Abstract

In this work we study vacuum decay and bubble nucleation in models of $f(R)$ higher curvature gravity. Building upon the analysis of Coleman-De Luccia (CDL), we present the formalism to calculate the Euclidean action and the bounce solution for a general $f(R)$ gravity in the thin wall approximation. We calculate the size of the nucleated bubble and the decay exponent for the Starobinsky model and its higher power extensions. We have shown that in the Starobinsky model with a typical potential the nucleated bubble has a larger size in comparison to the CDL bubble and with a lower tunneling rate. However, for higher power extension of the Starobinsky model the size of the bubble and the tunneling exponent can be larger or smaller than the CDL bubble depending on the model parameters. As a counterintuitive example, we have shown that a bubble with a larger size than the CDL bubble but with a higher nucleation rate can be formed in $f(R)$ gravity.

Highlights

  • Tunneling is a quantum mechanical phenomenon which does not occur in classical physics

  • We studied the vacuum decay for a scalar field in fðRÞ gravity

  • The higher curvature terms are expected to appear in the effective theories of gravity in high energy physics

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Summary

INTRODUCTION

Tunneling is a quantum mechanical phenomenon which does not occur in classical physics. In a quantum system where ħ is not zero, uncertainty in the momentum causes the state of the system to become unstable This is true for all minima of the potential energy, except the lowest one which remains stable. Vacuum tunneling plays important roles in various physical theories. It is important for the standard model of particle physics since in the absence of new physics in higher energy scales, the vacuum of the Higgs boson can become unstable [1]. It is a well motivated question to study the effects of vacuum decay in early universe. One natural question is to study vacuum decay and bubble nucleation in modified theories of gravity.

VACUUM DECAY IN FLAT SPACETIME
EUCLIDEAN ACTION FOR f ðRÞ GRAVITY
DECAY EXPONENT IN THE THIN WALL LIMIT
Λ22 þ ðR2F2
CDL solution
EINSTEIN FRAME FORMULATION
SUMMARY AND DISCUSSIONS
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