Abstract

Using a Linde reference, as well as another one from Padmanabhan for calculation of how the early universe expands, we obtain, by default the coefficient of scale factor expansion, t to the alpha value, with alpha being approximately the square root of five in value. We from there make an estimate as to the number of initial particles produced in the very beginning, which leads us to conclude that a graviton, would be a preferred initial by product. The argument as to gravitons, also reflects a choice of how the decay of initial BEC condensates of Planck sized black holes would commence, using the work produced by Chavanis, as to BEC condensates and black holes. The object will be to obtain initial frequency spread plus strength of GW production plus a suggestion as to what polarization state may be accessible from initial conditions.

Highlights

  • We use the work by Linde, [1] as to what is given on page 257 which translates into a different model of the Hubble expansion H2 = 2 p ⋅ φ 2 2 +V (φ ) − H2 M2 ⋅ H 2 +

  • The argument as to gravitons, reflects a choice of how the decay of initial BEC condensates of Planck sized black holes would commence, using the work produced by Chavanis, as to BEC condensates and black holes

  • We show that fragmentation of the inflaton into long-lived spatially localized oscillon configurations can lead to copious production of black holes

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Summary

Introduction

Scalar-Tensor Gravity, BEC, Scale Factor, Massive Gravitons We will elaborate upon the implications of this in the third chapter of this paper after we go to asking if we construct a minimum value of the inflaton mass which we will try relating to formation of early universe Planck mass black holes.

Results
Conclusion

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