I have been wanting to make a comment or two about the prospects for Manasson's proposal... Consider figure 1a in his
2008 paper. That's a binary tree with sixteen leaves, the leaves being the 16 fixed points of a limit cycle in some unknown dynamical system, which are also supposed to be 16 particle states from the first generation of the standard model.
There are other ways you might want to assign particle states to the fixed points of the bifurcation diagram. For example, he doesn't include quark color, which would multiply the number of quark states by three. But that would just bring the total number of states per generation to 32, which is the number of fixed points after the next bifurcation.
Also, he implicitly treats these particles as 4-state Dirac fermions, whereas we now understand the phenomenological Dirac fermions to arise from a Higgs mechanism that pairs up two 2-state Weyl fermions. Again, this is just a change in the details, it doesn't inherently affect the viability of the concept.
But however you make the assignment, ultimately you want to mimic the standard model. We know the lagrangian of the standard model, it contains many interaction terms that involve these fermionic states. So given a particular assignment of states to the tree, you can directly translate the lagrangian into the dynamical systems language.
The lagrangian will contain terms like "electron couples to charged weak boson and becomes neutrino", or "left-handed fermion couples to right-handed fermion via Higgs". These should translate directly to statements like "third fixed point on level 4 couples to charged weak boson and becomes seventh fixed point on level 4", etc.
Recall that, on the dynamical-systems side of this correspondence, the 16 states correspond to fixed points of a limit cycle in an iterated dynamical system. So the seventh fixed point is what you get after applying some mapping four times to the third fixed point.
There is another way to get there, and that is to change levels within the tree, rather than move along the same level. But either way, once you make a specific assignment of fermion states to the tree, this implies a large number of highly specific claims about how the bosons of the standard model (whatever they are) interact with the different states of the fundamental self-organizing system described by the bifurcation diagram.
So I want to propose a rather concrete way to explore the difficulties of implementing Manasson's vision. It's partly inspired by quantum computing, where there are concepts of a "physical qubit" and a "logical qubit". A physical qubit is a concrete quantum system - a nuclear spin, an electron spin, whatever. A logical qubit is a qubit at the level of quantum algorithms. A logical qubit is typically made of some number of physical qubits with an error correction scheme applied.
Anyway, what Manasson has done is to take a type of universal dynamical behavior, and propose that some version of it underlies particle physics. To judge the viability of this idea, we need a way to explore it in generality, or at least without already knowing the details of the fundamental self-organizing system. But we also need something concrete enough that we can try to make it work, and learn from the difficulties.
I think a quantum version of the logistic map can provide a concrete starting point. The logistic map, maps one value of x to another value of x, and has a parameter r. So the first step that I suggest, is to think of these as quantum states... |x>. There can be technical problems with having a continuum of quantum states, but they are familiar from ordinary quantum mechanics and we can use ordinary methods should they prove necessary.
So then the logistic map is actually an operator on a Hilbert space, or rather a family of operators parametrized by r. These states are then analogous to the states of the "physical qubit". Then, for specific values of r, there are fixed points and basins of attraction. These are analogous to the "logical qubit" states. Note that if a particular range of x-values belong to the basin of attraction for a single fixed point, there will be a subspace of the overall Hilbert space, whose basis vectors are the |x>s in that range.
So now we have a kind of concrete model for the fundamental self-organizing system. When we say "left-handed electron is third fixed point on level 4", that refers to a particular subspace of our Hilbert space. And this also gives a new concreteness to the propositions like "third fixed point on level 4 couples to charged weak boson and becomes seventh fixed point on level 4"; that is now a statement about how certain quantum systems interact.
I know that Manasson (and also
@Auto-Didact) hope to derive quantum mechanics itself from something more fundamental, but whatever the foundations, the standard model is quantum-mechanical and e.g. obeys the principle of superposition, so some version of the scheme has to make sense as a quantum theory.
Nonetheless, for those seeking something beneath quantum mechanics, I would point out a
recent paper by Tejinder Singh, which takes as its subquantum theory a version of Stephen Adler's trace dynamics. It's a relatively sophisticated approach.