Werner (1985) proved that the vacuum state of a quantum field is not only entangled across algebras associated with certain spacelike separated regions of Minkowski spacetime, but that it also maximally violates Bell inequalities for algebras associated with these regions. They also proved (1988) that every state on a pair of space-like separated open regions whose closures share a single point is maximally entangled across their algebras. For each state, the degree of entanglement decreases rapidly with spatial separation. But if and only if \(R_{A}, R_{B}\) possess what is called the split property is any state decomposable across these algebras.

The split property (Valente 2010, p. 1035) is a strengthening of the condition of microcausality (observables on space-like separated regions commute). Summers (2009) argues that it is meaningful to speak of independent subsystems in relativistic quantum theory if they can be localized in spacetime regions \(A, B\) whose algebras \(R_{A}, R_{B}\) posses the split property; and that most, if not all, physically relevant models of quantum field theories have this property (for sufficiently space-like separated regions \(A, B)\).

The split property is a kind of independence condition. Rédei (2010) argues that, by conforming to this and other independence conditions, an AQFT can meet all the requirements Einstein (1948) considered necessary for a quantum theory satisfactorily to realize the field-theoretic ideal. These were the requirement that physical things be arranged in a space-time continuum (Spatiotemporality); that things located in space-like separated regions have their own distinct states (Independence); and that if \(a, b\) are located in space-like separated regions \(A, B\) respectively, then an external influence on a has no immediate effect on b (Local Action). (The first two names are Rédei’s: the last is Einstein’s.) Rédei takes AQFT to satisfy Spatiotemporality because of its basic assumption that observables are localized in space-time regions; that an AQFT’s satisfaction of the split property and other members of a hierarchy of independence conditions establishes Independence; and that an AQFT obeys Local Action insofar as it meets a condition he calls operational separability.

In evaluating Rédei’s argument it is important to ask what counts as a physical thing. Einstein mentioned two possible candidates: bodies and fields. Howard’s separability principle permits a natural transposition of Einstein’s real state separability principle to field theory. Entangled states in AQFT violate section 5’s state separability principle just as they do in nonrelativistic quantum mechanics even though the split property and related independence conditions on their algebras hold. So if the content of a space-time region were specified by its algebra in AQFT, considered as a physical system with real physical state given by a state on that algebra, then Howard’s separability principle would fail. (Although the failure of the split property or other algebraic independence conditions for certain regions in a quantum field theory would represent a more radical threat to the separate existence of such physical systems in those regions than mere entanglement). But it is doubtful that Einstein would have counted observables or their algebras as physical things. If instead these are taken to represent magnitudes of physical fields or the spatio-temporal region on which they are defined then meeting Rédei’s Independence requirement is still consistent with failure of Howard’s (stronger) separability principle. Finally meeting Rédei’s operational separability condition only for non-selective operations would not suffice to ensure conformity to Local Action. Einstein’s reasons for rejecting the completeness of quantum mechanical description are naturally extended to AQFT: if a state on its local algebra completely specifies the real state of a space-time region then either the natural extension of his real state separability principle or his principle of Local Action fails.

Metaphysical holism presupposes a division of a whole into parts. To apply the part/whole distinction here one must address the ontology of quantum field theory. Taking spacetime regions to be the relevant physical objects, one could understand the system/subsystem and part/whole relations in terms of spatiotemporal inclusion. To assess physical property holism or nonseparability we need to determine the qualitative intrinsic properties and relations pertaining to spacetime regions in quantum field theory.

Arageorgis (2013) gives an example of quantum field states entangled across two regions which nevertheless, he argues, fail to exhibit the same kind of state nonseparability as singlet and triplet spin states of a pair of quantum particles (see Maudlin 1998). But he suggests that his example does exhibit a kind of epistemological state nonseparability, in so far as an agent confined to a single region cannot determine its state by operations confined to that region. By applying the eigenvalue-eigenstate link to his example, Arageorgis (2013) argues that the energy of a particular compound quantum field system is not determined by the energies (or any other qualitative intrinsic properties and relations) of its component subsystems. He concludes that this example manifests physical property holism.

Wayne (2002) has suggested that quantum field theory is best interpreted as postulating extensive holism or nonseparability. On this interpretation, the fundamental quantities in quantum field theory are vacuum expectation values of products of field operators defined at various spacetime points. The field can be reconstructed out of all of these. Nonseparability supposedly arises because the vacuum expectation value of a product of field operators defined at an n-tuple of distinct spacetime points does not supervene on qualitative intrinsic physical properties defined at those n points, together with the spatiotemporal relations among the points. But it is not clear that vacuum expectation values of products of field operators defined at n-tuples of distinct spacetime points represent either qualitative intrinsic physical properties of these n-tuples or physical relations between them. Improved assessment of the extent to which quantum field theory illustrates holism or nonseparability must await further progress in the interpretation of quantum field theory. (Kuhlman, Lyre and Wayne (2002) represents a relevant first step: but see also Fraser (2008), Baker (2009).)

13. String Theory

String theory (or its descendant, M-theory) has emerged as a speculative candidate for unifying much of fundamental physics, including quantum mechanics and general relativity. Existing string theories proceed by quantizing classical theories of basic entities that are extended in one or more dimensions of a space that has 6 or 7 tiny compact dimensions in addition to the three spatial dimensions of ordinary geometry. If these additional dimensions are appropriately considered spatial, then it is natural to extend the concepts of spatial and spatiotemporal separability to encompass them. In that case, processes involving classical strings (or p-branes with \(p \gt 0\)) would count as (spatiotemporally) nonseparable, even though all particles and their properties conform to spatial separability.

The status of nonseparability within a quantized string field theory is not so easy to assess, because of the general problems associated with deciding what the ontology of any relativistic quantum field theory should be taken to be.


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