Abstract

Fermionic terms in a class of locally supersymmetric theories called "liberated supergravity" are nonrenormalizable interactions proportional to inverse powers of the supersymmetry breaking scale and Planck mass. This property defines an intrinsic cutoff for liberated supergravities, which are therefore effective theories valid only below energies that never exceed the cutoff. Requiring that the cutoff exceeds current theoretical and observational bounds shows that the new scalar potential terms allowed by liberated supergravity can neither change the cosmological constant predicted by supergravity by any observable amount, nor give measurable contributions to particle masses. We show that it is nevertheless possible to define a simple liberated supergravity model of slow roll inflation valid up to energy scales that are well above the Hubble parameter during inflation and exceeds observable limits after inflation. The key to constructing a viable model is to change the supersymmetry breaking scale, from a Planck-scale value during inflation, to TeV-scale after inflation.

Highlights

  • Supergravity strongly constrains the form of the scalar potential [1], it makes the construction of specific models of elementary interactions or inflation challenging

  • The scalar potential of liberated supergravity need not be of the special form given in [1]; it is a completely general function of the scalar fields

  • As any other gravity theory, liberated supergravity contains nonrenormalizable interaction, so it is by construction an effective theory valid only up to a finite cutopffffiffiffitffihffiffiffiaffiffit cannot exceed the Planck scale Λcut ≲ 1= 8πG ≡ Mpl

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Summary

Constraining liberated supergravity

Fermionic terms in a class of locally supersymmetric theories called “liberated supergravity” are nonrenormalizable interactions proportional to inverse powers of the supersymmetry breaking scale and Planck mass Mpl. Fermionic terms in a class of locally supersymmetric theories called “liberated supergravity” are nonrenormalizable interactions proportional to inverse powers of the supersymmetry breaking scale and Planck mass Mpl This property defines an intrinsic cutoff for liberated supergravities, which are effective theories valid only below energies that never exceed the cutoff. Requiring that the cutoff exceeds current theoretical and observational bounds shows that the new scalar potential terms allowed by liberated supergravity can neither change the cosmological constant predicted by supergravity by any observable amount, nor give measurable contributions to particle masses. We show that it is possible to define a simple liberated supergravity model of slow roll inflation valid up to energy scales that are well above the Hubble parameter during inflation and exceeds observable limits after inflation.

INTRODUCTION
HUN JANG and MASSIMO PORRATI
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CONSTRAINING LIBERATED SUPERGRAVITY
UFW F W
PL χI
LK ðT
During inflation we demand that the initial supersymmetry breaking scale is
Note that
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