Pairs of mirror nuclei have the same spin and parity.
2.
Since the strong interaction is invariant to protons and neutrons one can expect these mirror nuclei to have very similar binding energies.
3.
If we constrain to odd number of nucleons ( A = Z + N ) then we find mirror nuclei that differ one another by exchanging a proton by a neutron.
4.
The interesting observation is that " y " for mirror nuclei is on the order of the value of " y " for neutron decay while non-mirror nuclear decays tend to be an order of magnitude less.
5.
"' Mirror nuclei "'are nuclei where the number of protons of element one ( Z 1 ) equals the number of neutrons of element two ( N 2 ), the number of protons of element two ( Z 2 ) equal the number of neutrons in element one ( N 1 ) and, as a condequence, the mass number is the same ( A = N 1 + Z 2 = N 2 + Z 1 ).
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