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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Operator describing collisions in quantum kinetic theory}}&lt;br /&gt;
&lt;br /&gt;
{{Quantum methods backlink|Plasma and kinetic methods}}&lt;br /&gt;
&lt;br /&gt;
[[File:Quantum_field_theory_dependency_map.png|250px|right]]&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Quantum collision operator&amp;#039;&amp;#039;&amp;#039; is an operator used in [[Physics:Quantum kinetic theory]] to describe how interactions between particles change a quantum distribution function or density matrix over time. It represents the collisional part of a kinetic equation, separating scattering, relaxation, and redistribution processes from free motion and external-field evolution.&lt;br /&gt;
&lt;br /&gt;
In plasma, condensed-matter, and many-body systems, collision operators are used to model effects such as particle scattering, energy exchange, decoherence, damping, and transport. They provide a bridge between microscopic quantum dynamics and macroscopic quantities such as conductivity, diffusion, viscosity, and relaxation rates.&lt;br /&gt;
&lt;br /&gt;
== Role in kinetic equations ==&lt;br /&gt;
&lt;br /&gt;
A quantum kinetic equation often separates evolution into a reversible part and a collision part. Schematically,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\partial f}{\partial t} + \text{transport terms} = C[f],&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; is a distribution function and &amp;lt;math&amp;gt;C[f]&amp;lt;/math&amp;gt; is the collision operator.&lt;br /&gt;
&lt;br /&gt;
The collision operator accounts for interactions that change the occupation of quantum states. Depending on the system, these may include electron-electron collisions, electron-phonon scattering, particle-wave interactions, or collisions between charged particles in a plasma.&lt;br /&gt;
&lt;br /&gt;
== Quantum features ==&lt;br /&gt;
&lt;br /&gt;
Unlike a purely classical collision term, a quantum collision operator may include:&lt;br /&gt;
&lt;br /&gt;
* Pauli blocking for fermions;&lt;br /&gt;
* Bose enhancement for bosons;&lt;br /&gt;
* transition probabilities from quantum scattering amplitudes;&lt;br /&gt;
* coherence and off-diagonal density-matrix effects;&lt;br /&gt;
* detailed balance between quantum states.&lt;br /&gt;
&lt;br /&gt;
These features are important when the occupation of states, wave interference, or quantum statistics affect transport and relaxation.&lt;br /&gt;
&lt;br /&gt;
== Applications ==&lt;br /&gt;
&lt;br /&gt;
Quantum collision operators appear in:&lt;br /&gt;
&lt;br /&gt;
* [[Physics:Quantum kinetic theory]];&lt;br /&gt;
* [[Physics:Quantum Vlasov equation]];&lt;br /&gt;
* [[Physics:Quantum Transport theory]];&lt;br /&gt;
* nonequilibrium quantum field theory;&lt;br /&gt;
* semiconductor transport;&lt;br /&gt;
* dense plasma physics;&lt;br /&gt;
* quantum hydrodynamic and many-body models.&lt;br /&gt;
&lt;br /&gt;
They are especially useful when a system is not in thermal equilibrium but still requires a statistical description.&lt;br /&gt;
&lt;br /&gt;
=See also=&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also/Methods}}&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|Collision operator|1}}&lt;/div&gt;</summary>
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