Nuclear Shell Model: Explaining Nucleon Occupancy

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SUMMARY

The discussion centers on the Nuclear Shell Model, specifically the occupancy of nucleons in the 1p3/2 energy level. It is established that according to the Pauli exclusion principle, two fermions cannot occupy the same quantum state, leading to complex pairing scenarios among nucleons. The valence nucleon model is referenced, highlighting its limitations in accurately predicting nuclear spin and parity for certain nuclei, such as 11B and 10B. Ryan suggests consulting Krane's "Introductory Nuclear Physics" for a deeper understanding of these concepts.

PREREQUISITES
  • Understanding of the Nuclear Shell Model
  • Familiarity with the Pauli Exclusion Principle
  • Knowledge of nuclear spin quantum numbers
  • Basic concepts of nucleon pairing and energy levels
NEXT STEPS
  • Study the implications of the Pauli Exclusion Principle in nuclear physics
  • Explore Krane's "Introductory Nuclear Physics" for insights on the shell model
  • Research the nuclear spin quantum numbers of NMR active elements
  • Investigate the coupling of nucleons in various isotopes
USEFUL FOR

Students and researchers in nuclear physics, particularly those interested in nucleon occupancy, nuclear spin calculations, and the limitations of the Nuclear Shell Model.

Winga
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I don't know how nucleons occupy each energy level, especially the one with multiple states.

For example, 1p3/2, there are 4 states in this level, that can be occupied 4 nucleons.

If there are 2 nucleons in this level, do they must be paired-up? Why?

And if there are 3 nucleons in this level, 2 nucleons are paired and 1 nucleon is unpaired? Why?

According to Pauli exclusion principle, two fermions cannot occupy the same quantum state.
For 1p3/2, how can I assign nucleons to this state without violating this principle?
 

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The number of independent spin states for spin j is (2j+1), so j=3/2 has four independent spin states. There can be 4 protons and 4 neutrons in the 1p3/2 level.
The pairing in an unfilled level can be complicated.
 
Meir Achuz said:
The pairing in an unfilled level can be complicated.
This is what I wonder.

Is it the 1st one is upaired,
2nd ---> paired with the 1st one
3rd ---> unpaired
4th ---> paired with the 3rd one
 
Winga said:
This is what I wonder.

Is it the 1st one is upaired,
2nd ---> paired with the 1st one
3rd ---> unpaired
4th ---> paired with the 3rd one

In the valence nucleon model, this is usually assumed. But when you look at some nuclei and compute the nuclear spin and parity from the valence nucleon shell model, it often times gives the incorrect answers. So there must be something more going on than the shell model is able to tell us about. Krane's book, "introductory nuclear physics" gives a good (ok decent) discussion on this model and its short comings.

Cheers,
Ryan
 
Meir Achuz said:
The number of independent spin states for spin j is (2j+1), so j=3/2 has four independent spin states. There can be 4 protons and 4 neutrons in the 1p3/2 level.
The pairing in an unfilled level can be complicated.
Are these 4 states degenerate?
 
Astronuc said:
I had read it already, but it is not detail enough.

I just wonder the nuclear spin quantum number for some NMR active elements and their isotopes, but I have a difficulty in pairing up of nucleons.
 
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i also have same problem with use of nuclear shell to predict net spin of nuclei, for example in case of 11B(3/2) and 10B(I=3)
 
tuul said:
i also have same problem with use of nuclear shell to predict net spin of nuclei, for example in case of 11B(3/2) and 10B(I=3)

You mean how to find Nuclear spins of ground state for the following nuclei: ??

^{\text{11}}B and ^{\text{10}}B
 
  • #10
Perhaps this link will help see how nucleons fill shells:

http://www.lbl.gov/abc/wallchart/chapters/06/1.html
 
  • #11
Rade said:
Perhaps this link will help see how nucleons fill shells:

http://www.lbl.gov/abc/wallchart/chapters/06/1.html


But one has to know how to cuople.
 

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