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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Fundamental theorem demonstrating incompatibility of quantum mechanics with local hidden-variable theories}}&lt;br /&gt;
&lt;br /&gt;
{{Quantum book backlink|Conceptual and interpretations}}&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Bell&amp;#039;s theorem&amp;#039;&amp;#039;&amp;#039; is a foundational result in [[Physics:Quantum mechanics|quantum mechanics]] demonstrating that no theory based on [[Local hidden-variable theory|local hidden variables]] can reproduce all predictions of quantum physics. It establishes that quantum correlations arising from [[Physics:Quantum entanglement|entanglement]] are fundamentally incompatible with the classical assumptions of locality and realism.&amp;lt;ref name=&amp;quot;Bell1964&amp;quot;&amp;gt;{{cite journal |last=Bell |first=J. S. |title=On the Einstein Podolsky Rosen paradox |journal=Physics Physique Физика |volume=1 |issue=3 |pages=195–200 |year=1964 |doi=10.1103/PhysicsPhysiqueFizika.1.195}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Mermin1993&amp;quot;&amp;gt;{{cite journal |last=Mermin |first=N. David |title=Hidden variables and the two theorems of John Bell |journal=Reviews of Modern Physics |volume=65 |issue=3 |pages=803–815 |year=1993 |doi=10.1103/RevModPhys.65.803}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In essence, Bell showed that:&lt;br /&gt;
&lt;br /&gt;
→ If a theory is local, it cannot agree with quantum mechanics  &lt;br /&gt;
→ If it agrees with quantum mechanics, it must be nonlocal  &lt;br /&gt;
[[File:Bell_theorem_entanglement.jpg|thumb|400px|Illustration of Bell’s theorem: measurements on entangled particles exhibit correlations that violate classical (local realistic) expectations.]]&lt;br /&gt;
&lt;br /&gt;
== Conceptual background ==&lt;br /&gt;
&lt;br /&gt;
Bell’s theorem builds on the [[Physics:EPR paradox|Einstein–Podolsky–Rosen (EPR) paradox]], which questioned whether quantum mechanics provides a complete description of reality.&amp;lt;ref name=&amp;quot;EPR1935&amp;quot;&amp;gt;{{cite journal |last1=Einstein |first1=A. |last2=Podolsky |first2=B. |last3=Rosen |first3=N. |title=Can quantum-mechanical description of physical reality be considered complete? |journal=Physical Review |volume=47 |issue=10 |pages=777–780 |year=1935 |doi=10.1103/PhysRev.47.777}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
EPR considered pairs of particles in an entangled state:&lt;br /&gt;
&lt;br /&gt;
* Measuring one particle instantaneously determines the state of the other  &lt;br /&gt;
* Even when separated by large distances  &lt;br /&gt;
&lt;br /&gt;
This suggests either:&lt;br /&gt;
&lt;br /&gt;
* Faster-than-light influence (violating locality), or  &lt;br /&gt;
* Pre-existing hidden variables determining outcomes  &lt;br /&gt;
&lt;br /&gt;
Bell formalized this dilemma mathematically.&lt;br /&gt;
&lt;br /&gt;
== Bell inequalities ==&lt;br /&gt;
&lt;br /&gt;
Bell derived inequalities that any local hidden-variable theory must satisfy. The most widely used version is the **CHSH inequality**, which constrains correlations between measurements:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\langle A_0 B_0 \rangle + \langle A_0 B_1 \rangle + \langle A_1 B_0 \rangle - \langle A_1 B_1 \rangle| \leq 2&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This inequality relies on two key assumptions:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Locality&amp;#039;&amp;#039;&amp;#039;: no influence propagates faster than light  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Realism&amp;#039;&amp;#039;&amp;#039;: physical properties exist prior to measurement  &lt;br /&gt;
&lt;br /&gt;
Quantum mechanics predicts violations of this bound.&lt;br /&gt;
&lt;br /&gt;
== Quantum violation ==&lt;br /&gt;
&lt;br /&gt;
For entangled states, quantum mechanics predicts stronger correlations. For example, using a maximally entangled Bell state:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\psi\rangle = \frac{|0\rangle|1\rangle - |1\rangle|0\rangle}{\sqrt{2}}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
the CHSH expression reaches:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
2\sqrt{2}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This exceeds the classical limit of 2 and is known as the &amp;#039;&amp;#039;&amp;#039;Tsirelson bound&amp;#039;&amp;#039;&amp;#039;.&amp;lt;ref&amp;gt;{{cite book |last=Rau |first=Jochen |title=Quantum Theory: An Information Processing Approach |publisher=Oxford University Press |year=2021}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus:&lt;br /&gt;
&lt;br /&gt;
→ Quantum correlations violate Bell inequalities  &lt;br /&gt;
→ Local hidden-variable theories cannot reproduce these results  &lt;br /&gt;
&lt;br /&gt;
== Experimental tests ==&lt;br /&gt;
&lt;br /&gt;
[[Physics:Bell test|Bell tests]] experimentally measure correlations between entangled particles.&lt;br /&gt;
&lt;br /&gt;
Key milestones include:&lt;br /&gt;
&lt;br /&gt;
* 1972 – First experimental test (Clauser &amp;amp; Freedman)  &lt;br /&gt;
* 1982 – Aspect experiments improving locality conditions  &lt;br /&gt;
* 2015 – Loophole-free Bell tests  &lt;br /&gt;
&lt;br /&gt;
All experiments consistently confirm:&lt;br /&gt;
&lt;br /&gt;
* Violation of Bell inequalities  &lt;br /&gt;
* Agreement with quantum mechanics  &lt;br /&gt;
&lt;br /&gt;
These results rule out local hidden-variable theories.&amp;lt;ref name=&amp;quot;Hensen2015&amp;quot;&amp;gt;{{cite journal |last=Hensen |first=B. |title=Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometres |journal=Nature |volume=526 |pages=682–686 |year=2015 |doi=10.1038/nature15759}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Conceptual implications ==&lt;br /&gt;
&lt;br /&gt;
Bell’s theorem has profound implications:&lt;br /&gt;
&lt;br /&gt;
* Nature is not both local and realistic  &lt;br /&gt;
* Quantum entanglement implies non-classical correlations  &lt;br /&gt;
* Classical intuitions about separability fail  &lt;br /&gt;
&lt;br /&gt;
It does &amp;#039;&amp;#039;&amp;#039;not&amp;#039;&amp;#039;&amp;#039; specify which assumption must be abandoned, leading to multiple interpretations.&lt;br /&gt;
&lt;br /&gt;
== Relation to other no-go theorems ==&lt;br /&gt;
&lt;br /&gt;
Bell’s theorem is part of a broader class of results limiting classical interpretations:&lt;br /&gt;
&lt;br /&gt;
* [[Kochen–Specker theorem]] → rules out non-contextual hidden variables  &lt;br /&gt;
* [[Physics:Quantum contextuality|Quantum contextuality]] → measurement outcomes depend on context  &lt;br /&gt;
* [[Physics:Free will theorem|Free will theorem]] → constraints on determinism and locality  &lt;br /&gt;
&lt;br /&gt;
== Interpretational perspectives ==&lt;br /&gt;
&lt;br /&gt;
Different interpretations resolve Bell violations differently:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Copenhagen&amp;#039;&amp;#039;&amp;#039;: abandons realism or counterfactual definiteness  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Many-worlds&amp;#039;&amp;#039;&amp;#039;: retains locality but allows multiple outcomes  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Bohmian mechanics&amp;#039;&amp;#039;&amp;#039;: retains realism but introduces nonlocality  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Objective collapse&amp;#039;&amp;#039;&amp;#039;: modifies quantum dynamics  &lt;br /&gt;
&lt;br /&gt;
No consensus exists on the “correct” interpretation.&lt;br /&gt;
&lt;br /&gt;
== Physical significance ==&lt;br /&gt;
&lt;br /&gt;
Bell’s theorem demonstrates that:&lt;br /&gt;
&lt;br /&gt;
→ Quantum mechanics is fundamentally incompatible with classical worldviews  &lt;br /&gt;
&lt;br /&gt;
It underpins modern developments such as:&lt;br /&gt;
&lt;br /&gt;
* [[Physics:Quantum information theory|Quantum information]]  &lt;br /&gt;
* [[Physics:Quantum cryptography|Quantum cryptography]]  &lt;br /&gt;
* [[Physics:Quantum computing|Quantum computing]]  &lt;br /&gt;
&lt;br /&gt;
and is one of the most experimentally tested principles in physics.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
&lt;br /&gt;
{{Author|Harold Foppele}}&lt;br /&gt;
{{Sourceattribution|Physics:Quantum Bell&amp;#039;s theorem|1}}&lt;/div&gt;</summary>
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