Predicting Nuclear Spin with Shell Model: How is it Calculated and Validated?

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SUMMARY

The discussion focuses on predicting the total nuclear spin using the shell model, specifically addressing the roles of even-even, even-odd, and odd-odd nuclei. It establishes that double magic nuclei exhibit a total spin of 0+ due to paired neutrons and protons. The presence of unpaired nucleons significantly influences the total nuclear spin, with odd-even configurations having precise spins and odd-odd configurations yielding a range of possible spins. The shell model provides potential quantum numbers, but experimental validation is necessary to determine the ground state configuration.

PREREQUISITES
  • Understanding of nuclear physics concepts, specifically the shell model.
  • Familiarity with nuclear spin and parity definitions.
  • Knowledge of pairing techniques in nuclear configurations.
  • Basic grasp of quantum numbers and their significance in nuclear states.
NEXT STEPS
  • Study the shell model of the nucleus in detail, focusing on magic numbers.
  • Explore pairing techniques and their application in predicting nuclear properties.
  • Learn about the experimental methods used to validate nuclear spin predictions.
  • Investigate the implications of unpaired nucleons on nuclear spin and parity.
USEFUL FOR

Students and researchers in nuclear physics, physicists specializing in nuclear structure, and anyone interested in the theoretical predictions and experimental validations of nuclear spin properties.

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How would one predict the total spin of a nucleus given Z, N and the shell model? Does it have to to do with even-even, even-odd, odd-odd nuclei?
 
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Yes, defenetly. In "close to magic numbers" nuclei, one can use the shell model to predict spin and parity of ground states, using pairing techniques. For example, a double magic nuclei, surely has 0+, because all it neutrons and protons are paired, and closing shells. If you add one neutron then spin and parity only depend on the posibilitis of this last one.
 
unpaired nucleons determine total nuclear spin.

odd-even or even-odd have presise spin (only 1 unpaire nucleon)

even - even no net spin

odd - odd spin lies in range \vert j_{1}-j_{2}\vertto j_{1}+j_{2}
 
Also you must serach for every unpaired nucleon i shells, and add their spins acording to the formula given by neu.

And then multiply each unpaired nucelon parity (parity is given by quantum number l)

Then also the shell model just gives you the possible quantum numbers (you do not know witch one is the ground state if you get three possible solutions for a given configuration) the experient gives you the outcome of this.
 

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