Is there a Friedmann equation form with inflation?

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SUMMARY

The discussion centers on the existence of a Friedmann equation that incorporates a transition from the inflation era to subsequent eras, specifically radiation, matter, and dark energy. It is established that while such an equation may not exist in a straightforward form, general relativity (GR) effectively describes these transitions using the basic Friedmann equations, which relate energy density (ρ) and pressure (p). The transition involves a change in the equation of state from inflation's p = -ρ to radiation's p = ρ/3, indicating a discontinuous change in the parameters ΩΛ and Ωr. The 4 Ωs form is not suited for handling these discontinuities.

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Buzz Bloom
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TL;DR
I have been unable to find on the Internet any form of GR similar to the 4 Omegas Friedmann equation that includes a transition from an inflation era back to a radiation era. Is it known whether of not such a equation currently exists?
If it is known that such an equation exists, I would much appreciate seeing a link to a reference. If it is known that such an equation does not exist, I would much appreciate seeing a reference with an explanation of implications regarding the compatibility of general relativity with a transition from the inflation era to subsequent eras: radiation to matter to dark energy/cosmological constant.
 
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Buzz Bloom said:
I have been unable to find on the Internet any form of GR similar to the 4 Omegas Friedmann equation that includes a transition from an inflation era back to a radiation era.

That's probably because it's cumbersome, at best, to describe such a transition in the form you are talking about. It's easier to use the more basic form of the Friedmann equations in terms of the energy density ##\rho## and the pressure ##p##. The transition from inflation to radiation dominated involves a change in the equation of state that relates ##\rho## and ##p##, from the inflation era's equation ##p = - \rho## to the radiation dominated ##p = \rho / 3##. In terms of the 4 ##\Omega##s, that would mean a discontinuous change in at least two of the ##\Omega##s, ##\Omega_\Lambda## and ##\Omega_r## (the lambda and radiation ##\Omega##s), and the 4 ##\Omega##s form is not really set up to handle discontinuous changes like that.
 
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Buzz Bloom said:
the compatibility of general relativity with a transition from the inflation era to subsequent eras: radiation to matter to dark energy/cosmological constant.

General relativity can describe all of these transitions just fine.
 
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