The oxygen-burning process is a set of nuclear fusion reactions that take place in massive stars that have used up the lighter elements in their cores. Oxygen-burning is preceded by the neon-burning process and succeeded by the silicon-burning process. As the neon-burning process ends, the core of the star contracts and heats until it reaches the ignition temperature for oxygen burning. Oxygen burning reactions are similar to those of carbon burning; however, they must occur at higher temperatures and densities due to the larger Coulomb barrier of oxygen.
Reactions
Oxygen ignites in the temperature range of (1.5–2.6)×10<sup>9</sup> K and in the density range of (2.6–6.7)×10<sup>12</sup> kg·m<sup>−3</sup>. The principal reactions are given below, where the branching ratios assume that the deuteron channel is open (at high temperatures):
|- style="height:2em;"
| || || ||→ || ||+ ||
| +
|16.539 MeV
|- style="height:2em;"
| || || ||→ || ||+ ||2 Alpha particle|
| −
|0.393 MeV
|}
Near 2×10<sup>9</sup> K, the oxygen-burning reaction rate is approximately 2.8×10<sup>−12</sup>(T<sub>9</sub>/2)<sup>33</sup>,
