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		<id>https://scholarlywiki.org/index.php?title=Physics:Quantum_Open_systems&amp;diff=155&amp;oldid=prev</id>
		<title>imported&gt;WikiHarold: Repair Quantum Collection B backlink template</title>
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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|Open quantum systems}}&lt;br /&gt;
In quantum mechanics, an &amp;#039;&amp;#039;&amp;#039;open quantum system&amp;#039;&amp;#039;&amp;#039; is a system that interacts with its surrounding environment. Such systems cannot be fully described by a single wavefunction; instead, they are described using a &amp;#039;&amp;#039;&amp;#039;density operator&amp;#039;&amp;#039;&amp;#039; &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt;.&amp;lt;ref&amp;gt;{{cite book |last=Breuer |first=Heinz-Peter |last2=Petruccione |first2=Francesco |title=The Theory of Open Quantum Systems |publisher=Oxford University Press |year=2002}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
This interaction leads to phenomena such as decoherence and dissipation, which cause the loss of quantum coherence and energy into the environment. As a result, the system’s dynamics are typically governed by master equations that account for both unitary evolution and environmental effects.&lt;br /&gt;
&lt;br /&gt;
[[File:Open_quantum_systems_yellow.jpg|thumb|400px|Open quantum systems: interaction with the environment, decoherence, dissipation, and quantum noise.]]&lt;br /&gt;
&lt;br /&gt;
=== Density matrix ===&lt;br /&gt;
The density operator provides a general description of quantum states, including both pure states and statistical mixtures:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho = \sum_i p_i |\psi_i\rangle \langle \psi_i|,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;p_i&amp;lt;/math&amp;gt; are probabilities.&lt;br /&gt;
&lt;br /&gt;
It satisfies:&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math&amp;gt;\rho \ge 0&amp;lt;/math&amp;gt; (positive)  &lt;br /&gt;
* &amp;lt;math&amp;gt;\mathrm{Tr}(\rho) = 1&amp;lt;/math&amp;gt; (normalized)  &lt;br /&gt;
* &amp;lt;math&amp;gt;\rho^\dagger = \rho&amp;lt;/math&amp;gt; (Hermitian)  &lt;br /&gt;
&lt;br /&gt;
The expectation value of an observable &amp;lt;math&amp;gt;\hat{A}&amp;lt;/math&amp;gt; is&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\langle \hat{A} \rangle = \mathrm{Tr}(\rho \hat{A}).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Reduced density matrix ===&lt;br /&gt;
&lt;br /&gt;
For a system composed of a subsystem &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; and environment &amp;lt;math&amp;gt;E&amp;lt;/math&amp;gt;, the total state lives in&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\mathcal{H}_S \otimes \mathcal{H}_E.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The state of the subsystem alone is obtained by taking the &amp;#039;&amp;#039;&amp;#039;partial trace&amp;#039;&amp;#039;&amp;#039; over the environment:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho_S = \mathrm{Tr}_E(\rho_{SE}).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This operation removes environmental degrees of freedom.&lt;br /&gt;
&lt;br /&gt;
=== Mixed states and entanglement ===&lt;br /&gt;
&lt;br /&gt;
Even if the combined system &amp;lt;math&amp;gt;\rho_{SE}&amp;lt;/math&amp;gt; is in a pure state, the reduced state &amp;lt;math&amp;gt;\rho_S&amp;lt;/math&amp;gt; is generally mixed. This reflects entanglement between the system and its environment.&lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
The density matrix formalism:&lt;br /&gt;
&lt;br /&gt;
* allows description of open systems,  &lt;br /&gt;
* captures statistical mixtures and decoherence,  &lt;br /&gt;
* is essential in quantum information and thermodynamics.&lt;br /&gt;
&lt;br /&gt;
=Decoherence=&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Decoherence&amp;#039;&amp;#039;&amp;#039; is the process by which a quantum system loses its coherent superposition due to interaction with its environment. It provides a mechanism for the emergence of classical behavior from quantum systems.&amp;lt;ref&amp;gt;{{cite book |last=Zurek |first=Wojciech H. |title=Decoherence and the Transition from Quantum to Classical |publisher=Springer |year=2003}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Basic idea ===&lt;br /&gt;
&lt;br /&gt;
When a quantum system interacts with its environment, the combined system becomes entangled:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\psi\rangle_S \otimes |E_0\rangle \rightarrow \sum_i c_i |i\rangle_S \otimes |E_i\rangle.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The environment effectively &amp;quot;records&amp;quot; information about the system.&lt;br /&gt;
&lt;br /&gt;
=== Loss of coherence ===&lt;br /&gt;
&lt;br /&gt;
The reduced density matrix of the system becomes&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho_S = \mathrm{Tr}_E(\rho_{SE}).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Off-diagonal elements (coherences) in the density matrix decay over time:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho_{ij} \rightarrow 0 \quad (i \ne j).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This suppresses interference effects.&lt;br /&gt;
&lt;br /&gt;
=== Pointer states ===&lt;br /&gt;
&lt;br /&gt;
Certain states, called &amp;#039;&amp;#039;&amp;#039;pointer states&amp;#039;&amp;#039;&amp;#039;, remain stable under environmental interaction. These states form the preferred basis in which classical behavior emerges.&lt;br /&gt;
&lt;br /&gt;
=== Relation to measurement ===&lt;br /&gt;
&lt;br /&gt;
Decoherence explains why quantum superpositions are not observed at macroscopic scales. It does not by itself select a single outcome, but it explains the apparent collapse of the wavefunction in practical terms.&lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
Decoherence:&lt;br /&gt;
&lt;br /&gt;
* explains the quantum-to-classical transition,  &lt;br /&gt;
* limits coherence in quantum systems,  &lt;br /&gt;
* is a major challenge in quantum computing and information processing.  &lt;br /&gt;
&lt;br /&gt;
It is a central concept in understanding real-world quantum systems.&lt;br /&gt;
&lt;br /&gt;
=Environment coupling=&lt;br /&gt;
&lt;br /&gt;
In an open quantum system, the system of interest interacts with an external &amp;#039;&amp;#039;&amp;#039;environment&amp;#039;&amp;#039;&amp;#039; (or bath). This interaction is responsible for decoherence, dissipation, and noise.&amp;lt;ref&amp;gt;{{cite book |last=Breuer |first=Heinz-Peter |last2=Petruccione |first2=Francesco |title=The Theory of Open Quantum Systems |publisher=Oxford University Press |year=2002}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== System–environment model ===&lt;br /&gt;
&lt;br /&gt;
The total Hamiltonian is typically written as&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{H} = \hat{H}_S + \hat{H}_E + \hat{H}_{\text{int}},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where:&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math&amp;gt;\hat{H}_S&amp;lt;/math&amp;gt; describes the system,  &lt;br /&gt;
* &amp;lt;math&amp;gt;\hat{H}_E&amp;lt;/math&amp;gt; describes the environment,  &lt;br /&gt;
* &amp;lt;math&amp;gt;\hat{H}_{\text{int}}&amp;lt;/math&amp;gt; represents the interaction.  &lt;br /&gt;
&lt;br /&gt;
=== Weak coupling ===&lt;br /&gt;
&lt;br /&gt;
In many cases, the interaction between system and environment is weak. This allows approximate descriptions where:&lt;br /&gt;
&lt;br /&gt;
* the environment acts as a reservoir,  &lt;br /&gt;
* the system evolves with small perturbations.  &lt;br /&gt;
&lt;br /&gt;
This regime is often treated using perturbation theory.&lt;br /&gt;
&lt;br /&gt;
=== Markovian approximation ===&lt;br /&gt;
&lt;br /&gt;
If the environment has no memory (fast relaxation), the dynamics are called &amp;#039;&amp;#039;&amp;#039;Markovian&amp;#039;&amp;#039;&amp;#039;. In this case:&lt;br /&gt;
&lt;br /&gt;
* the system evolution depends only on its current state,  &lt;br /&gt;
* memory effects can be neglected.  &lt;br /&gt;
&lt;br /&gt;
This approximation leads to simple evolution equations.&lt;br /&gt;
&lt;br /&gt;
=== Non-Markovian dynamics ===&lt;br /&gt;
&lt;br /&gt;
If the environment retains memory, the system exhibits &amp;#039;&amp;#039;&amp;#039;non-Markovian&amp;#039;&amp;#039;&amp;#039; behavior:&lt;br /&gt;
&lt;br /&gt;
* information can flow back from environment to system,  &lt;br /&gt;
* coherence can partially recover,  &lt;br /&gt;
* dynamics become more complex.  &lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
Environment coupling:&lt;br /&gt;
&lt;br /&gt;
* explains why real quantum systems are never perfectly isolated,  &lt;br /&gt;
* determines decoherence rates,  &lt;br /&gt;
* is central to quantum technologies and noise control.&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 Open quantum systems|1}}&lt;/div&gt;</summary>
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