| Term 
 | Definition 
 
        | Fragmentation of heavier nuclei by cosmic-ray bombardment Accounts for abundance of elements not synthesised in
 thermonuclear reactions.
 Explains existence and low abundance of some elements
 e.g.  6Li, 7Li, 9Be, 10B, 11B
 |  | 
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        | Term 
 
        | p-process (proton capture) |  | Definition 
 
        | Occur in supernova Makes small contribution to elemental abundance for elements synthesised
 by the s- or r-processes
 Explains existence and low abundance of some elements
 e.g.190Pt or 168Yb
 |  | 
        |  | 
        
        | Term 
 
        | r-process (rapid neutron addition) |  | Definition 
 
        | Timescale 0.01 – 10s Lots of neutrons added to nuclei  unstable
 Rapid - decay :  8-10 - emissions cascade to the next stable isotope
 -->Increased abundance peaks at 80, 30 and 194 as 8-10 mass units
 below nuclides associated with the s process.
 |  | 
        |  | 
        
        | Term 
 
        | s-process (slow neutron addition) |  | Definition 
 
        | Timescale 102 – 105 years Collision of nucleus with neutron  heavier nucleus
 Unstable nuclei formed decay by electron emission (-)
 -->formation of elements of mass 63-209 and non -process nuclei
 in 23-46 range
 |  | 
        |  | 
        
        | Term 
 
        | Neutron capture cross-section |  | Definition 
 
        | Build-up of certain isotopes e.g. 138Ba, 218Pb, 209Bi |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | s-process (slow neutron addition)--->Occurs in red giants r-process  (rapid neutron addition)--->Occurs in supernovae
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Supernova Violent explosion during supernova – massive release of energy
 Interconversions between nuclei, free protons and free neutrons
 Explains abundance of  Ti to Cu
 |  | 
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