As someone coming from a materials science and engineering background, I've always approached quantum mechanics with a pragmatic mindset: it's a tool to make useful predictions. My guess is most in applied disciplines have a smiliar perspective. But sometimes I find myself asking detailed questions on the language used to describe the theory itself. I mean what does non-local actually refer to? When you try to find out just plain boring explanations I think your meet with assumptions that both reader and author are on the same standing about the meaning of words. This poor assumption is where I think, or at least I found for me, the confusion surrounding QM stems from sloppy language and mismatched conceptual frameworks, particularly around the nature of the quantum state space (i.e., wave function) and the term non-locality. I'm going to write about how I've come to understand the perspectives on the foundations of quantum mechanics.
Quantum State/Wave Function
I will use the quantum state and wave function interchangeably, but this is ironic because I've just lambasted about the lack of clarity in the language used to describe QM. The specifics are the quantum state is a complex-valued vector in a Hilbert space, while the wave function is the projection2 of this quantum state onto a physical space(i.e., our 3D space and 1D time) basis of position eigenstates.
The Core Question: What Is the Quantum State?
At the heart of QM is the quantum state/wave function ($\Psi$), a complex-valued mathematical or physical object, depending on your view, that is used to compute probabilities of outcomes of observables, thats really all its utility! The fundamental nature of the quantum state is where things become difficult to wrap your head around (for a review see [2]). The nature of the quantum state, $\Psi$ has two "beliefs"1, which are:
- It is an ontological object, meaning it is something real, part of the physical world we observe and exist in.
- Or it is an epistemological object meaning it is a representation of our knowledge or information about the world that we inhabit.
The view one takes fundamentally determines how one interprets the foundations of quantum behavior: entanglement and "non-local" (more on this next) correlations. But from a "shut-up and calculate" [1] perspective, it doesn't matter.
Non-Locality
In QM, the word "non-locality" is thrown around often, but it's crucial to disentangle (😆) its usage in physical reality versus mathematical contexts. Non-locality is an underpinning concept of the mathematical formalism of QM; it refers to a property of a mathematical space (not our physical space and time) that has a structure allowing for correlations (i.e., entanglement) which appear coordinated over spatial separations without a direct mediating causal signal limited by the speed of light. This 'acausal' nature of correlations in the mathematical formalism is distinct from, and does not enable violation of the principles of causality in physical spacetime as described by special relativity. How can this be? What such space has that feature? Turns out in information theory, the space of all possible distributions of probability over a finite set of outcomes has such a property.
Digression: Bell's Theorem
Bell's theorem shows that no theory of local hidden3 variables can reproduce all the predictions of QM [3]. John S. Bell formulated this as an mathematical inequality, which if violated, rules out the possibility of combining locality AND hidden variables.
So far all experiments have verified violation of Bell's inequality, and thus we can have a local theory with hidden variables or a non-local theory without hidden variables. The former (i.e., local hidden variables) is not consistent with any observations and thus is not considered a valid theory. This means we must give up either locality or hidden variables (or both). Various interpretations of QM make different choices: Copenhagen and QBism interpretations maintain locality by giving up hidden variables, while Bohmian mechanics maintains hidden variables by embracing non-locality. The theorem doesn't force us to conclude QM is inherently non-local, its more that it depends on your interpretational framework.
Physical Space (Spacetime)
In physical spacetime, which has a continuous geometric structure defined by coordinates, metrics, and causality, locality is built-in. Things happen through the continuity of the space and time. Events occur at points in space and time. Forces and interactions are local as they propagate through space over time and cannot influence distant points instantaneously without violating causality. Putting it more basic, point A cannot go to point B without going through the points in between.
This geometric structure ensures that:
- Causality is respected.
- Influence is constrained by light cones.
- Distances and continuity matter.
Hilbert Space (Quantum State Space)
In contrast, the quantum state lives in Hilbert space, which is a mathematical geometric space, again its mathematical not the physical space that we are familiar with. It has a structure:
- Inner product
- Norms
- Angles
This allows for some very important and convenient mathematical results. But again, it is not directly apart (embedded?) of spacetime, and therefore:
- Does not need to have spatial locality, i.e., the distance between two points can be disjointed in this space.
- Does not need to obey causal propagation in this geometric space.
- Can encode non-local correlations purely as part of its informational structure
I think this is a big reason people often get confused. More over we are usually taught from the position basis projection2 perspective of the quantum state onto physical space so it makes this decoupling something we have to backtrack on to understand. Physics PhDs and mathmeticians probably have no issues here, but others I think might (I know I did!). The key point is Hilbert space is geometric, but not physically local in our familiar spacetime. The language used in our courses/textbooks tends to blend physical and mathematical notions carelessly.
Two Views of the Quantum State
Ontological Interpretation
If you treat the Quantum State as a real object in the physical world, then you're saying there exists an object -- the quantum state -- that is part of everything. This assumption then leads to:
- The Quantum State can be non-local in that it encodes information (i.e., entanglement), even if in a projected position-basis that information is spatially separated systems.
- It evolves unitarily even across space-like separations.
- Measurement collapse (i.e., observables/observational outcomes) is a physical process, albeit a non-unitary one.
This leads to ideas like Many-Worlds and Bohmian mechanics [4]. It demands that we expand our notion of physical reality beyond just local spacetime. Space and time are still very much local, but the quantum state is not.
Epistemological Interpretation
If one views the quantum state as just a tool that encodes information (as in Copenhagen or QBism [5]), then it's not a real object. It reflects an observer's state of belief about outcomes.
- Measurement collapse isn't physical, it's a Bayesian update (i.e., we got more info from observing).
- Entanglement reflects only non-local information, not non-local causes.
- No signal travels faster than light—only correlated expectations are updated.
This is why the quantum state can have non-local structure without violating causality. It's not describing the world directly as it is but describing what we know (or can infer) about it.
In this view, quantum mechanics becomes an information theory, with the quantum state as a formal device for encoding and updating expectations.
- This "information" doesn't have to live in physical space.
- It can exist in mathematical abstract spaces (e.g., Hilbert space), where correlations span across what would be distant points in spacetime.
- There's no requirement for continuity, geometry, or causality in this mathematical space.
This aligns with modern perspectives from quantum information theory, where entanglement is a resource, and non-locality is an informational, not physical, phenomenon.
Thoughts on how to communicate this
First, its okay to be verbose and expressive when explaining. We can say things like:
- Our reality of physical geometry means space and time is always local because it is continuous, if we say otherwise then causality is violated and we've got a problem because we don't observe this nor does general relativity tell us this!
- Mathematical geometries which refers to abstract concepts like Hilbert space have a structure that has similar properties of physical geometry (i.e., a metric4), but does not have to maintain locality. Things can be far apart in this geometric space and still be connected by the metric (i.e., entanglement).
Making these distinctions should help fade the confusion with these conceptual aspects. I could be wrong, but I think it helps.
The quantum state, depending on your interpretation, is either a very weird, non-local physical object or an informational object living in a non-local, non-physical space. Either way, the math is consistent and making predictions occurs without conflict. The confusion is in the language we use to describe such perspectives, well at least its confusing for me.
Footnotes
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Yes, seems like a strange word to use, surely I can't mean ones evidence lacking perspective and feelings about something. But this is exactly what I mean. I think whether you view the quantum state as an ontological or epistemological object is a question of your prior. ↩
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Hilbert space states can be projected onto physical space through a choice of basis—commonly the position basis $( |x\rangle )$. The Hamiltonian operator, which encodes dynamics and interactions, is expressed in this basis to produce differential equations in space and time (e.g., the Schrödinger equation). This projection allows abstract quantum states to manifest as real-space amplitudes and enables direct modeling of physical interactions in quantum field theory and many-body systems. ↩↩
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A metric is a function that defines the distance between any two points in a space. Its a "ruler" that can be adjusted to work correctly in the space of interest. ↩
References
[1] N.D. Mermin, Could Feynman Have Said This?, Physics Today 57 (2004) 10–11. https://doi.org/10.1063/1.1768652.
[2] Leifer, M. S. (2014). Is the quantum state real? An extended review of $\psi$-ontology theorems. Quanta, 3(1), 67-155. https://doi.org/10.12743/quanta.v3i1.22.
[3] Brunner, N., Cavalcanti, D., Pironio, S., Scarani, V., & Wehner, S. (2014). Bell nonlocality. Reviews of Modern Physics, 86(2), 419–478. https://doi.org/10.1103/RevModPhys.86.419.
[4] Maudlin, T. (2011). Quantum Non-Locality and Relativity: Metaphysical Intimations of Modern Physics (3rd ed.). Wiley-Blackwell. URL.
[5] Fuchs, C. A., Mermin, N. D., & Schack, R. (2014). An introduction to QBism with an application to the locality of quantum mechanics. American Journal of Physics, 82(8), 749-754. https://doi.org/10.1119/1.4874855.