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Page Title: Energy Levels of the Nucleus
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Energy  Levels  of  Atoms
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Nuclear Physics and Reactor Theory Volume 1 of 2
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Mass  Defect and Binding Energy Summary

MASS DEFECT AND BINDING ENERGY DOE-HDBK-1019/1-93 Atomic and Nuclear Physics An atom cannot stay in the excited state for an indefinite period of time.   An excited atom will eventually  transition  to  either  a  lower-energy  excited  state,  or  directly  to  its  ground  state,  by emitting a discrete bundle of electromagnetic energy called an x-ray.   The energy of the x-ray will be equal to the difference between the energy levels of the atom and will typically range from several eV to 100,000 eV in magnitude. Energy  Levels  of  the  Nucleus The nucleons in the nucleus of an atom, like the electrons that circle the nucleus, exist in shells that  correspond  to  energy  states.    The  energy  shells  of  the  nucleus  are  less  defined  and  less understood than those of the electrons.   There is a state of lowest energy (the ground state) and discrete possible excited states for a nucleus.  Where the discrete energy states for the electrons of an atom are measured in eV or keV, the energy levels of the nucleus are considerably greater and typically measured in MeV. A nucleus that is in the excited state will not remain at that energy level for an indefinite period. Like the electrons in an excited atom, the nucleons in an excited nucleus will transition towards their  lowest  energy  configuration  and  in  doing  so  emit  a  discrete  bundle  of  electromagnetic radiation called a gamma ray (g-ray).   The only differences between x-rays and g-rays are their energy levels and whether they are emitted from the electron shell or from the nucleus. The ground state and the excited states of Figure 7    Energy Level Diagram - Nickel-60 a  nucleus  can  be  depicted  in  a  nuclear energy-level    diagram. The    nuclear energy-level diagram consists of a stack of horizontal  bars,  one  bar  for  each  of  the excited states of the nucleus.  The vertical distance  between  the  bar  representing  an excited state and the bar representing the ground state is proportional to the energy level  of  the  excited  state  with  respect  to the   ground   state. This   difference   in energy  between  the  ground  state  and  the excited state is called the excitation energy of the excited state.   The ground state of a nuclide has zero excitation energy.  The bars for the excited states are labeled with their respective energy levels.  Figure 7 is the energy level diagram for nickel-60. NP-01 Page 20 Rev. 0

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