Abstract

We study gravitational particle production of the massive spin-$3/2$ Rarita-Schwinger field, and its close relative, the gravitino, in Friedmann-Robertson-Walker cosmological spacetimes. For masses lighter than the value of the Hubble expansion rate after inflation, ${m}_{3/2}\ensuremath{\lesssim}H$, we find catastrophic gravitational particle production, wherein the number of gravitationally produced particles is divergent, caused by a transient vanishing of the helicity-$1/2$ gravitino sound speed. In contrast with the conventional gravitino problem, the spectrum of produced particles is dominated by those with momentum at the UV cutoff. This suggests a breakdown of effective field theory, which might be cured by new degrees of freedom that emerge in the UV. We study the UV completion of the Rarita-Schwinger field, namely $\mathcal{N}=1$, $d=4$, supergravity. We reproduce known results for models with a single superfield and models with an arbitrary number of chiral superfields, find a simple geometric expression for the sound speed in the latter case, and extend this to include nilpotent constrained superfields and orthogonal constrained superfields. We find supergravity models where the catastrophe is cured and models where it persists. Insofar as quantizing the gravitino is tantamount to quantizing gravity, as is the case in any UV completion of supergravity, the models exhibiting catastrophic production are prime examples of four-dimensional effective field theories that become inconsistent when gravity is quantized, suggesting a possible link to the swampland program. We propose the gravitino swampland conjecture, which is consistent with and indeed follows from the Kachru-Kallosh-Linde-Trivedi and large volume scenarios for moduli stabilization in string theory.

Highlights

  • Gravitational particle production (GPP) is ubiquitous in quantum field theories in curved spacetime

  • In the spirit of effective field theory, one might hope that the catastrophic particle production exhibited by the RaritaSchwinger model with m ≲ He would be cured by UV completion

  • In this work we have considered the dynamics of massive spin-3=2 fields in curved spacetime

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Summary

INTRODUCTION

Gravitational particle production (GPP) is ubiquitous in quantum field theories in curved spacetime. Note that the additional fermionic degrees of freedom in supergravity, which allow the helicity-1=2 gravitino to decay, and the identification of the gravitino as a linear combination of spin-1=2 fermions that may change with time does not ameliorate the breakdown of effective field theory that defines catastrophic production This is in contrast with the conventional gravitino problem (for example [56]), where the EFT is valid at all times (unlike the catastrophe), and where the changing identity of the gravitino can significantly amelioriate the problem [57,58] (see [59] in the context of orthogonal constrained superfield supergravity models). Our sign conventions correspond to ð−; þ; þÞ in their table

RARITA-SCHWINGER MODEL IN MINKOWSKI SPACETIME
RARITA-SCHWINGER MODEL IN A FRIEDMANN-ROBERTSON-WALKER BACKGROUND
Action and field equations
Constraints
Fourier decomposition and mode equations
Helicity eigenspinors
Quantization
CATASTROPHIC GRAVITATIONAL PARTICLE PRODUCTION
Initial conditions and particle number spectrum
Catastrophic particle production-numerical results
Conditions for a vanishing sound speed
Nonadiabatic particle production from vanishing sound speed
THE SITUATION IN SUPERGRAVITY
Models with a single chiral superfield
Models with multiple chiral superfields
Nilpotent superfield models
Orthogonal constrained superfield models
Corrections to the Kähler potential
THE GRAVITINO SWAMPLAND CONJECTURE
DISCUSSION AND CONCLUSIONS

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