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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Nuclear fusion as a quantum-mechanical process}}&lt;br /&gt;
&lt;br /&gt;
{{Quantum matter backlink|Plasma and fusion physics}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Nuclear fusion&amp;#039;&amp;#039;&amp;#039; is a process in which two atomic nuclei combine to form a heavier nucleus, releasing energy. Fusion reactions power stars and are the basis for controlled fusion research on Earth.&lt;br /&gt;
&lt;br /&gt;
Fusion is fundamentally a quantum-mechanical process because it relies on quantum tunnelling to overcome the electrostatic repulsion between positively charged nuclei.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;float:right; border:1px solid #e0d890; background:#fff8cc; padding:6px; margin:0 0 1em 1em; width:420px;&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Fusion_reaction.png]]&lt;br /&gt;
&amp;lt;div style=&amp;quot;font-size:90%;&amp;quot;&amp;gt;Fusion reaction: two light nuclei combine to form a heavier nucleus, releasing energy.&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Basic mechanism ==&lt;br /&gt;
&lt;br /&gt;
Classically, two nuclei cannot approach each other due to the Coulomb barrier. However, quantum tunnelling allows particles to penetrate this barrier with a finite probability.&lt;br /&gt;
&lt;br /&gt;
The fusion rate depends on:&lt;br /&gt;
&lt;br /&gt;
* Particle density  &lt;br /&gt;
* Temperature  &lt;br /&gt;
* Quantum tunnelling probability  &lt;br /&gt;
&lt;br /&gt;
== Coulomb barrier ==&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Coulomb barrier&amp;#039;&amp;#039;&amp;#039; is the electrostatic repulsion between positively charged nuclei. It prevents nuclei from approaching each other at low energies.&lt;br /&gt;
&lt;br /&gt;
In classical physics, fusion would require extremely high temperatures to overcome this barrier. However, quantum tunnelling allows particles to penetrate the barrier even when their kinetic energy is insufficient.&lt;br /&gt;
&lt;br /&gt;
The height of the barrier depends on the charges of the nuclei and their separation distance.&lt;br /&gt;
&lt;br /&gt;
== Maxwellian average ==&lt;br /&gt;
&lt;br /&gt;
In a thermal plasma, particle velocities follow a Maxwell–Boltzmann distribution. The fusion reaction rate depends on the average of the product of cross section and velocity:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\langle \sigma v \rangle&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This quantity is known as the &amp;#039;&amp;#039;&amp;#039;Maxwellian average&amp;#039;&amp;#039;&amp;#039; and determines the effective fusion rate at a given temperature.&lt;br /&gt;
&lt;br /&gt;
== Gamow peak ==&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Gamow peak&amp;#039;&amp;#039;&amp;#039; represents the most probable energy range at which fusion reactions occur.&lt;br /&gt;
&lt;br /&gt;
It arises from the combination of:&lt;br /&gt;
&lt;br /&gt;
* The Maxwell–Boltzmann distribution (favoring higher energies)  &lt;br /&gt;
* Quantum tunnelling probability (favoring lower energies)  &lt;br /&gt;
&lt;br /&gt;
The resulting peak defines the energy window where fusion reactions are most likely.&lt;br /&gt;
&lt;br /&gt;
== Fusion reactions ==&lt;br /&gt;
&lt;br /&gt;
Common fusion reactions include:&lt;br /&gt;
&lt;br /&gt;
* Deuterium–tritium (D–T)  &lt;br /&gt;
* Deuterium–deuterium (D–D)  &lt;br /&gt;
* Proton–proton (stellar fusion)  &lt;br /&gt;
&lt;br /&gt;
These reactions release energy according to mass–energy conversion.&lt;br /&gt;
&lt;br /&gt;
== Relation to plasma physics ==&lt;br /&gt;
&lt;br /&gt;
Fusion occurs in high-temperature [[Physics:Quantum Plasma physics|plasmas]] where particles have sufficient energy to approach each other.&lt;br /&gt;
&lt;br /&gt;
The conditions required for sustained fusion are described by the [[Physics:Quantum Fusion reactions and Lawson criterion|Lawson criterion]].&lt;br /&gt;
&lt;br /&gt;
== Confinement ==&lt;br /&gt;
&lt;br /&gt;
To achieve fusion, plasma must be confined:&lt;br /&gt;
&lt;br /&gt;
* Magnetic confinement → [[Physics:Quantum Tokamak|tokamak]]  &lt;br /&gt;
* Inertial confinement  &lt;br /&gt;
&lt;br /&gt;
Confinement determines how long particles remain in conditions suitable for fusion.&lt;br /&gt;
&lt;br /&gt;
== Physical interpretation ==&lt;br /&gt;
&lt;br /&gt;
Fusion represents the conversion of mass into energy through nuclear interactions governed by quantum mechanics.&lt;br /&gt;
&lt;br /&gt;
It connects:&lt;br /&gt;
&lt;br /&gt;
* Quantum tunnelling  &lt;br /&gt;
* Plasma physics  &lt;br /&gt;
* Energy generation  &lt;br /&gt;
&lt;br /&gt;
=See also=&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also/Matter}}&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|Nuclear fusion|1}}&lt;/div&gt;</summary>
		<author><name>imported&gt;WikiHarold</name></author>
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