- Is the interpretation of β0 as a velocity parameter necessary? The gravitational Compton length Λgr =rs/2β0 has no dependence on the small mass m, which conforms with the Equivalence Principle. Also the cyclotron frequencies at the monopole flux tubes of the gravitational field body are independent of m.
- There are two preferred values for β0: β0∼ 1 assigned with the Earth's gravitational field body an and β0∼ 2-11 assigned with the field body of the Sun.
- The velocity of the solar system with respect to the galaxy is of the same magnitude as β0, which supports the interpretation as velocity. The interpretation of β0=v0/c∼ 1 as a velocity of a massive object does not however look sensible.
- In the standard quantum theory two quantum lengths characterize a massive particle. The Compton length Λc= h/m and the de-Broglie wavelength Λde-B= h/mβ0, where β0=v0/c is the velocity of particle using light velocity as a unit.
- Could the gravitational Planck constant ℏgr(S) assigned to Sun and also planets in the Bohr model for planetary orbits corresponds to de-Broglie wave length and could β0 correspond to a velocity 220-230 km/s giving β ∈ [(.73, .77) × 10-3] of the solar system with respect to galactic center. The error is about 20 per cent. The gravitational Planck constant assigned with the Earth would correspond to the gravitational Compton length and the problem with β0=1 would disappear.
- M8-H duality for the gravitational Planck constant leads to a fractal generalization of Hubble's law suggesting that Hubble tension might relate to two slightly different values of β0∼1 in short and long length scales differing by 5-6 percent (see this). This interpretation is not consistent with the interpretation of Λgr for β0=1 as gravitational Compton length.
- The problem disappears if one can interpret v0≤ c as light velocity with c#= gtt1/2c≤ c along the space-time surface in the formula for the gravitational Compton length.
- This interpretation has non-trivial consequences. In the case of the Sun, the disappearance of the 1/β0(S)∼ 211 from the formula hgr reduces the gravitational Compton length and gives Λgr(S)= 3× 105Λgr(E) rather than Λgr(S)∼ 211× 3× 105× Λgr(E). The energy E= hgr(S)f for a given frequency would be also reduced by β0(S)∼ 2-11.
- For the dark cyclotron the transitions at the magnetic body, the dependendence of cyclotron energy on m disappears. For other frequencies this is not the case and one would have E=hgrf= (GMm/2πc#)× f. A possible test is to look whether the energies for slightly different masses m differ.
- Examples would be proton and hydrogen atom with a relative mass difference of order 2-11 and proton and neutron with mass difference of .14 per cent. One can imagine an entire spectroscopy allowing to test the notion of gravitational Planck constant by using the effects caused by the transformation of gravitationally dark photons to ordinary ones. Biophotons could be products of this transformation.
Could the values of E be invariant under fluctuations and so that the small fluctuations of hgr induce small fluctuations of f.
- The fluctuations Δ c#/c# required to produce the effect would be quite too large as compared to the reduction of the value of c from its maximal value by GMS/AU =rs(S)/2AU∼ 10-9 and GME/RE= rs(E)/2RE∼ 10-9.
- The model for the Allais effect proposed that diffraction-like effect for the gravitational flux tubes meaning a deviation of the monopole flux tubes, analogous to the deviation of flow lines of a hydrodynamic flow past solid object, could produce reduction of the effective gravitational flux. This would reduce the effective gravitational mass MS experienced by the pendulum.
- But why should this reduction be Δ f/f≤ 2-11? Could the change of the mass of the pendulum could affect the value of hgr forcing the change of f if E is invariant? The reduction Δ m/m≤ 2-11 for the mass of the pendulum is highly implausible.
- What about the mass of the field body? Δ f/f≤ 2-11 is not far from the electron-proton mass ratio me/mp∼ 1/1880: the deviation is 9 per cent. If the field body contains hydrogen atoms, their ionization to protons and electrons transforming to ordinary electrons would reduce hgr by the required amount.
The hydrogen atoms should be Rydberg atoms with a very small binding energy and therefore with very large size: this is indeed possible at the field body. The dropped electrons should have smaller energy compensating for the energy needed for the energy needed for ionization. The transition could take place by tunnelling and therefore involve a pair of "big" state function reductions (BSFRs).
This kind of phase transition should occur at quantum criticality assigned with the beginning of the solar eclipse? Why the turning of the monopole flux tubes meeting the Moon should induce a phase transition leading to the transformation of dark electrons to ordinary electrons? Are the electrons so near to ionization state the turning ionizes them?
For a summary of earlier postings see Latest progress in TGD.
For the lists of articles (most of them published in journals founded by Huping Hu) and books about TGD see this.
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