“…When there is a single term on the right-hand side of the cooling equation for the temperature difference θ ≡ T − T ∞ , the analogous FLRW universe filled with a single perfect fluid, and ruled by the Friedmann equation 16, is spatially flat. In this case, the Einstein-Friedmann equations enjoy certain symmetries [10][11][12], which are studied in the cosmological literature, mostly in relation with solution-generating techniques [10][11][12][13][14][15][16][17]. In these symmetry transformations, one rescales time t, scale factor a, or Hubble function H and changes barotropic fluid appropriately, leaving the Einstein-Friedmann equations invariant.…”