Abstract
Abstract
Scalars are widely used in cosmology to model novel phenomena such as the late-time cosmic
acceleration. These are effective field theories with highly nonlinear interactions, including
Horndeski theory/generalized galileon and beyond. We use the latest fully crossing symmetric
positivity bounds to constrain these cosmological EFTs. These positivity bounds, based on
fundamental principles of quantum field theory such as causality and unitarity, are able to
constrain the EFT coefficients both from above and below. We first map the mass dependence of the
fully crossing symmetric bounds, and find that a nonzero mass generically enlarges the positivity
regions. We show that fine-tunings in the EFT construction can significantly reduce the viable
regions and sometimes can be precarious. Then, we apply the positivity bounds to several models in
the Horndeski class and beyond, explicitly listing the ready-to-use bounds with the model
parameters, and discuss the implications for these models. The new positivity bounds are found to
severely constrain some of these models, in which positivity requires the mass to be
parametrically close to the cutoff of the EFT, effectively ruling them out. The examples include
massive galileon, the original beyond Horndeski model, and DHOST theory with unity speed of
gravity and nearly constant Newton's coupling.
Subject
Astronomy and Astrophysics
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