Undergrad Understand selection rules in ##\beta##-decay/EC

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Direct decay to the ground state in beta decay is considered absolutely forbidden due to the significant change in angular momentum and parity, specifically a Δ J of 3, which requires a third order forbidden transition. First order forbidden transitions allow for Δ J of 0, 1, or 2, but they cannot accommodate such a large change. The discussion also clarifies that the selection rules for electron capture (EC) are not the same as those for beta decay, although both processes involve similar conservation laws. The participants emphasize that the questions raised about these concepts are valid and important for understanding nuclear physics. Overall, the complexities of selection rules in beta decay and EC highlight the intricate nature of nuclear transitions.
dRic2
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I'm not very familiar with this topic so I quickly went through some introductory books on nuclear physics and read the chpater about beta decay. What I don't understand looking at this graph is the following:
Why is the direct decay to ground state absolutely forbidden ? If you take a 1st order forbidden transition with ##l = 3##, then parity can change and conservation of angular momentum can be assured by requiring the electron and neutrino to have opposite spin (S = 0). Yet you don't see this.

An other question I have is: are EC selection rules the same ones I have in ##\beta##-decay? (I have zero background in nuclear physics so I apologize if my question is stupid)

Thanks Ric
 
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It's not impossible but apparently so unlikely that people haven't measured it yet.
 
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dRic2 said:
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I'm not very familiar with this topic so I quickly went through some introductory books on nuclear physics and read the chpater about beta decay. What I don't understand looking at this graph is the following:
Why is the direct decay to ground state absolutely forbidden ?

The groundstate of 152Eu is 3− and the groundstate of 152Gd is 0+. That's a change Δ J=3 and a change of parity. That's at least a third order forbidden transition.

If you take a 1st order forbidden transition with l=3, then parity can change and conservation of angular momentum can be assured by requiring the electron and neutrino to have opposite spin (S = 0). Yet you don't see this.
A first forbidden Fermi transition has a Δ J of 0,1. A first forbidden GT transition has a Δ J of 0,1,2. Both have a change of parity. You have to go to a third order forbidden transition to get Δ J = 3 with a change of parity.

An other question I have is: are EC selection rules the same ones I have in β-decay? (I have zero background in nuclear physics so I apologize if my question is stupid)
Yes and none of those questions were stupid in any way.
 
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bobob said:
You have to go to a third order forbidden transition to get Δ J = 3 with a change of parity.
Yes, sorry. I was writing in a rush and didn't notice. Thank you for spotting my mistake :)
 

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