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Standard Model Background of the Cosmological Collider

Xingang Chen, Yi Wang, Zhong-Zhi Xianyu

TL;DR

The standard model background of the cosmological collider is described, a prerequisite to understand the background signals from the particle physics standard model to explore any new physics at very high scales.

Abstract

The inflationary universe can be viewed as a "Cosmological Collider" with energy of Hubble scale, producing very massive particles and recording their characteristic signals in primordial non-Gaussianities. To utilize this collider to explore any new physics at very high scales, it is a prerequisite to understand the background signals from the particle physics Standard Model. In this paper we describe the Standard Model background of the Cosmological Collider.

Standard Model Background of the Cosmological Collider

TL;DR

The standard model background of the cosmological collider is described, a prerequisite to understand the background signals from the particle physics standard model to explore any new physics at very high scales.

Abstract

The inflationary universe can be viewed as a "Cosmological Collider" with energy of Hubble scale, producing very massive particles and recording their characteristic signals in primordial non-Gaussianities. To utilize this collider to explore any new physics at very high scales, it is a prerequisite to understand the background signals from the particle physics Standard Model. In this paper we describe the Standard Model background of the Cosmological Collider.

Paper Structure

This paper contains 12 equations, 2 figures.

Figures (2)

  • Figure 1: The mass spectrum of Standard Model during inflation. The left three columns correspond the non-Higgs inflation with zero Higgs VEV, and Higgs masses are chosen to be $(0.05,0.5,5)H$, respectively. The rightmost column corresponds to the original Higgs inflation model.
  • Figure 2: The diagram contributing to the squeezed limit of the bispectrum with SM loop. The $\Phi$ field represents any of SM fields.