2020
DOI: 10.1002/prop.202000072
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Dark Energy and the Time Dependence of Fundamental Particle Constants

Abstract: The cosmic time dependencies of G, α, ℏ and of Standard Model parameters like the Higgs vev and elementary particle masses are studied in the framework of a new dark energy interpretation. Due to the associated time variation of rulers, many effects turn out to be invisible. However, a rather large time dependence is claimed to arise in association with dark energy measurements, and smaller ones in connection with the Standard Model.

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Cited by 2 publications
(5 citation statements)
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“…So the whole universe is carrying an extremely low frequency breathing vibration ω ≪ 10 −10 yrs −1 around L s , and all the tetron bonds on average are vibrating in accord with the universe. One can work out the details of this picture and indeed show that this effect accounts for the present accelerated expansion as given by the dark energy observations [4].…”
Section: Spring Modelmentioning
confidence: 60%
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“…So the whole universe is carrying an extremely low frequency breathing vibration ω ≪ 10 −10 yrs −1 around L s , and all the tetron bonds on average are vibrating in accord with the universe. One can work out the details of this picture and indeed show that this effect accounts for the present accelerated expansion as given by the dark energy observations [4].…”
Section: Spring Modelmentioning
confidence: 60%
“…Any cosmological constant contribution from tetrons has been removed in (26), because for the matter free elastic tetron substrate the binding forces do not drive the universe with Λa 2 to infinity, but with ω 2 (a − a s ) 2 to a s . As will turn out later in section 3.4.3, in the presence of matter a cosmological constant reappears because the time dependent [4] Newton constant (17) implies a time dependent matter contribution to the cosmological constant [8,9,10].…”
Section: Spring Modelmentioning
confidence: 95%
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“…It may be stressed that I have noch undertaken to calculate the couplings J and K in terms of the 12-dimensional V 1 and V 3 exchange integrals as defined in (17) and (16). What is done here, is to use the J and K as free parameters and calculate the masses of the excitations in terms of these couplings.…”
Section: Dzyaloshinskii Masses For the Heavy Family; Heisenberg Masse...mentioning
confidence: 99%