<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JHEPGC</journal-id><journal-title-group><journal-title>Journal of High Energy Physics, Gravitation and Cosmology</journal-title></journal-title-group><issn pub-type="epub">2380-4327</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jhepgc.2017.33038</article-id><article-id pub-id-type="publisher-id">JHEPGC-78084</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  How a Minimum Time Step Leads to a Causal Structure Used to Form Initial Entropy Production and High Frequency Gravitons, with 7 Subsequent Open Questions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Andrew</surname><given-names>Walcott Beckwith</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Physics Department, College of Physics, Chongqing University, Chongqing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>rwill9955b@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>06</month><year>2017</year></pub-date><volume>03</volume><issue>03</issue><fpage>493</fpage><lpage>502</lpage><history><date date-type="received"><day>March</day>	<month>20,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>July</month>	<year>28,</year>	</date><date date-type="accepted"><day>July</day>	<month>31,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  We start where we use an inflaton value due to use of a scale factor 
  <img src="Edit_78becbed-2b52-4baa-83aa-9d7638d63298.bmp" alt="" /> . Also we use 
  <img src="Edit_5d9f5afa-d023-4439-8bec-4a075d7eaea7.bmp" alt="" /> as the variation of the time component of the metric tensor in Pre-Planckian Space-time up to the Planckian spacetime initial values. In doing so, we come up with a polynomial expression for a minimum time step; we can call which leads to a development of the arrow of time. We show an inter relationship between the formation of the Arrow of time, and Causal structure, assuming the setting of H = 0 in the Friedman equation 
  This in turn leads to entropy production at the start of causal structure in the onset of inflation. This then leads to three and a quarter pages of 7 open questions we think have to be answered, subsequently. It is noted that high frequency gravitational waves as specified are due to the 1/delta t entry in Equation (45) of the document which comes out to about 44 Hertz, and certainly is high frequency gravitational waves for the initial cosmological conditions, so this is definitely about high frequency gravitational wave focused initial conditions.
 
</html></p></abstract><kwd-group><kwd>Inflaton Physics</kwd><kwd> Causal Structure Entropy</kwd><kwd> HFGW</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Examination of the Minimum Time Step, in Pre-Planckian Space-Time as a Root of a Polynomial Equation</title><p>We initiate our work, citing [<xref ref-type="bibr" rid="scirp.78084-ref1">1</xref>] to the effect that we have a polynomial equation for the formation of a root finding procedure for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x6.png" xlink:type="simple"/></inline-formula>, namely if</p><disp-formula id="scirp.78084-formula30"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x7.png"  xlink:type="simple"/></disp-formula><p>From here, we then cited, in [<xref ref-type="bibr" rid="scirp.78084-ref1">1</xref>] , using [<xref ref-type="bibr" rid="scirp.78084-ref2">2</xref>] , a criteria as to formation of entropy, i.e. if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x8.png" xlink:type="simple"/></inline-formula> is an invariant cosmological “constant” and if Equation (2) holds, we can use the existence of nonzero initial entropy as the formation point of an arrow of time.</p><disp-formula id="scirp.78084-formula31"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x9.png"  xlink:type="simple"/></disp-formula><p>In short, our view is that the formation of a minimum time step, if it satisfies Equation (2) which is a necessary and sufficient condition for the formation of an arrow of time, at the start of cosmological evolution, we have a necessary and sufficient condition for the initiation of an arrow of time. In other words, Equation (2) being non zero with a minimum time step, is necessary and sufficient for the formation of an arrow of time. The remainder of our article is focused upon the issues of a necessary and sufficient condition for causal structure being initiated, along the lines of Dowker, as in [<xref ref-type="bibr" rid="scirp.78084-ref3">3</xref>] .</p></sec><sec id="s2"><title>2. Considerations as to the Start of Causal Structure of Space-Time</title><p>In [<xref ref-type="bibr" rid="scirp.78084-ref1">1</xref>] , we make our treatment of the existence of causal structure, as given by writing its emergence as contingent upon having</p><disp-formula id="scirp.78084-formula32"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x10.png"  xlink:type="simple"/></disp-formula><p>We have assumed in writing this, that our initial starting point for which we can write a Friedman Equation with H = 0 is a finite, very small ball of space- time and that within this structure that the Friedman Equation follows the following conventions, namely</p><disp-formula id="scirp.78084-formula33"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x11.png"  xlink:type="simple"/></disp-formula><p>The relativistically correct Friedman equation assumes, that within the confines of the regime for where H = 0 that we write <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x12.png" xlink:type="simple"/></inline-formula> equal to zero; i.e. there is no effective curvature within the confines of Pre-Planckian Space-time and that we make the following assumptions, namely that satisfying Equation (3) above is contingent upon [<xref ref-type="bibr" rid="scirp.78084-ref4">4</xref>] where we are assuming that the volume is normalized to =1, i.e. Planck length is set equal to one.</p><disp-formula id="scirp.78084-formula34"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x13.png"  xlink:type="simple"/></disp-formula><p>i.e. the regime of where we have the initiation of causal structure, if allowed would be contingent upon the behavior of [<xref ref-type="bibr" rid="scirp.78084-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref7">7</xref>]</p><disp-formula id="scirp.78084-formula35"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x14.png"  xlink:type="simple"/></disp-formula><p>i.e. the right hand side of Equation (6) is the square of the scale factor, which we assume is ~10^-110, due to [<xref ref-type="bibr" rid="scirp.78084-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref6">6</xref>] , and an inflaton given by [<xref ref-type="bibr" rid="scirp.78084-ref8">8</xref>]</p><disp-formula id="scirp.78084-formula36"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x15.png"  xlink:type="simple"/></disp-formula><p>These are the items which were enfolded into the derivation of Equation (1) of reference [<xref ref-type="bibr" rid="scirp.78084-ref1">1</xref>] i.e. our following claim is that Causal structure commences if we can say the following,</p><disp-formula id="scirp.78084-formula37"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x16.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. So What Is the Root of Our Approximation for a Time Step?</title><p>Here for the satisfying of Equation (8) is contingent upon <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x17.png" xlink:type="simple"/></inline-formula> as an initial event horizon, of our bubble of space-time being of the order of magnitude of Planck Length, for the satisfaction of forming a regime of space time which may have causal structure as given by Dowker [<xref ref-type="bibr" rid="scirp.78084-ref3">3</xref>] , i.e. at the boundary of a space-time initial bubble [<xref ref-type="bibr" rid="scirp.78084-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref6">6</xref>] which may contravene the Penrose conjecture [<xref ref-type="bibr" rid="scirp.78084-ref9">9</xref>] as to initial singularities.</p><p>Furthermore, this is not incommensurate with what Penrose wrote himself in [<xref ref-type="bibr" rid="scirp.78084-ref10">10</xref>] , namely reviewing the Weyl Curvature hypothesis, as given in [<xref ref-type="bibr" rid="scirp.78084-ref10">10</xref>] , i.e. singularities as presumed in initial space-time are very different from singularities of black holes, and that modification of the Weyl curvature hypothesis, may be allowing for what Penrose referred to as gravitational clumping initially to boost the initial entropy, above a presumed initial value. i.e. this we believe is commensurate with Equation (2) above, and is crucially important.</p><p>We close this inquiry by noting that what we have done is also conditional upon [<xref ref-type="bibr" rid="scirp.78084-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref12">12</xref>] to the effect that we can write the genesis of our time step formula, as given by Equation (1) above as crucially dependent upon, the following</p><disp-formula id="scirp.78084-formula38"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x18.png"  xlink:type="simple"/></disp-formula><p>In the third line of Equation (9) the essential substitution is to go from a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula> in the Newtonian case where we have the universe as bounded if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x20.png" xlink:type="simple"/></inline-formula> in a gravitational sense, or unbounded in a gravitational sense, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x21.png" xlink:type="simple"/></inline-formula> to the question of, in relativity of negative curvature, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x22.png" xlink:type="simple"/></inline-formula>or positive curvature, with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x23.png" xlink:type="simple"/></inline-formula>. Here what we do, in our own adaptation of Equation (9) is to realize that the Newtonian case involves the conservation of energy for an expanding universe, while we conflate the 2<sup>nd</sup> and 3<sup>rd</sup> relativistic case involves changing from a mass density, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x24.png" xlink:type="simple"/></inline-formula>, by an energy Density, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x25.png" xlink:type="simple"/></inline-formula>which is a generalized version of what we are attempting to analyze.</p><p>So, in the Pre Planckian regime of Space-time, our initial assumption is twofold, i.e. we assume that we cannot reference either <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x26.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x27.png" xlink:type="simple"/></inline-formula>. The default choice we will pick is, in the Pre Planckian space-time to simplify our analysis, is to then set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x28.png" xlink:type="simple"/></inline-formula>. And then we will re image the energy density which will then be in conjunction with a revitalized version of a modified early universe version of the Heisenberg Uncertainty principle.</p></sec><sec id="s4"><title>4. Links to Entropy Production</title><p>We claim that what we are doing is contingent upon having<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x29.png" xlink:type="simple"/></inline-formula>, with a specified time step, and this at the boundary of H = 0, as a precursor for forming a causal structure i.e. this will enable us to make full sense out of Equation (9) provided, that within the pre Planckian space-time we have what appears to be paradoxical, i.e. a NEGATIVE energy density, but this consistent with having a negative energy density prior to the Causal barrier, of H = 0. The type of causal set was designated a Conformal causal set, by L. Crowell, [<xref ref-type="bibr" rid="scirp.78084-ref13">13</xref>] whom reviewed an earlier version of this document in the FQXI contest, sans the explicit reference to entropy. Also, we claim that our mixing of entropy and causal structures is an early universe take off of the following document which initially was for black holes, but which we claim is relevant for Pre Planckian structure [<xref ref-type="bibr" rid="scirp.78084-ref14">14</xref>] , but in doing so we make use of the following thought experiment as to forming entropy, gravitons and the like from the following use of H = 0</p><disp-formula id="scirp.78084-formula39"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x30.png"  xlink:type="simple"/></disp-formula><p>The key to this development is accessing the negative energy density in pre Planckian space-time , which if one crosses a causal barrier at H = 0, having this initial energy density, in Pre Causal space-time as negative, which once past the Causal barrier becomes positive, whereas the magnitude of the initial energy would be set at</p><disp-formula id="scirp.78084-formula40"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x31.png"  xlink:type="simple"/></disp-formula><p>In doing so, we have the mass if a graviton is specified as in [<xref ref-type="bibr" rid="scirp.78084-ref15">15</xref>] . And then the open question to be asked is, do we have in this case a situation where say the gravitons act as information carriers from a prior universe? Our intuition says yes, and we will follow up upon this with necessary and sufficient conditions for cyclic universe interpretations of this model, in a future publication.</p><p>In this case, the mass of a graviton, would be of the order of 10^−62 grams, which would specify, then a very small initial energy if we have that we are also using the Ng approximation for infinite quantum statistics of [<xref ref-type="bibr" rid="scirp.78084-ref16">16</xref>]</p><disp-formula id="scirp.78084-formula41"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x32.png"  xlink:type="simple"/></disp-formula><p>As well as an initial frequency of the “particles” given by</p><disp-formula id="scirp.78084-formula42"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x33.png"  xlink:type="simple"/></disp-formula><p>We also claim, that this procedure, is in its own way tandem with [<xref ref-type="bibr" rid="scirp.78084-ref17">17</xref>] which in turn has another “bubble” in the start of space-time.</p><p>We furthermore claim that additional development of this methodology will entail use of reconciling this work with page 428 of Baez, and Muniain, [<xref ref-type="bibr" rid="scirp.78084-ref18">18</xref>] , specifically as an alternative to the well-researched section on Canonical quantization, used in ADM relativity i.e. what we are doing is by default coming up with an alternative to what has been done in [<xref ref-type="bibr" rid="scirp.78084-ref18">18</xref>] and other places, as well as making a semi classical linkage to gravitons and entropy.</p></sec><sec id="s5"><title>5. Seven Open Questions, Which Remain to Be Answered</title><p>To close this section, one of the remaining problems which have to be addressed in this methodology is to address what was brought up by Tolman, [<xref ref-type="bibr" rid="scirp.78084-ref19">19</xref>] , i.e. if we have a cyclical universe that from each cyclical “bounce”, from cycle to cycle, entropy will increase especially at the beginning.</p><p>Our Causal structure argument has to be tweaked in order to avoid this development, which will be a topic of a future publication i.e. we need to have exact referencing of a nonzero, but not incrementally increasing initial entropy, per start of a cosmological cycle.</p><p>The final set up of our problem will also entail the use of, also reconciling the H = 0 structure of the Causal structure boundary, with what is given for the initial expansion of the Universe as given by [<xref ref-type="bibr" rid="scirp.78084-ref20">20</xref>] , i.e.</p><disp-formula id="scirp.78084-formula43"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x34.png"  xlink:type="simple"/></disp-formula><p>Here, the term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x35.png" xlink:type="simple"/></inline-formula> is for degrees of freedom of the universe, which is usually of the order of 100, [<xref ref-type="bibr" rid="scirp.78084-ref21">21</xref>] but the author got figures in the ballpark of about 1000, in [<xref ref-type="bibr" rid="scirp.78084-ref22">22</xref>] . Needless to state, with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x36.png" xlink:type="simple"/></inline-formula> being an enormous value, and the mass scale being less than or equal to Planck’s mass, the question of what causes a perturbation from H = 0 to Equation (14) needs to be addressed i.e. do we have to say that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x37.png" xlink:type="simple"/></inline-formula> was initially zero, and then obtained an enormous value?</p><p>Last but not least, is that we have in our pre causal Pre Planckian structure,</p><disp-formula id="scirp.78084-formula44"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x38.png"  xlink:type="simple"/></disp-formula><p>What values of the Cosmological constant are we assuming in the Pre Planckian to Planckian Universe transition?</p><p>Either it is of the sort where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x39.png" xlink:type="simple"/></inline-formula> remains invariant, or else we have to say [<xref ref-type="bibr" rid="scirp.78084-ref23">23</xref>]</p><disp-formula id="scirp.78084-formula45"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x40.png"  xlink:type="simple"/></disp-formula><p>This has to be worked out, for the obvious reasons, as well as looking at, if we have an iterative process for the generation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x41.png" xlink:type="simple"/></inline-formula> along the lines of looking at an iterative dynamical systems mapping, i.e. a chaotic map driven increase in degrees of freedom from a low point to a high point with vacuum thermal energy initially tied to [<xref ref-type="bibr" rid="scirp.78084-ref22">22</xref>]</p><disp-formula id="scirp.78084-formula46"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x42.png"  xlink:type="simple"/></disp-formula><p>Not only this, we should also consider if we are looking at massive gravitons, an analytical bridge between Pre Planckian representations of Gravitons and the following Planckian, to post Planckian space-time physics as given by a regime of space-time where we go from close to zero, or initially zero Pre Planckian space-time temperatures, to the super-hot initial conditions of inflation, i.e. note that as given by Giovanni, the figure of 10<sup>88</sup> as due to gravitons can be seen to come from [<xref ref-type="bibr" rid="scirp.78084-ref5">5</xref>] , page 156 as</p><disp-formula id="scirp.78084-formula47"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x43.png"  xlink:type="simple"/></disp-formula><p>There are two questions which this raises: What would be the driving impetus to go from a low temperature pre space time temperature, then to Planck time entropy, then to the entropy of today as given in Equation (18)?</p><p>One way to look at it would be to suggest as done by H. Kadlecova [<xref ref-type="bibr" rid="scirp.78084-ref24">24</xref>] in the 12 Marcel Grossman meeting the typical energy stress tensor, using, instead, Gyratons, with an electro-magnetic energy density addition to effective Electromagnetic cosmological value as given by</p><disp-formula id="scirp.78084-formula48"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x44.png"  xlink:type="simple"/></disp-formula><p>i.e. that there be, due to effective E and M fields, a boost from an initially low vacuum energy to a higher ones, as given by Kadlecova [<xref ref-type="bibr" rid="scirp.78084-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref25">25</xref>]</p><disp-formula id="scirp.78084-formula49"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x45.png"  xlink:type="simple"/></disp-formula><p>How would Equation (25) is used in Equation (11) to Equation (15) affect our Pre Planckian to Planckian physics results? This needs to be considered.</p><p>Last but not least, if we are considering massive gravitons, we should look at the following perturbative terms added to a metric tensor by massive gravitons. I.e. understand the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x46.png" xlink:type="simple"/></inline-formula> values as influenced by massive gravitons. As read from Beckwith [<xref ref-type="bibr" rid="scirp.78084-ref26">26</xref>] we get excessive nonlinearity, and the equations of perturbation of the metric tensor are given by the following treatment by Hinterbichler [<xref ref-type="bibr" rid="scirp.78084-ref27">27</xref>] , if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x47.png" xlink:type="simple"/></inline-formula>, and we look at a mass induced <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x48.png" xlink:type="simple"/></inline-formula> suppression factor put in of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x49.png" xlink:type="simple"/></inline-formula>, with m perhaps the mass of a massive graviton, and M say Planck’s mass then</p><disp-formula id="scirp.78084-formula50"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x50.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78084-formula51"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x51.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78084-formula52"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x52.png"  xlink:type="simple"/></disp-formula><p>Here, we have that these are solutions to the following equation, as given by [<xref ref-type="bibr" rid="scirp.78084-ref27">27</xref>]</p><disp-formula id="scirp.78084-formula53"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x53.png"  xlink:type="simple"/></disp-formula><p>So the question remains how to be bridge Equation (23) and Equation (24) to the massive graviton conditions we are considering for Pre Planckian space- time? Clearly, Equation (23) and Equation (24) are for Planckian to Post Planckian space-time physics.</p><p>Here, we are assuming for Equation (23) and Equation (24)</p><disp-formula id="scirp.78084-formula54"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x54.png"  xlink:type="simple"/></disp-formula><p>And use the value of the radius of the universe, as given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x55.png" xlink:type="simple"/></inline-formula>, and rather than a super partner Gravitino, use the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x56.png" xlink:type="simple"/></inline-formula>.</p><p>How do they get bridged to the Pre Planckian regime?</p><p>One possible benefit, if we get this matter of information theory and entropy settled i.e. does the following make sense?</p><p>In an earlier document the author submitted to FQXI, in 2012, the author tried to make the following linkage between presumed super partners (SUSY), in the electroweak regime of space-time, and the mass of non-super partner particles i.e. in 2012, the supposition was that</p><disp-formula id="scirp.78084-formula55"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2180206x57.png"  xlink:type="simple"/></disp-formula><p>In an earlier document, the idea was to make a bridge between presumed total mass of Gravitinos, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x58.png" xlink:type="simple"/></inline-formula>, in the electroweak era with their counterpart in</p><p>Gravitons, today, which we called,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x59.png" xlink:type="simple"/></inline-formula>. In Equation (26), we also</p><p>had <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x60.png" xlink:type="simple"/></inline-formula> being the presumed radius of the universe in the electroweak era, with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2180206x61.png" xlink:type="simple"/></inline-formula> the radius of the universe “today”.</p><p>Equation (26) was a presumed “conservation law”.</p><p>The problem, in all this, is that there is still not definitive evidence of super partners in CERN! Nor may there ever be found either! Can we, then if we abandon the idea of super partners, come up with a bridge between Pre Planckian to Planckian physics, using gravitons, along the lines of Equation (26)? This requires a review, of the issues, brought up in [<xref ref-type="bibr" rid="scirp.78084-ref28">28</xref>] , and to see if they are necessary.</p><p>We should note in passing that [<xref ref-type="bibr" rid="scirp.78084-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.78084-ref31">31</xref>] are important considerations, with [<xref ref-type="bibr" rid="scirp.78084-ref29">29</xref>] giving the details of gravitational wave detection, as noted by LIGO in 2016. [<xref ref-type="bibr" rid="scirp.78084-ref30">30</xref>] Confirms the essence of scalar tensor theories as a competitor to General Relativity which should be falsified, if possible, and [<xref ref-type="bibr" rid="scirp.78084-ref31">31</xref>] goes into more of massive body generation of gravitational waves which certainly is appropriate here in the early universe.</p><p>With that the questions are laid out for review and consideration.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work is supported in part by National Nature Science Foundation of China Grant No. 11375279.</p></sec><sec id="s7"><title>Cite this paper</title><p>Beckwith, A.W. (2017) How a Minimum Time Step Leads to a Causal Structure Used to Form Initial Entropy Production and High Frequency Gravitons, with 7 Subsequent Open Questions. Journal of High Energy Physics, Gravitation and Cosmology, 3, 493-502. https://doi.org/10.4236/jhepgc.2017.33038</p></sec></body><back><ref-list><title>References</title><ref id="scirp.78084-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Beckwith, A. How a Minimum Time Step Based in Pre Planckian Space-Time If Friedman Equation H Set Equal to Zero Leads to the Arrow of Time.  
http://vixra.org/abs/1702.0290</mixed-citation></ref><ref id="scirp.78084-ref2"><label>2</label><mixed-citation publication-type="book" xlink:type="simple">Keifer, C. (2012) Can the Arrow of Time Be Understood from Quantum Cosmology? In: Mersini-Houghton, L. and Vaas, R., Eds., The Arrows of Time, a Debate in Cosmology, Vol. 172, Springer Verlag, Heidelberg, 191-203.  
&lt;br /&gt;https://doi.org/10.1007/978-3-642-23259-6_10</mixed-citation></ref><ref id="scirp.78084-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Dowker, F. Causal Sets and the Deep Structure of Space-Time.  
&lt;br /&gt;https://arxiv.org/abs/gr-qc/0508109</mixed-citation></ref><ref id="scirp.78084-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Beckwith, A. (2016) Gedanken Experiment for Refining the Unruh Metric Tensor Uncertainty Principle via Schwarzschild Geometry and Planckian Space-Time with Initial Nonzero Entropy and Applying the Riemannian-Penrose Inequality and Initial Kinetic Energy for a Lower Bound to Graviton Mass (Massive Gravity). Journal of High Energy Physics, Gravitation and Cosmology, 2, 106-124.  
&lt;br /&gt;https://doi.org/10.4236/jhepgc.2016.21012</mixed-citation></ref><ref id="scirp.78084-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Giovanni, M. (2008) A Primer on the Physics of the Cosmic Microwave Background. World Press Scientific, Hackensack. New Jersey, USA.  
&lt;br /&gt;https://doi.org/10.1142/6730</mixed-citation></ref><ref id="scirp.78084-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Camara, C.S., de Garcia Maia, M.R., Carvalho, J.C. and Lima, J.A.S. (2004) Nonsingular FRW Cosmology and Non Linear Dynamics. Version 1.  
Arxiv astro-ph/0402311</mixed-citation></ref><ref id="scirp.78084-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Rovelli, C. and Vidotto, F. (2015) Covariant Loop Quantum Gravity. Cambridge University Press, Cambridge, United Kingdom.</mixed-citation></ref><ref id="scirp.78084-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Padmanabhan, T. (2005) Understanding Our Universe; Current Status, and Open Issues. 100 Years of Relativity, Space-Time, Structure: Einstein and Beyond, 175-204.&lt;br /&gt; http://arxiv.org/abs/gr-qc/0503107  
&lt;br /&gt;https://doi.org/10.1142/9789812700988_0007</mixed-citation></ref><ref id="scirp.78084-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Roger, P. (1965) Gravitational Collapse and Space-Time Singularities. Physical Review Letters, 14, 57. &lt;br /&gt;https://doi.org/10.1103/PhysRevLett.14.57</mixed-citation></ref><ref id="scirp.78084-ref10"><label>10</label><mixed-citation publication-type="book" xlink:type="simple">Roger, P. (1981) Time—Asymmetry and Quantum Gravity. In: Isham, C., Penrose, R. and Sciama, D., Eds., Quantum Gravity, a Second Oxford Symposium, Oxford University Press, Oxford, UK, 244-272.</mixed-citation></ref><ref id="scirp.78084-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Roos, M. (2002) Introduction to Cosmology. 2nd Edition, Wiley, New York.</mixed-citation></ref><ref id="scirp.78084-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Ryden, B. and Peterson, B. (2010) Foundations of Astrophysics. Wiley, New York.</mixed-citation></ref><ref id="scirp.78084-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Crowell, L. Notes as to the Recent FQXI Contest.  
http://fqxi.org/community/forum/topic/2796</mixed-citation></ref><ref id="scirp.78084-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Dou, D. (2001) Causal Sets, a Possible Interpretation for the Black Hole Entropy, and Related Topics. &lt;br /&gt;https://arxiv.org/pdf/gr-qc/0106024.pdf</mixed-citation></ref><ref id="scirp.78084-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Goldhaber, A. and Nieto, M. (1954) Mass of the Graviton. PRD Vol. 9, Number 4.</mixed-citation></ref><ref id="scirp.78084-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Ng, J.Y. (2008) Space-Time Foam: From Entropy and Holography to Infinite Statistics and Nonlocality. Entropy, 10, 441-461. &lt;br /&gt;https://doi.org/10.3390/e10040441</mixed-citation></ref><ref id="scirp.78084-ref17"><label>17</label><mixed-citation publication-type="book" xlink:type="simple">Freese, K., Brown, M. and Kinny, W. (2012) The Phantom Bounce: A New Proposal for an Oscillating Cosmology. In: Mersini-Houghton, L. and Vaas, R., Eds., The Arrows of Time: A Debate in Cosmology, Springer Verlag, Fundamental Theories in Physics, Heidelberg, Vol. 172, 149-156.</mixed-citation></ref><ref id="scirp.78084-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Baez, J. and Munian, J. (1994) Gauge Fields, Knots, and Gravity. Part of the Series on Knots and Everything, Vol. 4, World Scientific, Singapore.</mixed-citation></ref><ref id="scirp.78084-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Tolman, R. (1987) Relativity, Thermodynamics, and Cosmology. Dover Publishing Company, Mineola.</mixed-citation></ref><ref id="scirp.78084-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Sarkar, U. (2008) Particle and Astro Particle Physics. Series in High Energy Physics and Gravitation, Taylor &amp; Francis, New York.</mixed-citation></ref><ref id="scirp.78084-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Kolb, E. and Turner, M. (1991) The Early Universe. Westview Frontiers in Physics Series, Vol. 69.</mixed-citation></ref><ref id="scirp.78084-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Beckwith, A. (2011) How to Use the Cosmological Schwinger Principle for Energy, Entropy, and “Atoms of Space-Time” to Create a Thermodynamic Space-Time and Multiverse. Journal of Physics: Conference Series, 306, Article ID: 012064.&lt;br /&gt;  
http://iopscience.iop.org/1742-6596/306/1/012064   
&lt;br /&gt;http://iopscience.iop.org/1742-6596/306/1;jsessionid=A05372A78C18D970BF35F40A9A863B51.c2</mixed-citation></ref><ref id="scirp.78084-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Penrose, R. (2011) Cycles of Time. Alfred Knopf, New York.</mixed-citation></ref><ref id="scirp.78084-ref24"><label>24</label><mixed-citation publication-type="book" xlink:type="simple">Kadlecova H. (2012) Gravitational Field of Gyratons Propagating on Backgrounds Formed by Direct Product Space-Time’s. In: Damour, T. and Jantzen, R., Eds., The 12 Marcel Grossman Meetings of General Relativity Proceedings, World Press Scientific, Singapore, Vol. 3, 1899-1901.</mixed-citation></ref><ref id="scirp.78084-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Kadlecova, H., Zelinikov, A., Krtous P. and Podolsky, J. (2009) Gyratons on Direct-Product Space-Times. Physical Review D, 80, Article ID: 024004.  
&lt;br /&gt;https://doi.org/10.1103/PhysRevD.80.024004</mixed-citation></ref><ref id="scirp.78084-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Beckwith, A. (2011) Identifying a Kaluza Klein Treatment of a Graviton Permitting a Deceleration Parameter Q (Z) as an Alternative to Standard DE. Journal of Cosmology, 13, 1-15. http://journalofcosmology.com/BeckwithGraviton.pdf</mixed-citation></ref><ref id="scirp.78084-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Hinterbichler, K. (2011) Theoretical Aspects of Massive Gravity. Reviews of Modern Physics, 84, 671-710. http://arxiv.org/abs/1105.3735.pdf</mixed-citation></ref><ref id="scirp.78084-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">The LHCb Collaboration (2015) Determination of the Quark Coupling Strength |Vub| Using Baryonic Decays. Nature Physics, 11,743-747.  
&lt;br /&gt;https://doi.org/10.1038/nphys3415</mixed-citation></ref><ref id="scirp.78084-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Abbott, B.P., et al. (2016) Observation of Gravitational Waves from a Binary Black Hole Merger. PRL, 116, Article ID: 061102.  
&lt;br /&gt;https://physics.aps.org/featured-article-pdf/10.1103/PhysRevLett.116.061102</mixed-citation></ref><ref id="scirp.78084-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Corda, C. (2009) Interferometric Detection of Gravitational Waves: The Definitive Test for General Relativity. International Journal of Modern Physics D, 18, 2275-2282. &lt;br /&gt;https://doi.org/10.1142/S0218271809015904</mixed-citation></ref><ref id="scirp.78084-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Abbot, B.P., et al. (2016) GW151226: Observation of Gravitational Waves from a 22-Solar-Mass Binary Black Hole Coalescence. Physical Review Letters, 116, Article ID: 241103. &lt;br /&gt;https://doi.org/10.1103/PhysRevLett.116.241103</mixed-citation></ref></ref-list></back></article>