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		<summary type="html">&lt;p&gt;Repair Quantum Collection B backlink template&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Quantum book backlink|Quantum information and computing}}&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Quantum entanglement&amp;#039;&amp;#039;&amp;#039; is a phenomenon in which the state of a composite quantum system cannot be expressed as a product of the states of its individual subsystems. It is one of the central features distinguishing quantum from classical physics.&amp;lt;ref&amp;gt;{{cite journal&lt;br /&gt;
| last1 = Horodecki&lt;br /&gt;
| first1 = Ryszard&lt;br /&gt;
| last2 = Horodecki&lt;br /&gt;
| first2 = Paweł&lt;br /&gt;
| last3 = Horodecki&lt;br /&gt;
| first3 = Michał&lt;br /&gt;
| last4 = Horodecki&lt;br /&gt;
| first4 = Karol&lt;br /&gt;
| title = Quantum entanglement&lt;br /&gt;
| journal = Reviews of Modern Physics&lt;br /&gt;
| volume = 81&lt;br /&gt;
| issue = 2&lt;br /&gt;
| pages = 865–942&lt;br /&gt;
| year = 2009&lt;br /&gt;
| doi = 10.1103/RevModPhys.81.865&lt;br /&gt;
| arxiv = quant-ph/0702225&lt;br /&gt;
| bibcode = 2009RvMP...81..865H&lt;br /&gt;
| s2cid = 59577352&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;NielsenChuang2010&amp;quot;&amp;gt;{{cite book |last1=Nielsen |first1=Michael A. |last2=Chuang |first2=Isaac L. |title=Quantum Computation and Quantum Information |publisher=Cambridge University Press |year=2010}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Quantum_entanglement.jpg|thumb|400px|Entangled quantum states exhibit correlations that cannot be described by independent subsystems.]]&lt;br /&gt;
&lt;br /&gt;
== Definition ==&lt;br /&gt;
Consider a bipartite system with subsystems A and B. A pure state is called &amp;#039;&amp;#039;&amp;#039;separable&amp;#039;&amp;#039;&amp;#039; if it can be written as&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\psi\rangle = |\psi_A\rangle \otimes |\psi_B\rangle.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If no such decomposition exists, the state is said to be &amp;#039;&amp;#039;&amp;#039;entangled&amp;#039;&amp;#039;&amp;#039;.&amp;lt;ref name=&amp;quot;NielsenChuang2010&amp;quot; /&amp;gt;&amp;lt;ref&amp;gt;{{cite book&lt;br /&gt;
| last1 = Nielsen&lt;br /&gt;
| first1 = Michael A.&lt;br /&gt;
| last2 = Chuang&lt;br /&gt;
| first2 = Isaac L.&lt;br /&gt;
| title = Quantum Computation and Quantum Information&lt;br /&gt;
| edition = 10th anniversary&lt;br /&gt;
| publisher = Cambridge University Press&lt;br /&gt;
| location = Cambridge&lt;br /&gt;
| year = 2010&lt;br /&gt;
| isbn = 978-0-521-63503-5&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Bell states ==&lt;br /&gt;
&lt;br /&gt;
The simplest examples of entangled states are the &amp;#039;&amp;#039;&amp;#039;Bell states&amp;#039;&amp;#039;&amp;#039;:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\Phi^+\rangle = \frac{1}{\sqrt{2}}(|00\rangle + |11\rangle),&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\Phi^-\rangle = \frac{1}{\sqrt{2}}(|00\rangle - |11\rangle),&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\Psi^+\rangle = \frac{1}{\sqrt{2}}(|01\rangle + |10\rangle),&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\Psi^-\rangle = \frac{1}{\sqrt{2}}(|01\rangle - |10\rangle).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
These states exhibit maximal entanglement and perfect correlations between measurement outcomes.&lt;br /&gt;
&lt;br /&gt;
== Measurement correlations ==&lt;br /&gt;
&lt;br /&gt;
In an entangled state, measurement outcomes on one subsystem are correlated with outcomes on the other subsystem.&lt;br /&gt;
&lt;br /&gt;
For example, in the state &amp;lt;math&amp;gt;|\Phi^+\rangle&amp;lt;/math&amp;gt;, measuring one qubit determines the outcome probabilities of the other, regardless of spatial separation.&lt;br /&gt;
&lt;br /&gt;
These correlations cannot be explained by classical local hidden-variable theories.&amp;lt;ref&amp;gt;{{cite book |last=Bell |first=John S. |title=Speakable and Unspeakable in Quantum Mechanics |publisher=Cambridge University Press |year=1987}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reduced states ==&lt;br /&gt;
&lt;br /&gt;
Even if a composite system is in a pure state, its subsystems may be described by mixed states.&lt;br /&gt;
&lt;br /&gt;
The reduced density matrix of subsystem A is given by&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho_A = \mathrm{Tr}_B(\rho_{AB}),&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathrm{Tr}_B&amp;lt;/math&amp;gt; denotes the partial trace over subsystem B.&lt;br /&gt;
&lt;br /&gt;
This reflects the fact that subsystems of entangled systems do not possess independent pure states.&lt;br /&gt;
&lt;br /&gt;
== Entanglement as a resource ==&lt;br /&gt;
&lt;br /&gt;
Entanglement is a key resource in quantum information processing. It enables:&lt;br /&gt;
&lt;br /&gt;
* quantum teleportation &amp;lt;ref&amp;gt;{{cite web&lt;br /&gt;
| last = Francis&lt;br /&gt;
| first = Matthew&lt;br /&gt;
| title = Quantum entanglement shows that reality can&amp;#039;t be local&lt;br /&gt;
| website = Ars Technica&lt;br /&gt;
| date = 30 October 2012&lt;br /&gt;
| url = https://arstechnica.com/science/2012/10/quantum-entanglement-shows-that-reality-cant-be-local/&lt;br /&gt;
| access-date = 22 August 2023&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
* superdense coding  &lt;br /&gt;
* quantum cryptography  &lt;br /&gt;
* quantum computation beyond classical limits  &lt;br /&gt;
&lt;br /&gt;
== Generation of entanglement ==&lt;br /&gt;
&lt;br /&gt;
Entanglement is typically created by applying quantum operations to multiple qubits.&lt;br /&gt;
&lt;br /&gt;
For example, applying a Hadamard gate followed by a controlled-NOT (CNOT) gate to an initial state&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|0\rangle \otimes |0\rangle&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
produces the Bell state&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\frac{1}{\sqrt{2}}(|00\rangle + |11\rangle).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Physical significance ==&lt;br /&gt;
&lt;br /&gt;
Quantum entanglement:&lt;br /&gt;
&lt;br /&gt;
* is a fundamental feature of composite quantum systems  &lt;br /&gt;
* produces correlations beyond classical physics  &lt;br /&gt;
* underlies many quantum technologies and protocols&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;
&lt;br /&gt;
{{Sourceattribution|Quantum entanglement|1}}&lt;/div&gt;</summary>
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