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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;
&amp;#039;&amp;#039;&amp;#039;Quantum trajectories&amp;#039;&amp;#039;&amp;#039; the stochastic time evolution of individual quantum systems interacting with an environment or undergoing continuous measurement. A representation of open quantum dynamics in terms of random pure-state evolutions instead of deterministic density matrix evolution.&amp;lt;ref name=&amp;quot;WisemanMilburn&amp;quot;&amp;gt;{{cite book |last=Wiseman|first=H. M.|last2=Milburn|first2=G. J.|title=Quantum Measurement and Control|publisher=Cambridge University Press|year=2010|doi=10.1017/CBO9780511813948|url=https://www.cambridge.org/core/books/quantum-measurement-and-control/F78F445CD9AF00B10593405E9BAC6B9F&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dalibard1992&amp;quot;&amp;gt;{{cite journal |last=Dalibard |first=J. |last2=Castin |first2=Y. |last3=Mølmer |first3=K. |title=Wave-function approach to dissipative processes in quantum optics |journal=Physical Review Letters |volume=68 |pages=580–583 |year=1992 |url=https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.68.580 |doi=10.1103/PhysRevLett.68.580}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
This approach is also known as the &amp;#039;&amp;#039;&amp;#039;quantum jump method&amp;#039;&amp;#039;&amp;#039; or &amp;#039;&amp;#039;&amp;#039;stochastic unraveling&amp;#039;&amp;#039;&amp;#039; of the master equation.&amp;lt;ref name=&amp;quot;PlenioKnight1998&amp;quot;&amp;gt;{{cite journal |last=Plenio |first=M. B. |last2=Knight |first2=P. L. |title=The quantum-jump approach to dissipative dynamics in quantum optics |journal=Reviews of Modern Physics |volume=70 |pages=101–144 |year=1998 |url=https://link.aps.org/doi/10.1103/RevModPhys.70.101 |doi=10.1103/RevModPhys.70.101}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:Quantum_trajectories.jpg|thumb|400px|Quantum trajectories describe stochastic evolution of individual quantum systems under measurement and environmental interaction.]]&lt;br /&gt;
&lt;br /&gt;
=Quantum Trajectories=&lt;br /&gt;
== Basic idea ==&lt;br /&gt;
&lt;br /&gt;
Instead of evolving the density operator &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt;, quantum trajectories describe the evolution of a state vector &amp;lt;math&amp;gt;|\psi(t)\rangle&amp;lt;/math&amp;gt; subject to stochastic processes.&lt;br /&gt;
&lt;br /&gt;
=== Ensemble interpretation ===&lt;br /&gt;
&lt;br /&gt;
The density operator is recovered as an average over trajectories:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\rho(t) = \mathbb{E}\left[|\psi(t)\rangle \langle \psi(t)|\right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Each trajectory corresponds to a possible physical realization of the system’s evolution.&amp;lt;ref name=&amp;quot;WisemanMilburn&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Connection to Lindblad equation ==&lt;br /&gt;
&lt;br /&gt;
Quantum trajectories provide an equivalent formulation of the Lindblad master equation.&lt;br /&gt;
&lt;br /&gt;
=== Unraveling ===&lt;br /&gt;
&lt;br /&gt;
The Lindblad equation&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;
can be represented as stochastic evolution of pure states.&amp;lt;ref name=&amp;quot;PlenioKnight1998&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Physical meaning ===&lt;br /&gt;
&lt;br /&gt;
* continuous evolution → effective non-Hermitian Hamiltonian  &lt;br /&gt;
* jumps → discrete stochastic events  &lt;br /&gt;
&lt;br /&gt;
Together they reproduce the ensemble dynamics.&lt;br /&gt;
&lt;br /&gt;
== Quantum jump method ==&lt;br /&gt;
&lt;br /&gt;
=== Effective Hamiltonian ===&lt;br /&gt;
&lt;br /&gt;
Between jumps, the system evolves under&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{H}_{\mathrm{eff}} =&lt;br /&gt;
\hat{H}&lt;br /&gt;
-&lt;br /&gt;
\frac{i\hbar}{2}&lt;br /&gt;
\sum_k L_k^\dagger L_k.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This produces non-unitary evolution.&amp;lt;ref name=&amp;quot;Dalibard1992&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Jump process ===&lt;br /&gt;
&lt;br /&gt;
At random times:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|\psi\rangle \rightarrow \frac{L_k |\psi\rangle}{\|L_k |\psi\rangle\|}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The jump probability depends on &amp;lt;math&amp;gt;\langle L_k^\dagger L_k \rangle&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Continuous measurement ==&lt;br /&gt;
&lt;br /&gt;
Quantum trajectories arise naturally in continuous measurement theory.&lt;br /&gt;
&lt;br /&gt;
=== Measurement interpretation ===&lt;br /&gt;
&lt;br /&gt;
Each trajectory corresponds to a measurement record.&lt;br /&gt;
&lt;br /&gt;
Examples:&lt;br /&gt;
&lt;br /&gt;
* photon counting  &lt;br /&gt;
* homodyne detection  &lt;br /&gt;
* weak measurement  &lt;br /&gt;
&lt;br /&gt;
This links stochastic evolution to experimental observations.&amp;lt;ref name=&amp;quot;WisemanMilburn&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Diffusive trajectories ==&lt;br /&gt;
&lt;br /&gt;
In some cases, evolution is continuous rather than involving jumps.&lt;br /&gt;
&lt;br /&gt;
=== Stochastic Schrödinger equation ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
d|\psi\rangle = -\frac{i}{\hbar}\hat{H}|\psi\rangle dt + \text{noise terms}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
These describe continuous monitoring processes.&amp;lt;ref name=&amp;quot;PlenioKnight1998&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Relation to decoherence ==&lt;br /&gt;
&lt;br /&gt;
Decoherence emerges from averaging over trajectories:&lt;br /&gt;
&lt;br /&gt;
* individual trajectories remain pure  &lt;br /&gt;
* ensemble average produces mixed states  &lt;br /&gt;
&lt;br /&gt;
This explains loss of coherence in open systems.&lt;br /&gt;
&lt;br /&gt;
== Applications ==&lt;br /&gt;
&lt;br /&gt;
=== Quantum optics ===&lt;br /&gt;
&lt;br /&gt;
Used to model photon emission and detection processes.&amp;lt;ref name=&amp;quot;Dalibard1992&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Quantum information ===&lt;br /&gt;
&lt;br /&gt;
Applied in:&lt;br /&gt;
&lt;br /&gt;
* quantum feedback  &lt;br /&gt;
* error correction  &lt;br /&gt;
* qubit monitoring&amp;lt;ref name=&amp;quot;WisemanMilburn&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Numerical simulation ===&lt;br /&gt;
&lt;br /&gt;
Trajectory methods are often more efficient than solving master equations directly.&amp;lt;ref name=&amp;quot;PlenioKnight1998&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Physical significance ==&lt;br /&gt;
&lt;br /&gt;
Quantum trajectories provide a detailed picture of open quantum dynamics at the level of individual realizations. They unify stochastic processes, measurement theory, and quantum evolution.&amp;lt;ref name=&amp;quot;WisemanMilburn&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
They are essential for interpreting modern quantum experiments involving continuous observation.&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 Trajectories|1}}&lt;/div&gt;</summary>
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