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Differential equations and recursive solutions for cosmological amplitudes
A bstract Recently considerable efforts have been devoted to computing cosmological correlators and the corresponding wavefunction coefficients, as well as understanding their analytical structures. In this note, we revisit the computation of these “cosmological amplitudes” associated with any tree...
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Published in: | The journal of high energy physics 2025-01, Vol.2025 (1), p.1-43, Article 1 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | A
bstract
Recently considerable efforts have been devoted to computing cosmological correlators and the corresponding wavefunction coefficients, as well as understanding their analytical structures. In this note, we revisit the computation of these “cosmological amplitudes” associated with any tree or loop graph for conformal scalars with time-dependent interactions in the power-law FRW universe, directly in terms of iterated time integrals. We start by decomposing any such cosmological amplitude (for loop graph, the “integrand” prior to loop integrations) as a linear combination of
basic time integrals
, one for each
directed graph
. We derive remarkably simple first-order differential equations involving such time integrals with edges “contracted” one at a time, which can be solved recursively and the solution takes the form of Euler-Mellin integrals/generalized hypergeometric functions. By combining such equations, we then derive a complete system of differential equations for all time integrals needed for a given graph. Our method works for any graph: for a tree graph with
n
nodes, this system can be transformed into the
canonical differential equations
of size 4
n
−1
equivalent to the graphic rules derived recently , and we also derive the system of differential equations for loop integrands e.g. of all-loop two-site graphs and one-loop
n
-gon graphs. Finally, we show how the differential equations truncate for the de Sitter (dS) case (in a way similar to differential equations for Feynman integrals truncate for integer dimensions), which immediately yields the complete symbol for the dS amplitude with interesting structures e.g. for
n
-site chains and
n
-gon cases. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP01(2025)001 |