Gedankerexperiment, assuming nonsingular quantum bounce Friedman Equations leading to a causal discontinuity between Pre Planckian to Planckian physics Space-Time regime

come up with restraints which are in line with modifications of the Friedman equation in a quantum bounce, with removal of the Penrose theorem initial singularity. In line with super negative pressure being applied, so as to understand what we can present as far as H = 0 ( quantum bounce) in terms of density of the Universe. And also considering what to expect when ~ ( 1 ) P w          . I.e. we have a negative energy density in Pre Planckian space-time. This leads to a causal discontinuity between Pre Planckian to Planckian space-time due to the sign of the inflaton changing from minus to positive, for reasons brought up in this manuscript. i.e. looking at Eq. (9) , Eq. (10) and Eq. (11) of this document, with explanations as to what is going on physically.


Introduction .
We will here, in Equations 9 and 10 and 11 of the following document, outline the point of the document. I.e. a change in inflaton field, from a 'negative' to a 'positive' field contribution, leading to a counter intuitive result, namely that there would be a causal barrier when the inflaton field would vanish in the denominator of the derived energy density expression , about at the boundary between Pre Planckian to Planckian space-time physics. The rest of the paper will be to explain the reasons for this startling model and its possible implications.

Setting up the template for the vanishing of the inflaton in the boundary between Pre Planckian Space-time to Planckian Space-time
We Which when this is set equal to zero, at the time of a quantum bounce for a non singular universe, with 2 2 This Eq.(2) will have a modification of the density along the lines of   We also will be examining the influence of [3]   With here as given by [4]   Our task will be to be looking at what this becomes with Eq. (4) put into Eq. (2) when   The term for pressure we will be using is, then from [5] ~( 1 ) Then, we will be looking at Eq. (2) written as Or then, if we use [2]   We get in the regime of Pre Planckian physics, the situation that we would have In the regime of boundary between Pre Plankian to Planckian physics, we would have, instead What will be examined, in this document will be what we will be considering i.e. when the bracket in the ln expression approaches zero, namely The terms Visc, 2 init a and 2 int H will be considered to be invariant in the area of the surface of the spherical (?) regime for where we have our analysis as to what this causal discontinuity implies, and why. This will be an addition to [4] and its analysis of space-time dynamics.

Causal discontinuity and what it may be
implying.
In reference [5] we have a condition for which there is an extraordinarily rapid change in the value of the derivative of the inflation, namely, an argument for which we have In so many words, we believe that the dynamics of Eq. (11) as it applies to Eq. (9) and Eq. (10) fit this bill and also add, perforce a way as to confirm the existence of such behavior.

Examination of the Causal structure, as implied by Fay Dowker, and what we are saying replaces it.
With the initial Hubble parameter, in this situation a constant value in the Pre Planckian regime of space-time, instead of the usual Hubble H a a  (13) Also, visc in Eq. (1) is for a viscous "fluid" approximation in a non-singular regime of space-time namely, that we have initially due to [4] and the proportionality of energy to Boltzman's constant times temperature [4] 2ĩ nitial tt initial tt B initial At about this time interval, and beyond, we are examining 2 init a as given by [6] and also, the minimum scale factor has a factor of  which we interpret as todays value of the cosmological constant. B is the early cosmological B field , the To get to the bottom of what this is implying as far as causal structure and how we modify it, we will be examining what Dowker brought up in [7], namely that she is assuming that there is no breakage as to what the causal interpolation of space time dynamics, to which we say, stuff and nonsense. However, we would be looking to preserve enough information exchange between physical domains in the prior to the present universe, as to preserve the operational continuity of physical law. As will be discussed in the conclusion. actually give us a clue as to how this is possible. I.e. to use , due to the brevity of time interval, the equivalent of quantum teleportation between both sides of the causal barrier, to insure continuity of physical processes, along the lines of [9] . Note that we are doing this even while maintaining fidelity with respect to [10] In other words, only enough information between both sides of the causal barrier would be swapped as to insure the continuity of physical processes, and this would be commensurate with an inquiry as to issues we will bring up next. This also is the same condition for which we would have to have visc, i.e. the viscosity of the initial spherical starting point for expansion, nonzero as well as reviewing the issues as of [11,12,13,14,15] Whereas how we do it may allow for the Corda references, [12,14] to be experimentally investigated. Finally the Abbot articles of [13,15] must be adhered to

Acknowledgements
This work is supported in part by National Nature Science Foundation of China grant No. 11375279