On the renormalization of the effective field theory of large scale structures
By E. Pajer, M. Zaldarriaga. 2013
148 citations recorded by the source corpus.
Standard perturbation theory (SPT) for large-scale matter inhomogeneities is unsatisfactory for at least three reasons: there is no clear expansion parameter since the density contrast is not small on all scales; it does not fully account for deviations at large scales from a perfect pressureless fluid induced by short-scale non-linearities; for generic initial conditions, loop corrections are UV-divergent, making predictions cutoff dependent and hence unphysical. The Effective Field Theory of Large Scale Structures successfully addresses all three issues. Here we focus on the third one and show explicitly that the terms induced by integrating out short scales, neglected in SPT, have exactly the right scale dependence to cancel all UV-divergences at one loop, and this should hold at all loops. A particularly clear example is an Einstein deSitter universe with no-scale initial conditions Pin ~ kn. After renormalizing the theory, we use self-similarity to derive a very simple result for the final power spectrum for any n, excluding two-loop corrections and higher. We show how the relative importance of different corrections depends on n. For n ~ −1.5, relevant for our universe, pressure and dissipative corrections are more important than the two-loop corrections.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/04a8272887b31e9905a7b1fdaafa3c97f79a0cdc
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Citations in the corpus
- Renormalized halo bias (2014, methodology): “In the case of a scaling universe with P (q) ∝ qn, the finite part of F can be computed analytically using dimensional regularization [22]”
- Limits on wCDM from the EFTofLSS with the PyBird code (2020, methodology): “These calculations were accompanied by some theoretical developments of the EFTofLSS, such as a careful understanding of renormalization [8, 20, 21] (including rather-subtle aspects such as lattice-running [8] and a better understanding of the velocity field [10, 22]), of the several ways for extrac”
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- On the statistics of biased tracers in the Effective Field Theory of Large Scale Structures (2015, background): “The Effective Field Theory of Large Scale Structures (EFTofLSS) [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16] is a theoretical framework that aims at developing a rigorous analytic understanding of the clustering of LSS, through a perturbative expansion in the size of the fluctuations.”
- The Effective Field Theorist's Approach to Gravitational Dynamics (2016, background): “On the other hand, the (renormalized) N -loop order in perturbation theory scales as [352, 354]”
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- The IR-resummed Effective Field Theory of Large Scale Structures (2014, methodology): “The fact that modes larger and smaller than k affect the power spectrum through different parameters is what allows SPT to be nondivergent for equal time correlators power law Universes in the range −3 < n < −1.”
- Biased Tracers in Redshift Space in the EFT of Large-Scale Structure (2016, background): “years the Effective Field Theory of Large-Scale Structure 1 (EFTofLSS) [2, 3, 4, 5] has provided a tool where predictions in the mildly non-linear regime can be delivered with an at-least-in-principle arbitrary theoretical precision, and most probably with a precision that should be enough for next ”
- The Lagrangian-space Effective Field Theory of large scale structures (2013, methodology): “As it was discussed in [7, 12], this is related to the UV divergences in the one-loop computations, that occur for n ≥ −1 when we remove the cutoff of the theory.”