Rade Posted March 29, 2010 Report Posted March 29, 2010 I have an observation about the 1s nuclear shell. If we assume the "shell model" is a valid explanation of energy levels for isotopes, I find it very interesting (but I do not in any way understand) that only four isotopes find "stability" when nucleons (thus quarks) are packed into the first energy level, the 1s shell. I will use N=neutron, P=proton; thus the isotopes that find stability within the 1s shell are: [P] = the proton[NP] = deuteron[PNP] = helium-3[NPNP] = helium-4 And, the set of other possible nucleon arrangements for the 1s shell that are "unstable": [N] = the neutron[NN] = dineutron[NNN] =trineutron[NNNN] = tetraneutron[NPN] = triton = hydrogen-3[PP] = diproton[PPP] = triproton[PPPP] = tetraproton[NPNN] = hydrogen-4[PNPP] = lithium-4 Now, I look at the set of four stable isotopes, and I see a possible selection "fermion to boson" rule that would explain the building of stable light isotopes. It is: 1. Start with the stable proton [P] = fermion2. Add an unstable neutron [N] = result is stable deuteron [PN] = boson3. Add a second stable proton [P] = result is stable helium-3 [PNP] = fermion4. Add a second unstable [N] = result is very stable helium-4 [PNPN] = boson It thus seems to me, that stability in the 1s nuclear shell results from the formation of "clusters" of nucleons in a very specific order, from fermion to boson, starting with the very stable fermion [P], and ending with the very stable boson [PNPN] and not from the random placement of "individual" fermions [P & N] into separate proton and neutron energy potential wells within the 1s nuclear shell. I would appreciate comments on the above from someone that studies nuclear shell structure. Thanks. Quote
Recommended Posts
Join the conversation
You can post now and register later. If you have an account, sign in now to post with your account.