Fig. I.2.

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Equation of state at a = 10−4 as a function of Q0/𝒵0 for the exponential 𝒦(Q) function for various masses m. This is for KB = 0.1, H0 = 70 km s−1 Mpc−1, and Ω0 = 0.25. The dotted gray line shows the upper bound from Ilić et al. (2021). We note that m2 is the prefactor of 𝒦(Q). Thus, both the density and the pressure are proportional to m2 and this prefactor cancels in w. The dependence on m shown here comes from the constraint that the density parameter today is Ω0.
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