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s-process

physical science Maturity 11-13 Next article →

The s-process, or slow neutron-capture process, is a vital series of nuclear reactions in astrophysics. It is the mechanism responsible for creating nucleosynthesis for about half of all atomic nuclei heavier than iron. These reactions occur within stars, specifically in asymptotic giant branch (AGB) stars. By building heavier elements from lighter ones, the s-process helps populate the periodic table. It allows the universe to create a wide variety of stable isotopes through a measured, step-by-step chain of events.

Nucleosynthesis periodic table
Nucleosynthesis periodic table

The mechanism begins with a seed nucleus, which is typically iron left behind by previous supernova explosions. This nucleus undergoes neutron capture, where it absorbs a single neutron to form a new isotope with a higher atomic mass. If this new isotope is stable, it can capture another neutron to continue growing. However, if the isotope is unstable, it undergoes beta decay. This decay process changes the nucleus into an element with the next higher atomic number. The process is called "slow" because there is enough time for this radioactive decay to occur before the next neutron is captured.

S-process-elem-Ag-to-Sb
S-process-elem-Ag-to-Sb

Scientists categorize the s-process into two distinct components: the main component and the weak component. The main component is responsible for producing heavy elements beyond strontium and yttrium, reaching up to lead in stars with low metallicity. This occurs in low-mass asymptotic giant branch stars and relies on a neutron source called carbon-13. In contrast, the weak component synthesizes isotopes from iron-group seeds up to strontium and yttrium. This takes place at the end of helium- and carbon-burning stages in massive stars, primarily using a neon-22 neutron source. These massive stars eventually become supernovae and spread these isotopes into interstellar gas.

Our understanding of this process grew through several major scientific discoveries. In 1956, Hans Suess and Harold Urey published a table of abundances showing peaks for strontium, barium, and lead. These peaks suggested the existence of particularly stable nuclei, which implied a slow capture process must be at work. In 1957, the B2FH review paper argued that the s-process occurs in red giant stars. A major confirmation came in 1952 when Paul W. Merrill discovered technetium in S-type and carbon stars. Because technetium has no isotope with a half-life longer than 4.2 million years, its presence proved stars were creating it recently.

S-process-elem-Ag-to-Sb
S-process-elem-Ag-to-Sb

The s-process is defined by its specific timescales and environmental conditions. While the r-process (rapid neutron-capture process) happens in seconds during violent explosions, the s-process takes place over thousands of years. In the s-process, decades can pass between individual neutron captures. The total amount of elements produced depends on the star's initial iron abundance and its ability to produce neutrons. The flux, or the number of neutrons passing through a unit area, is also critical. A 1961 model showed that a wide range of neutron fluxes is required to account for the specific abundances we observe in red-giant stars.

An interesting feature of the s-process is how it eventually reaches a termination point. The reaction chain eventually ends in a cycle involving lead, bismuth, and polonium. Specifically, the cycle includes the stable isotopes lead-206, 207, 208, and bismuth-209. When a nucleus captures a neutron and becomes polonium-210, it undergoes alpha decay to move back through the cycle. Because the neutron capture cross-section of lead-208 is so small, that specific isotope accumulates in large amounts. This creates a "ledge-precipice" structure in the abundance of elements rather than a smooth curve.

S-R-processes-atomic-mass-201-to-210
S-R-processes-atomic-mass-201-to-210

We can find physical evidence of these stellar factories in the form of stardust. Stardust consists of individual solid grains, such as silicon carbide, that condensed during mass loss from long-dead stars. These grains were trapped in meteorites during the formation of our Solar System. By using mass spectrometers to study these presolar grains, scientists have detected enriched s-process isotopes of xenon and krypton. These tiny grains serve as a direct link to the chemical history of the galaxy. They show how the s-process abundances in AGB-star atmospheres can change over time or vary from one star to another.

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File:Nucleosynthesis periodic table.svg
Nucleosynthesis periodic table.svg
File:S-process-elem-Ag-to-Sb.svg
S-process-elem-Ag-to-Sb.svg
File:S-R-processes-atomic-mass-201-to-210.svg
S-R-processes-atomic-mass-201-to-210.svg
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