Non-dissipative waves in excitonic insulators: a connection with superconductivity?

This comment was inspired by a popular article, which tells that in excitonic insulators, very fast waves with velocity about v∼ .01c, are detected. What caught my attention is that these waves do not dissipate. The theoretical challenge is to explain why this the case. The absence of dissipation means an analogy with superconductors.

I have just worked out the newest version of the TGD based model of superconductivity (see this) with an inspiration coming from the Berry phases model, in particular the anomalies of the BCS model mentioned in the article describing the model.

1. The model suggests a universal framework applying not only to super-conductivity but also to super-fluidity and various phenomena involving absence of dissipative effects.
2. The model predicts that also electrons rather than only Cooper pairs can propagate without dissipation at magnetic flux tubes at which $h_eff> h$ electrons and their Cooper behaving effectively like dark matter are. Also the Berry phase model predicts this.
3. Second prediction is that by external energy feed it is possible to have superconductivity also above Tc: this mechanism (metabolic energy feed) is the basic mechanism of TGD inspired quantum biology making possible high Tc superconductivity.
4. An attractive assumption is that the flux tubes mediated gravitational interaction: in this case one would have heff =h_gr= GMm/v₀, where M is Earth mass, m is the mass of charge carrier, and v₀ is velocity parameter with at Earth surface has value v₀=c/2 giving for the universal gravitational Compton length the value λ_gr= 2GM =r_s, the Scwartshild radius, which is .9 cm for Earth. This would predict universality for various supraphases. Intriguingly, for Sun and inner planets one has v₀= about 2^-11 and λ_gr is very near to the radius of Earth!

Excitonic insulators are described in a second popular article telling about their discovery (see this . They exist in a phase transition region between insulator and conductor as the gap between valence band and conduction band becomes zero. In the TGD framework this means quantum criticality and the presence of h_eff> h phases are associated with the long range correlations and fluctuations at criticality quite generally.

The physical picture looks very similar to that in super-conductivity.

1. Instead of Cooper pairs, one could have bound states of electron and hole bound by Coulomb interaction. The gap energy approaches zero at critical temperature in both cases. For a superconductor the gap energy corresponds to the energy needed to kick out an electron or Cooper pair formed at the level of ordinary matter to the magnetic flux tube with h_eff> h (increase of h_eff increases the energy of the state). The liberated binding energy – gap energy – allows the kicking. The gap energy is negative above Tc and superconductivity is not possible.

The same would apply also in the case of excitonic insulators. The formation of the bound states of h_eff> helectrons and holes would liberate the binding energy allowing kicking of something to the magnetic flux with h_eff> h.