Abstract
Scattering amplitudes at weak coupling are highly constrained by Lorentz invariance, locality and unitarity, and depend on model details only through coupling constants and the particle content of the theory. For example, four-particle amplitudes are analytic for contact interactions and have simple poles with appropriately positive residues for tree-level exchange. In this paper, we develop an understanding of inflationary correlators which parallels that of flat-space scattering amplitudes. Specifically, we study slow-roll inflation with weak couplings to extra massive particles, for which all correlation functions are controlled by an approximate conformal symmetry on the boundary of the spacetime. After systematically classifying all possible contact terms in de Sitter space, we derive an analytic expression for the four-point function of conformally coupled scalars mediated by the tree-level exchange of massive scalars. Conformal symmetry implies that the correlator satisfies a pair of differential equations with respect to spatial momenta, encoding bulk time evolution in purely boundary terms. The absence of unphysical singularities (and the correct normalization of physical ones) completely fixes this correlator. Moreover, a “spin-raising” operator relates it to the correlators associated with the exchange of particles with spin, while “weight-shifting” operators map it to the four-point function of massless scalars. We explain how these de Sitter four-point functions can be perturbed to obtain inflationary three-point functions. Using our formalism, we reproduce many classic results in the literature, such as the three-point function of slow-roll inflation, and provide a complete classification of all inflationary three- and four-point functions arising from weakly broken conformal symmetry. Remarkably, the inflationary bispectrum associated with the exchange of particles with arbitrary spin is completely characterized by the soft limit of the simplest scalar-exchange four-point function of conformally coupled scalars and a series of contact terms. Finally, we demonstrate that the inflationary correlators contain flat-space scattering amplitudes via a suitable analytic continuation of the external momenta, which can also be directly connected with the signals for particle production seen in the squeezed limit.
Highlights
Cosmology is famously an observational rather than an experimental science
A “spin-raising” operator relates it to the correlators associated with the exchange of particles with spin, while “weight-shifting” operators map it to the four-point function of massless scalars
In appendix E, we introduce a set of weight-shifting operators that allow us the bootstrap the solutions for massless external fields from those for conformally coupled fields. appendix F contains a few useful identities for the hypergeometric functions, and appendix G collects important variables used in the paper
Summary
Cosmology is famously an observational rather than an experimental science. No experimentalists were present in the early universe, and the experiment of the birth and subsequent evolution of the universe cannot be repeated. The character of the “cosmological bootstrap” that we pursue in this paper is closer in spirit to its modern incarnation in scattering amplitudes, striving to use a simplified analytic structure for correlators in perturbation theory, together with symmetries and singularities, to fully determine the final answer without reference to bulk time evolution. Equation (3.36) is the solution for the four-point function of conformally coupled scalars arising from the exchange of a massive scalar This provides the fundamental building block from which all other correlators are derived by spin-raising and weightshifting operators. We will often denote them by sflat and tflat to avoid confusion with s ≡ |k1 + k2| and t ≡ |k2 + k3|, which we employ for the exchange momenta in cosmological correlators
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