http://arxiv.org/abs/1908.08785
We discuss the difference between various gauge-invariant quantities typically used in single-field inflation, namely synchronous $\zeta_s$, comoving $\zeta_c$, and unitary $\zeta_u$ curvatures. We show that conservation of $\zeta_c$ outside the horizon is quite restrictive on models as it leads to conservation of $\zeta_s$ and $\zeta_u$, whereas the reverse does not hold. We illustrate the consequence of these differences with two inflationary models: ultra-slow-roll (USR) and braiding-ultra-slow-roll (BUSR). In USR, we show that out of the three curvatures, only $\zeta_s$ is conserved outside the horizon, and we connect this result to the concepts of separate universe and the usage of the $\delta N$ formalism. We find that even though $\zeta_s$ is conserved, there is still a mild violation of the separate universe approximation in the continuity equation. Nevertheless, the $\delta N$ formalism can still be applied to calculate the primordial power spectrum of some gauge-invariant quantities such as $\zeta_u$, although it breaks down for others such as the uniform-density curvature. In BUSR, we show that both $\zeta_u$ and $\zeta_s$ are conserved outside the horizon, but take different values. Additionally, since $\zeta_u\not=\zeta_c$ we find that the prediction for observable curvature fluctuations after inflation does not reflect $\zeta_c$ at horizon crossing during inflation and moreover involves not just $\zeta_u$ at that epoch but also the manner in which the braiding phase ends.
M. Lagos, M. Lin and W. Hu
Tue, 27 Aug 19
12/85
Comments: N/A
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