OK, as requested, below are a few citations of nucleon clusters (e.g., the spherons of Pauling) documented as realistic structures in isotopes--this forum does not allow for large downloads, so I limited the abstracts to essential details. I believe that the MIT bag model fits the hypothesis I suggest--although that may not be its original motivation.
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Cluster Nature of Li7 and Be7 Tombrello, T. A.; Phillips, G. C. ; Physical Review, vol. 122, Issue 1, pp. 224-228, 1961
Abstract
Measurements of the capture gamma-radiation processes, mass 3+alpha-->mass 7+gamma and nucleon+Li6-->mass 7+gamma, give information about the cluster structure of the mirror nuclei Li7 and Be7. The cluster model predicts that the ground state and low excited states of these nuclei should have large reduced widths...Scattering experiments provide accurate initial, capturing, wave functions, and an assumption of the cluster nature of the final, bound, states...reduced widths deduced show that theta3+42 is large, theta1+62 is small, and that the ground states and first excited states of Li7 and Be7 are primarily of the two-body cluster form mass 3 + alpha particle.
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The "two-body cluster mass 3" that is referenced for Li7 would be the [NPN] spheron and [PNP] for Be7. Thus the "fundamental structure" of Li7 is two spherons [NPN]+ alpha which is the spheron {[NP]+[NP]}. For Be7 we get [PNP]+ {[NP]+[NP]}. Now, if we apply MIT bag model formalism we see that the dynamics of Li7 at quark level would be a 9-quark bag for [NPN] forming resonance with alpha, which is itself a structure with two 6-quark bags interacting. I realize this is not how the Standard Model views Li7--that is why I offer a new hypothesis as discussed above, which is supported by experiment such as cited above and below.
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Supermultiplet Symmetry and Near-Threshold Levels in Systems Featuring Two or Three Extremely Light Clusters
Physics of the Atomic Nuclei, Vol. 63, 2000, pp. 195-203
Lebedev, V. M.a; Neudatchin, V. G.a; Sakharuk, A. A.b
a. Institute of Nuclear Physics, Moscow State University, Vorob’evy gory, Moscow, 119899 Russia b. Brest State University, Brest, Belarus
Abstract
On the basis of the supermultiplet potential model for the interaction of extremely light clusters (formalism of Young diagrams), it is explained why the d + t system does not feature a (1/2)+ (L = 0) level allied to (3/2)+ (L = 0) thermonuclear resonance. By using known data on the quasielastic knockout of nucleons from the inner 1s shell of light nuclei, a systematics of near-threshold states in the t + d + d, t + t + d, and t + t + t systems is constructed in terms of excited Young diagrams like \{f\} = \{322\}. The emergence of similar states in going over from the d + d and t + t systems (which feature no such states) to the alpha + d + d, alpha + t + d, and alpha + t + t systems (where they appear owing to the binding effect of the alpha particle) is discussed. The three-cluster states being considered may be important not only for nuclear physics proper but also for nuclear astrophysics. © 2000 MAIK “Nauka / Interperiodica”.
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The "three cluster states" cited above are the spherons of Pauling, today more commonly called "nucleon clusters".
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Finally, lots of good information on the cluster aspects of isotopes at these two links:
http://arjournals.annualreviews.org/doi/abs/10.1146/annurev.ns.45.120195.000513?journalCode=nucl&cookieSet=1
http://www.worldscibooks.com/physics/4354.html