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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Quantum book backlink|Open quantum systems}}&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Quantum decoherence&amp;#039;&amp;#039;&amp;#039; is the process by which a quantum system loses its ability to exhibit coherent superposition due to interaction with its environment. It explains how classical behavior emerges from quantum systems without invoking wavefunction collapse.&amp;lt;ref name=&amp;quot;Zurek2003&amp;quot;&amp;gt;{{cite book &lt;br /&gt;
|last=Zurek &lt;br /&gt;
|first=Wojciech H. &lt;br /&gt;
|title=Decoherence and the Transition from Quantum to Classical &lt;br /&gt;
|publisher=Springer &lt;br /&gt;
|year=2003&lt;br /&gt;
|url=https://link.springer.com/chapter/10.1007/978-3-540-35775-9_1&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;MIT_OCW&amp;quot;&amp;gt;{{cite web |url=https://ocw.mit.edu/courses/22-51-quantum-theory-of-radiation-interactions-fall-2012/resources/mit22_51f12_ch8/ |title=22.51 Course Notes, Chapter 8: Open Quantum Systems |website=MIT OpenCourseWare |access-date=2026-04-12}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
Decoherence plays a central role in quantum measurement, quantum information, and the quantum-to-classical transition.&lt;br /&gt;
&lt;br /&gt;
[[File:Quantum_decoherence.svg|thumb|400px|Decoherence describes the loss of quantum coherence due to interaction with the environment, leading to the emergence of classical behavior.]]&lt;br /&gt;
&lt;br /&gt;
=Quantum Decoherence=&lt;br /&gt;
== Basic mechanism ==&lt;br /&gt;
&lt;br /&gt;
In quantum mechanics, a system may exist in a superposition of states:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\psi\rangle = \alpha |0\rangle + \beta |1\rangle.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The corresponding density matrix is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho =&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
|\alpha|^2 &amp;amp; \alpha \beta^* \\&lt;br /&gt;
\alpha^* \beta &amp;amp; |\beta|^2&lt;br /&gt;
\end{pmatrix}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The off-diagonal elements represent quantum coherence.&lt;br /&gt;
&lt;br /&gt;
=== Interaction with environment ===&lt;br /&gt;
&lt;br /&gt;
When the system interacts with an environment, it becomes entangled with environmental degrees of freedom:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\psi\rangle \otimes |E_0\rangle&lt;br /&gt;
\rightarrow&lt;br /&gt;
\alpha |0\rangle \otimes |E_0&amp;#039;\rangle&lt;br /&gt;
+&lt;br /&gt;
\beta |1\rangle \otimes |E_1&amp;#039;\rangle.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Tracing out the environment yields a reduced density matrix:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho \rightarrow&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
|\alpha|^2 &amp;amp; \alpha \beta^* \langle E_1&amp;#039;|E_0&amp;#039;\rangle \\&lt;br /&gt;
\alpha^* \beta \langle E_0&amp;#039;|E_1&amp;#039;\rangle &amp;amp; |\beta|^2&lt;br /&gt;
\end{pmatrix}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the environment states become orthogonal, the coherence terms vanish.&lt;br /&gt;
&lt;br /&gt;
=== Loss of coherence ===&lt;br /&gt;
&lt;br /&gt;
In the limit&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\langle E_0&amp;#039;|E_1&amp;#039;\rangle \rightarrow 0,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
the density matrix becomes diagonal:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho \rightarrow&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
|\alpha|^2 &amp;amp; 0 \\&lt;br /&gt;
0 &amp;amp; |\beta|^2&lt;br /&gt;
\end{pmatrix}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This corresponds to a classical statistical mixture.&amp;lt;ref name=&amp;quot;Zurek2003&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Decoherence in master equations ==&lt;br /&gt;
&lt;br /&gt;
Decoherence is naturally described within the framework of quantum master equations.&lt;br /&gt;
&lt;br /&gt;
=== Lindblad description ===&lt;br /&gt;
&lt;br /&gt;
In the Lindblad equation, decoherence arises from dissipative terms:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\frac{d\rho}{dt}&lt;br /&gt;
=&lt;br /&gt;
-\frac{i}{\hbar}[\hat{H},\rho]&lt;br /&gt;
+&lt;br /&gt;
\sum_k&lt;br /&gt;
\left(&lt;br /&gt;
L_k \rho L_k^\dagger&lt;br /&gt;
-\frac{1}{2}\{L_k^\dagger L_k,\rho\}&lt;br /&gt;
\right).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Certain Lindblad operators suppress off-diagonal elements of &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=== Pure dephasing ===&lt;br /&gt;
&lt;br /&gt;
A simple model of decoherence is pure dephasing:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
L = \sqrt{\gamma_\phi}\,\sigma_z.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This leaves populations unchanged but causes exponential decay of coherence:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho_{01}(t) = \rho_{01}(0) e^{-\gamma_\phi t}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Pointer states ==&lt;br /&gt;
&lt;br /&gt;
Decoherence does not affect all states equally. Certain states remain stable under environmental interaction.&lt;br /&gt;
&lt;br /&gt;
=== Definition ===&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Pointer states&amp;#039;&amp;#039;&amp;#039; are the states that remain robust under decoherence. They are selected by the system–environment interaction.&amp;lt;ref name=&amp;quot;Zurek2003&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Environment-induced superselection ===&lt;br /&gt;
&lt;br /&gt;
The process by which pointer states emerge is called &amp;#039;&amp;#039;&amp;#039;einselection&amp;#039;&amp;#039;&amp;#039; (environment-induced superselection).&lt;br /&gt;
&lt;br /&gt;
These states form a preferred basis in which the density matrix becomes diagonal.&lt;br /&gt;
&lt;br /&gt;
== Decoherence timescales ==&lt;br /&gt;
&lt;br /&gt;
Decoherence typically occurs extremely rapidly compared to other dynamical processes.&lt;br /&gt;
&lt;br /&gt;
=== Decoherence time ===&lt;br /&gt;
&lt;br /&gt;
The decoherence time &amp;lt;math&amp;gt;\tau_D&amp;lt;/math&amp;gt; characterizes the decay of coherence:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho_{ij}(t) \sim e^{-t/\tau_D}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For macroscopic systems, &amp;lt;math&amp;gt;\tau_D&amp;lt;/math&amp;gt; is often extremely short.&lt;br /&gt;
&lt;br /&gt;
=== Comparison with relaxation ===&lt;br /&gt;
&lt;br /&gt;
* decoherence time: loss of phase coherence  &lt;br /&gt;
* relaxation time: energy dissipation  &lt;br /&gt;
&lt;br /&gt;
Usually:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\tau_D \ll \tau_R.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This explains why classical behavior appears so quickly.&lt;br /&gt;
&lt;br /&gt;
== Role in measurement ==&lt;br /&gt;
&lt;br /&gt;
Decoherence provides a mechanism for the apparent collapse of the wavefunction.&lt;br /&gt;
&lt;br /&gt;
=== Measurement interaction ===&lt;br /&gt;
&lt;br /&gt;
During measurement, the system becomes entangled with a measuring device and environment.&lt;br /&gt;
&lt;br /&gt;
Decoherence suppresses interference between different outcomes, making them effectively classical.&lt;br /&gt;
&lt;br /&gt;
=== Classical outcomes ===&lt;br /&gt;
&lt;br /&gt;
After decoherence, the system behaves as if it were in one of several classical states with certain probabilities.&lt;br /&gt;
&lt;br /&gt;
However, decoherence alone does not select a single outcome; it explains the absence of interference.&amp;lt;ref name=&amp;quot;MIT_OCW&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Applications ==&lt;br /&gt;
&lt;br /&gt;
Decoherence is central to many areas of modern physics.&lt;br /&gt;
&lt;br /&gt;
=== Quantum information ===&lt;br /&gt;
&lt;br /&gt;
It is the main obstacle to building stable quantum computers, as it destroys qubit coherence.&amp;lt;ref name=&amp;quot;QubitReview&amp;quot;&amp;gt;{{cite journal |last=Kjaergaard |first=Morten |last2=Schwartz |first2=Michael E. |last3=Braumüller |first3=Jochen |last4=Krantz |first4=Philip |last5=Wang |first5=J. I.-J. |last6=Gustavsson |first6=Simon |last7=Oliver |first7=William D. |title=Engineering high-coherence superconducting qubits |journal=Nature Reviews Materials |volume=5 |pages=309–324 |year=2020 |url=https://www.nature.com/articles/s41578-021-00370-4 |doi=10.1038/s41578-021-00370-4}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Quantum optics ===&lt;br /&gt;
&lt;br /&gt;
It explains line broadening, photon loss, and coherence decay in optical systems.&lt;br /&gt;
&lt;br /&gt;
=== Foundations of quantum mechanics ===&lt;br /&gt;
&lt;br /&gt;
Decoherence provides a physical explanation for the emergence of classical reality from quantum theory.&lt;br /&gt;
&lt;br /&gt;
== Physical significance ==&lt;br /&gt;
&lt;br /&gt;
Quantum decoherence bridges the gap between microscopic quantum laws and macroscopic classical phenomena. It explains why interference effects are not observed in everyday systems and provides a consistent framework for understanding open quantum systems.&amp;lt;ref name=&amp;quot;Zurek2003&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It is one of the key concepts in modern quantum theory.&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 Decoherence|1}}&lt;/div&gt;</summary>
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