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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Mathematical objects describing the propagation of quantum fields and particles between space-time points}}&lt;br /&gt;
&lt;br /&gt;
{{Quantum book backlink|Quantum field theory}}&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Propagators in quantum field theory&amp;#039;&amp;#039;&amp;#039; describe how quantum fields and their excitations propagate between different points in space-time.&amp;lt;ref name=&amp;quot;peskin&amp;quot;&amp;gt;Peskin, M. E.; Schroeder, D. V. &amp;#039;&amp;#039;An Introduction to Quantum Field Theory&amp;#039;&amp;#039; (1995).&amp;lt;/ref&amp;gt; They are central to the calculation of physical processes, particularly in perturbation theory and Feynman diagrams.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;float:right; border:1px solid #ccc; padding:4px; background:#fff8dc; margin:0 0 1em 1em; width:420px;&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Quantum_field_propagator.jpg|400px]]&lt;br /&gt;
&amp;lt;div style=&amp;quot;font-size:90%;&amp;quot;&amp;gt;Propagation of a quantum field excitation between two space-time points&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Definition ==&lt;br /&gt;
A propagator is a correlation function that gives the amplitude for a field to propagate from one point to another. For a scalar field, the time-ordered propagator is defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
D_F(x - y) = \langle 0 | T\{\phi(x)\phi(y)\} | 0 \rangle&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where:&lt;br /&gt;
* &amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt; denotes time ordering  &lt;br /&gt;
* &amp;lt;math&amp;gt;|0\rangle&amp;lt;/math&amp;gt; is the vacuum state  &lt;br /&gt;
&lt;br /&gt;
This function encodes how disturbances in the field travel through space-time.&amp;lt;ref name=&amp;quot;schwartz&amp;quot;&amp;gt;Schwartz, M. D. &amp;#039;&amp;#039;Quantum Field Theory and the Standard Model&amp;#039;&amp;#039; (2014).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Momentum-space representation ==&lt;br /&gt;
It is often useful to express propagators in momentum space:&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
D_F(p) = \frac{i}{p^2 - m^2 + i\epsilon}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where:&lt;br /&gt;
* &amp;lt;math&amp;gt;p^2 = p_\mu p^\mu&amp;lt;/math&amp;gt;  &lt;br /&gt;
* &amp;lt;math&amp;gt;m&amp;lt;/math&amp;gt; is the mass of the particle  &lt;br /&gt;
* &amp;lt;math&amp;gt;i\epsilon&amp;lt;/math&amp;gt; ensures proper boundary conditions  &lt;br /&gt;
&lt;br /&gt;
This form is widely used in calculations involving scattering amplitudes.&amp;lt;ref name=&amp;quot;peskin&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Physical interpretation ==&lt;br /&gt;
The propagator represents the probability amplitude for a particle to travel between two space-time points. However, in quantum field theory this is not a classical trajectory but a sum over all possible paths.&lt;br /&gt;
&lt;br /&gt;
It can also be interpreted as describing the propagation of virtual particles that mediate interactions.&amp;lt;ref name=&amp;quot;weinberg&amp;quot;&amp;gt;Weinberg, S. &amp;#039;&amp;#039;The Quantum Theory of Fields&amp;#039;&amp;#039; (1995).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Role in Feynman diagrams ==&lt;br /&gt;
In perturbation theory, propagators appear as internal lines in Feynman diagrams.&amp;lt;ref name=&amp;quot;feynman&amp;quot;&amp;gt;Feynman, R. P. (1949). Space-time approach to quantum electrodynamics.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Each internal line contributes a propagator factor, while vertices represent interactions. The full amplitude of a process is obtained by combining propagators and interaction terms according to specific rules.&lt;br /&gt;
&lt;br /&gt;
== Types of propagators ==&lt;br /&gt;
Different fields have different propagators:&lt;br /&gt;
&lt;br /&gt;
* Scalar propagator  &lt;br /&gt;
* Fermion propagator  &lt;br /&gt;
* Gauge boson propagator  &lt;br /&gt;
&lt;br /&gt;
For example, the fermion propagator is:&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
S_F(p) = \frac{i(\gamma^\mu p_\mu + m)}{p^2 - m^2 + i\epsilon}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
These reflect the spin and internal structure of the corresponding particles.&amp;lt;ref name=&amp;quot;schwartz&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Green&amp;#039;s function interpretation ==&lt;br /&gt;
Mathematically, propagators are Green&amp;#039;s functions of the field equations. For a scalar field:&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
(\Box + m^2) D_F(x - y) = -i \delta^{(4)}(x - y)&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This shows that the propagator acts as the fundamental solution to the field equation.&amp;lt;ref name=&amp;quot;weinberg&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Causality and time ordering ==&lt;br /&gt;
The time-ordering operator ensures that causality is preserved in relativistic quantum theory. Events are ordered such that operators at later times act first in the correlation function.&lt;br /&gt;
&lt;br /&gt;
This structure ensures consistency with relativistic causality and quantum mechanics.&amp;lt;ref name=&amp;quot;peskin&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Conceptual importance ==&lt;br /&gt;
Propagators connect the abstract field formalism to measurable quantities. They provide the link between:&lt;br /&gt;
&lt;br /&gt;
* field operators  &lt;br /&gt;
* particle propagation  &lt;br /&gt;
* observable scattering processes  &lt;br /&gt;
&lt;br /&gt;
They are therefore one of the central computational and conceptual tools in quantum field 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;
{{Author|Harold Foppele}}&lt;br /&gt;
&lt;br /&gt;
{{Sourceattribution|Quantum field theory (QFT) core|1}}&lt;/div&gt;</summary>
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