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Quantum mechanics is compatible with quantum no-signalling, but its full correlations are incompatible with Bell local causality under the usual additional assumptions. The answer depends on which locality condition is meant. A local operational prohibition on controllable faster-than-light communication is weaker than a causal explanation of correlations by a complete shared past.

Let $a,b\in \{-1,1\}$ be outcomes, $x,y$ local settings and $\lambda$ a complete relevant past specification. Bell factorization and measurement independence demandNeither assumes deterministic response. Put $A_x(\lambda )={\sum }_{a}ap(a|x,\lambda )$ and similarly $B_y$, so $|A_x|,|B_y|\le 1$. Pointwise,Averaging with the same $\rho$ for all settings gives the CHSH inequality $|E_{00}+E_{01}+E_{10}-E_{11}|\le 2$. For a spin singlet state, $E(\mathbf{a},\mathbf{b})=-\mathbf{a}\cdot \mathbf{b}$. Choose ${\mathbf{a}}_0=\hat{z}$, ${\mathbf{a}}_1=\hat{x}$, ${\mathbf{b}}_0=(\hat{z}+\hat{x})/\sqrt{2}$, ${\mathbf{b}}_1=(\hat{z}-\hat{x})/\sqrt{2}$; the magnitude becomes $2\sqrt{2}$. Thus the assumptions cannot all be maintained.^[ref]

There is nevertheless no signalling contradiction. If a local unread measurement has Kraus operators $M_a$ with ${\sum }_a{M}_a^{†}{M}_a=I$, thenThe equality follows by testing both sides against any distant observable and using cyclicity of the trace. Distant conditional states can differ after selecting $a$, but communicating that selection needs an ordinary message. The microcausality condition in quantum field theory similarly ensures commutation of spacelike-separated local observables; it does not make the vacuum or other entangled quantum states Bell-factorizable.

One can preserve different notions of locality by changing premises. Bohmian mechanics retains unique outcomes but its guidance equation is nonlocal for entangled systems; quantum equilibrium equivariance preserves the equilibrium distribution which masks that dependence from signalling. The many-worlds interpretation can combine local interaction equations with no unique global outcome, but a claim of locality must explain its branch-relative correlations; it has not thereby constructed the above Bell-local single-outcome model. The measurement-independence loophole, including suitable retrocausal or correlated-setting models, drops the shared setting-independent $\rho$ premise. Such models are logical possibilities, not demonstrations that the ordinary locality assumptions survive unchanged.

The justified answer is therefore conditional rather than an unqualified yes or no. Operational locality is retained by the quantum formalism. A theory reproducing all its correlations cannot retain Bell factorization, independent settings and the ordinary joint-outcome framework together. Neither denial of hidden variables nor an appeal to relativity alone removes the probabilistic contradiction.

The Bell theorem gives a powerful conditional constraint, but does not by itself establish the unrestricted philosophical sentence that every interpretation contains a literal instantaneous action between distant objects. One must specify what locality means and which further assumptions are retained. In particular, Bell local causality is stronger than an inability to send a faster-than-light message.

Let $a,b$ be settings in spacelike-separated laboratories, $A,B\in \{-1,1\}$ their recorded outcomes, and $\lambda$ a sufficient specification of relevant prior physical variables. A Bell-local model factorizes asTogether with measurement independence, $\rho (\lambda \mid a,b)=\rho (\lambda )$, this constrains observable correlations. It allows stochastic response functions: predetermination of all outcomes is not a necessary separate assumption in this general formulation. Bell's 1964 paper demonstrates the incompatibility between a local completion and selected quantum correlations; the two-setting inequality below is a standard later form of the argument, not a claim about the exact notation of that paper.^[ref]

For example, write the local conditional mean outcomes as $A(a,\lambda ),B(b,\lambda )\in [-1,1]$. At each $\lambda$,Averaging over the same setting-independent distribution gives the CHSH inequality, $|S|\le 2$. A suitable spin singlet state instead predicts $|S|=2\sqrt{2}$. Consequently no model retaining the stated factorization and independence assumptions can reproduce all those quantum correlations. Merely replacing deterministic hidden variables with local random noise cannot evade the bound.

However, violation of this bound does not entail operational signalling. For an ordinary entangled state, a remote nonselective measurement leaves the local reduced density matrix unchanged. The local experimenter cannot choose the outcome needed to encode a controllable message. Quantum no-signalling and failure of Bell factorization can therefore coexist; confusing them would misstate both the prediction and the theorem.

Interpretations allocate the explanatory burden differently. In Bohmian mechanics, the guiding dynamics of an entangled configuration is explicitly nonlocal, though quantum equilibrium masks controllable signalling. A collapse interpretation must explain the status of correlations and of any proposed nonlocal state change. Everettian accounts retain the entangled global state and multiple relative records; their defenders can deny a fundamental action that selects one distant outcome. That does not produce a factorizing classical common-cause model of the observed correlations. Whether such an account deserves the word local depends on whether locality means local dynamical interactions, separability, or Bell's single-outcome causal factorization.

One can also reject setting independence or change the assumed causal organization, but such proposals must be developed as physical models, not advertised as refutations of the inequality's proof. The warranted conclusion is that the conjunction of Bell locality, independent settings and the relevant outcome framework is incompatible with the quantum correlations. Calling the failure action-at-a-distance is justified only after an interpretation specifies the physical entities, events and causal commitments to which that phrase applies.

For local dichotomic outcomes define $A(a,\lambda ),B(b,\lambda )=\pm 1$ and a setting-independent normalized distribution $\rho (\lambda )$. At each $\lambda$,because exactly one bracket vanishes and the other is $\pm 2$. Integrating and using the triangle inequality yieldsFor stochastic local response functions the same bound follows by replacing outcomes with conditional means in $[-1,1]$, or by including local randomness in $\lambda$. The important locality condition is factorization of joint conditional outcome probabilities, together with independence of the setting distribution and $\lambda$.

The spin singlet instead predicts $E(a,b)=-a\cdot b$. Two orthogonal directions at one wing and directions halfway between them at the other give $|S|=2\sqrt{2}$. Therefore reproducing the quantum predictions requires giving up at least one of the stated premises. In the perfect-anticorrelation version, $B(a,\lambda )=-A(a,\lambda )$ gives Bell's three-setting form $|E(a,b)-E(a,c)|\le 1+E(b,c)$ by the same algebra.

This does not establish that all deterministic or hidden-variable theories are impossible: nonlocal guidance is a counterexample to that reading. Nor does it equate Bell locality with no-signalling; averaging quantum outcomes can preserve setting-independent local marginals despite nonfactorizing correlations. The theorem is significant because it turns a local-completeness dispute into incompatible quantitative correlation bounds, not because it refutes every possible meaning of physical reality.^[ref]

Bell's theorem makes precise an obstruction to reproducing quantum correlations with a local causal completion. Let measurement settings be $a,b$, outcomes $A,B=\pm 1$ and a more complete state $\lambda$. Bell locality factorizes $P(A,B|a,b,\lambda )=P(A|a,\lambda )P(B|b,\lambda )$; setting independence takes the distribution of $\lambda$ to be independent of the freely chosen settings. These assumptions imply a Bell inequality. For example deterministic assignments satisfy $|A(B+B^{\prime })+A^{\prime }(B-B^{\prime })|\le 2$, and averaging gives the CHSH bound $|S|\le 2$. The stochastic version follows by averaging local response probabilities too.

An entangled spin singlet predicts $E(a,b)=-a\cdot b$ and suitable four directions give $|S|=2\sqrt{2}$. Thus the quantum predictions are incompatible with the stated local model, not merely with an unnecessarily specific mechanical hidden-variable proposal. Perfect anticorrelation in the EPR argument had motivated inferring pre-existing properties from remote predictions under locality and a completeness criterion. Bell shows that retaining such a local completion cannot recover the broader quantum correlation pattern.

It would overstate the result to say that it proves the impossibility of every hidden-variable theory. Bohmian mechanics supplies a nonlocal example, and rejecting setting independence or changing the causal model changes the theorem's premises. It would also be wrong to equate Bell locality with operational no-signalling. Quantum outcome probabilities at either wing can remain independent of the distant setting after averaging, even though the joint correlations have no local factorized explanation.

The theorem therefore sharpens the EPR dilemma: one cannot preserve all of the local causal assumptions and the quantum predictions. Empirical Bell violations bear on that conjunction. They do not alone choose one interpretation, make controllable superluminal communication available, or settle every philosophical sense of “realism.”^[ref][ref]