NUCLEOSYNTHESIS!
    
      
        
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    There are two main processes by which nuclei that
      fill out the range of β-stable nuclei are formed. The most
      important process (since it has to happen first) is the so-called
      r process, an explosion which subjects the nuclei found in
      old, large stars to a flood of neutrons. This spray of neutrons
      instantly populates the neutron-drip line and then almost
      immediately these highly unstable nuclei decay down into the
      valley of β stability. The other important process is the
      so-called s process, which occurs over long periods of
      time in intermediate-mass stars, mainly in the so-called
      Asymptotic giant branch (AGB). This slow neutron capture process
      runs right down the valley of β stability; the nuclei formed are
      close to the valley and decay into it before they have any chance
      of capturing another neutron.  The r process is also vital in
      more exotic events, such as neutron-star collisions.  An
      imperfect knowledge of masses of nuclei far off the line of
      stability is needed in detailed calculations describing r
      processes. 
    
      
        
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    There are other processes of far less
        importance, such as proton capture. Observation of stars that
        formed very early in the history of the universe show an
        abundance of elements characteristic of the r process alone.
        While the types of supernovae that explosively compress the core
        are the standard suspects for r-process events, it is
        increasingly likely that scenarios involving collisions of
        neutron stars with other dense or denser objects play a
        significant role. 
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      NUCLEOSYNTHESIS IN THE
          EARLY UNIVERSE
      
      
      
      
       
      
      Between about 10 to 350
          seconds the entire universe had the right temperature and
          density, and comparable numbers of protons and neutrons, to do
          fusion in the ordinary nuclear way, which produced the
          primordial amounts of 4He, deuterium and 3He.
          Very, very tiny amounts of 7Be and 7Li
          were also generated. The incredibly rapid drop in density and
          temperature, and the fact that the half-life of a free neutron
          is only 10 minutes, made this era of Big Bang nucleosynthesis
          very short and very limited. The astonishing fact that
          interstellar gas which has never been inside a star is
          already only 75% protons and the remaining 25% helium made it
          very clear to researchers in the late 1950s that the
            entire universe must at one time have been hot and dense
            enough to fuse protons and neutrons into helium, and
          that this would have had to occur over a time frame fairly
          short compared to the free neutron lifetime.
      
      Pioneers of Cosmology
      
      Cosmology
        
      
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