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Carbon-burning process

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The carbon-burning process, also known as carbon fusion, is a series of nuclear fusion reactions. These reactions occur within the cores of massive stars. During this stage, carbon nuclei combine to create new, heavier elements. This process is a vital part of stellar evolution. It helps determine how a star lives and how it eventually dies.

To begin carbon burning, a star must reach extreme conditions. The core must have very high temperatures and high densities. The specific requirements depend on the mass of the star. More massive stars must offset greater gravitational forces to maintain hydrostatic equilibrium. This state of balance prevents the star from collapsing under its own weight. Because they must fight stronger gravity, massive stars often have higher temperatures but lower densities. Scientists use computer algorithms and numerical stellar models to calculate these exact figures.

When two carbon nuclei collide, they form an excited state of a magnesium-24 nucleus. This state is called a resonance. This resonance is very important because it makes the reaction easier. Without it, the star would need temperatures one hundred times higher to burn carbon. From this excited magnesium state, the nucleus can decay in several ways. The most frequent results are strongly exothermic reactions. This means they release a large amount of energy. Other reactions can be endothermic, meaning they absorb energy instead of releasing it. For example, one reaction produces neutrons. These neutrons can later help form even heavier isotopes through the s-process.

The resulting mixture in the core is quite diverse. The process primarily produces oxygen, neon, sodium, and magnesium. Some of the sodium produced can capture protons to form neon and helium. In stars between 4 and 11 solar masses, much of the oxygen from previous helium fusion survives. This is because it survives the carbon-burning process despite some of it being used up. The final core composition depends heavily on the star's starting mass and its evolutionary stage.

A major factor during this stage is neutrino loss. As temperatures rise, a process called pair production occurs. High-energy gamma rays interact with electromagnetic fields near atomic nuclei. This can create an electron and a positron. Usually, these particles annihilate to produce more light. However, about one in 10^19 times, they undergo a weak interaction. This replaces them with a neutrino and an anti-neutrino pair. These neutrinos move at nearly the speed of light. They interact very weakly with matter, so they escape the star immediately. This carries away a massive amount of energy.

Neutrino losses significantly change how stars age. The energy lost to neutrinos is comparable to the energy produced by fusion. To stay in equilibrium, the star must burn its fuel faster to offset these losses. This creates a cycle where the star burns through successive fuels more rapidly. For a star with 25 solar masses, the timing is dramatic. It burns hydrogen for 10^7 years and helium for 10^6 years. However, it burns carbon for only about 10^3 years.

Stars follow different paths based on their mass. Stars below 4 solar masses never reach the temperature needed for carbon burning. They end their lives as carbon-oxygen white dwarfs. Stars between 8 and 10 solar masses may experience a carbon flash. This is a sudden ignition that lasts only milliseconds and disrupts the core. These stars eventually leave behind an oxygen, neon, sodium, and magnesium white dwarf. Stars heavier than 8 solar masses start carbon burning in a non-degenerate core. Once the carbon is exhausted, they move on to neon burning as the core contracts and heats up.

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