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Nuclear reaction
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== Nuclear reaction equations == Nuclear reactions may be shown in a form similar to chemical equations, for which [[invariant mass]] must balance for each side of the equation, and in which transformations of particles must follow certain conservation laws, such as conservation of charge and baryon number (total atomic [[mass number]]). An example of this notation follows: {{block indent|[[Lithium-6|{{nuclide|lithium|6}}]] + [[Hydrogen-2|{{nuclide|hydrogen|2}}]] β [[Helium|{{nuclide|helium|4}}]] + ?.}} To balance the equation above for mass, charge and mass number, the second nucleus to the right must have atomic number 2 and mass number 4; it is therefore also helium-4. The complete equation therefore reads: {{block indent|[[Lithium-6|{{nuclide|lithium|6}}]] + [[Hydrogen-2|{{nuclide|hydrogen|2}}]] β [[Helium|{{nuclide|helium|4}}]] + [[Helium|{{nuclide|helium|4}}]].}} or more simply: {{block indent|[[Lithium-6|{{nuclide|lithium|6}}]] + [[Hydrogen-2|{{nuclide|hydrogen|2}}]] β 2 [[Helium|{{nuclide|helium|4}}]].}} Instead of using the full equations in the style above, in many situations a compact notation is used to describe nuclear reactions. This style of the form A(b,c)D is equivalent to A + b producing c + D. Common light particles are often abbreviated in this shorthand, typically p for proton, n for neutron, d for [[deuteron]], Ξ± representing an [[alpha particle]] or [[helium-4]], Ξ² for [[beta particle]] or electron, Ξ³ for [[gamma photon]], etc. The reaction above would be written as <sup>6</sup>Li(d,Ξ±)Ξ±.<ref>[http://www.astrophysicsspectator.com/topics/stars/FusionHydrogenRate.html The Astrophysics Spectator: Hydrogen Fusion Rates in Stars]</ref><ref> {{cite book |last=Tilley |first=R. J. D. |year=2004 |title=Understanding Solids: The Science of Materials |url=https://books.google.com/books?id=ZVgOLCXNoMoC&pg=PA495 |page=495 |publisher=[[John Wiley and Sons]] |isbn=0-470-85275-5 }}</ref>
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