Approximate de Sitter symmetry of inflating Universe is responsible for the approximate flatness of the power spectrum of scalar perturbations. However, this is not the only option. Another symmetry which can explain nearly scale-invariant power spectrum is conformal invariance. We give a short review of models based on conformal symmetry which lead to the scale-invariant spectrum of the scalar perturbations. We discuss also potentially observable features of these models.Observational data show that primordial scalar perturbations in the Universe must have been generated at some early cosmological stage, preceding the hot epoch. They are nearly Gaussian and have nearly flat power spectrum [1]. The first property suggests that these perturbations originate from amplified vacuum fluctuations of weakly coupled quantum field(s). Indeed, the defining property of Gaussian random field ζ(x) is that it obeys the Isserlis-Wick theorem, which holds also for any free quantum field in its vacuum state, while linear evolution in classical background does not induce non-Gaussianity.The second property is also very suggestive. The power spectrum P(k) defined asgives the fluctuation in logarithmic interval of momenta,where n s is a spectral index. The flat or scale invariant spectrum corresponds to n s = 1. In early 70's Harrison, Zeldovich and Peebles and Yu [2] conjectured that the spectrum is flat, to avoid large deviation from homogeneity and isotropy of the observed Universe on large scales and black hole formation on small scales. Current observational data [1] show that the power spectrum is indded nearly flat and give n s − 1 ≈ −0.032. The flatness of the power spectrum may be due to some symmetry. The best known candidate is the symmetry SO(4, 1) of the de Sitter metric ds 2 = 1)