<?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">WJCMP</journal-id><journal-title-group><journal-title>World Journal of Condensed Matter Physics</journal-title></journal-title-group><issn pub-type="epub">2160-6919</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/wjcmp.2015.54026</article-id><article-id pub-id-type="publisher-id">WJCMP-60214</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>
 
 
  A Resolution of the Black Hole Information Paradox via Transfinite Set Theory
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ohamed</surname><given-names>S. El Naschie</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>Department of Physics, University of Alexandria, Alexandria, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Chaossf@aol.com</email></corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>10</month><year>2015</year></pub-date><volume>05</volume><issue>04</issue><fpage>249</fpage><lpage>260</lpage><history><date date-type="received"><day>19</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>9</month>	<year>October</year>	</date><date date-type="accepted"><day>12</day>	<month>October</month>	<year>2015</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>
 
 
  A black hole is essentially a relativistic as well as a quantum object. Therefore the information paradox of black holes is a consequence of the clash between these two most fundamental theories of modern physics. It is logical to conclude that a resolution of the problem requires some form of a quantum gravity theory. The present work proposes such a resolution using set theory and pointless spacetime geometry.
 
</p></abstract><kwd-group><kwd>Information Paradox</kwd><kwd> Black Holes</kwd><kwd> S. Hawking</kwd><kwd> G. ‘t Hooft</kwd><kwd> L. Susskind</kwd><kwd> Transfinite Set Theory</kwd><kwd>  Noncommutative Geometry</kwd><kwd> Measure Concentration</kwd><kwd> Dvoretzky’s Theorem</kwd><kwd> Dark Energy</kwd><kwd>  Casimir Effect</kwd><kwd> Nano Casimir Reactor</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Physically empty space with no matter, virtual particles or radiation what so ever is still far from being nothing [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] . Empty spacetime in the above sense is a sophisticated sloika, i.e. Mille-Feuill of empty sets [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref20">20</xref>] . A point in such space is by no means the classical point defined somewhat naively as the intersection of two lines [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] . In fact a proper spacetime, which satisfies the physical quantum reality, is a points-less spacetime with geometry and topology akin to that of von Neumann’s continuous geometry [<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref119">119</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref132">132</xref>] as well as A. Conne’s noncommutative geometry [<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref132">132</xref>] apart from the arch typical pointless space of E-infinity Cantorian spacetime [<xref ref-type="bibr" rid="scirp.60214-ref11">11</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref132">132</xref>] . In such Cantorian-fractal geometry what appears to be a point is in actuality an entire Cantor set when magnified by sharpening the resolution of observation [<xref ref-type="bibr" rid="scirp.60214-ref33">33</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref130">130</xref>] . Combining the preceding fundamental insights gained from applying transfinite set theory and fractals to spacetime geometry with a fundamental theorem due to Aryeh Dvoretzky about measure concentration [<xref ref-type="bibr" rid="scirp.60214-ref65">65</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref67">67</xref>] , we can argue that only 4.5 percent of the information inside a black hole could be regarded as inaccessible while the rest of the 95.5 percent of the information remains on the surface of the black hole no matter how much it shrinks because in the end analysis, spacetime has no ordinary points and no matter how small such points are, they are not zero nor can they vanish into nothingness because empty spacetime is anything but nothing. In fact empty spacetime is a multi-fractal made of infinitely many empty sets with varying degrees of emptiness [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref12">12</xref>] . In this sense we can reconcile what appeared for a considerable time irreconcilable, namely the view point of S. Hawking [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] with all that speaks for it and speaks against it, with the clearly opposing views of L. Susskind and G. ‘t Hooft which is understandable, logical and correct, but nevertheless does not propose an alternative waterproof answer to replace that of S. Hawking’s famous but by no means entirely correct one [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] .</p><p>The paper is subdivided into three reasonably short parts. First, we introduce the required background information. Second, we sketch our basic analysis and finally we summarize our conclusions. Last but not least, it should be acknowledged from the outset that the recent revival of black hole physics and the information paradox at the prominent conference in Stockholm [<xref ref-type="bibr" rid="scirp.60214-ref133">133</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref135">135</xref>] as well as the highly influential writing of L. Susskind and G. ‘t Hooft [<xref ref-type="bibr" rid="scirp.60214-ref135">135</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref139">139</xref>] are the prime movers and motivation for the present work.</p></sec><sec id="s2"><title>2. Physical, Mathematical and Cosmological Measure Concentration Phenomena</title><p>There are at least three well known types of measure concentration phenomena [<xref ref-type="bibr" rid="scirp.60214-ref64">64</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref67">67</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref140">140</xref>] relevant to the present work. The first is what we could call physical measure concentration. We could give two examples for that. The first is the Faraday cage demonstrating that for a metal sphere the total electric charge is concentrated on the surface with zero change inside the sphere [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] . This fact is behind the fortunate situation that an aeroplane flying in a thunder and lightening storm can protect the passengers from being electrocuted as is the case with a car with closed doors and windows. The second example is the energy of the quantum particle-wave where 4.5% of the energy is inside the quantum wave concentrated in the quantum particle as measurable ordinary energy while the quantum wave surrounding the quantum particles possesses most of the energy density, namely 95.5% as dark energy [<xref ref-type="bibr" rid="scirp.60214-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref61">61</xref>] . The best example for mathematical measure concentration is the marvellous Dvoretzky’s theorem which states that in sufficiently high dimensionality, 96% of the volume of a sphere is concentrated near to its surface while the “bulk” contains only 4% of the volume [<xref ref-type="bibr" rid="scirp.60214-ref140">140</xref>] . Finally cosmological concentration phenomena may be found theoretically in the fact that all information of a black hole is proportional to the surface and not to the volume of the black hole as demonstrated by the Bekenstein formula [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref138">138</xref>] . As a second example we could cite the work of the present author showing that the 4.5% ordinary energy of the universe can be measure “inside” the universe while the rest, the 95.5% dark energy exists mainly near to the boundary of the holographic boundary of the universe [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref11">11</xref>] . It is the fact that our universe could be viewed as a giant black hole that we may argue that black holes, if they exist, will have most of its information, i.e. about 96% of the information on the surface of the black hole while 4% of the information could remain locked inside the black hole to which an outside observer will have no access.</p></sec><sec id="s3"><title>3. The Transfinite Theory of Spacetime</title><p>To make a long, in fact very long story short, we start our journey to the exact picture of our physico-mathe- matical spacetime from the bijection formula [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref75">75</xref>] .</p><disp-formula id="scirp.60214-formula81"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x5.png"  xlink:type="simple"/></disp-formula><p>corresponding to von Neumann-Conne’s dimensional function [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref75">75</xref>] of Penrose foliated universe, i.e. Penrose tiling. This is necessarily a fractal universe resembling a compactified holographic boundary, i.e. compactified Klein modular curve for a transfinite E8E8 Lie exceptional symmetry groups constituting our bulk [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref75">75</xref>] .</p><p>Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x6.png" xlink:type="simple"/></inline-formula> is the Hausdorff dimension corresponding to n Menger-Urysohn dimension and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x7.png" xlink:type="simple"/></inline-formula> is</p><p>the Hausdorff dimension of the zero set, i.e. n = 0. To see that we set n = 0 in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x8.png" xlink:type="simple"/></inline-formula> and find [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref75">75</xref>]</p><disp-formula id="scirp.60214-formula82"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x9.png"  xlink:type="simple"/></disp-formula><p>The corresponding von Neumann-Conne formula is [<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>]</p><disp-formula id="scirp.60214-formula83"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x10.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x11.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x12.png" xlink:type="simple"/></inline-formula>. Setting a = 0 and b = 1 one finds the same value, namely</p><disp-formula id="scirp.60214-formula84"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x13.png"  xlink:type="simple"/></disp-formula><p>This is our zero set which models the pre-quantum particle [<xref ref-type="bibr" rid="scirp.60214-ref129">129</xref>]</p><disp-formula id="scirp.60214-formula85"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x14.png"  xlink:type="simple"/></disp-formula><p>for the pre-quantum wave, i.e. the surface or cobordism of the quantum particle we just need to insert <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x15.png" xlink:type="simple"/></inline-formula> which is the dimension of the neighbourhood of a point. That way we find [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref75">75</xref>]</p><disp-formula id="scirp.60214-formula86"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x16.png"  xlink:type="simple"/></disp-formula><p>or equivalently by setting a = 1 and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x17.png" xlink:type="simple"/></inline-formula> one finds [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>]</p><disp-formula id="scirp.60214-formula87"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x18.png"  xlink:type="simple"/></disp-formula><p>This is the empty set which models the quantum particle. We see that the zero set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x19.png" xlink:type="simple"/></inline-formula> separates the sets <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x20.png" xlink:type="simple"/></inline-formula> from the empty sets <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x21.png" xlink:type="simple"/></inline-formula> and we are thus justified to speak of the degree of emptiness of an empty set [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>] as we move from n = 1 to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x22.png" xlink:type="simple"/></inline-formula> until we reach the truly insubstantial nothingness for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x23.png" xlink:type="simple"/></inline-formula> which leads to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x24.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. The Menger-Urysohn Dimensionality and the Dimensions of the Empty Set d(Menger) = −1</title><p>The discussion of the section on the transfinite theory of spacetime depended crucially upon the extension of the notion of topological dimensions into the negative regime. In this section we show how simple, intuitive and easily grasped this extension of the deductive topological dimension theory which goes back to the Russian Paul Urysohn and the Austrian Karl Menger [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>] . Take a 3D cube. The dimension of the cube is 3 but the dimension of the six sides of the surface of the cube is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula> which is a trivial result. Applying the same argument to the two dimensional surface, the borders are lines and therefore we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x26.png" xlink:type="simple"/></inline-formula> which is equally trivial. Continuing this for the line we find that the dimensions of the edges of the line must follow the same formula, namely<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x27.png" xlink:type="simple"/></inline-formula>. For a line n = 1 we find edge points<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x28.png" xlink:type="simple"/></inline-formula>, again a trivial result. Here triviality stops because continuing for the point n = 0 one finds a non-trivial result, namely<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x29.png" xlink:type="simple"/></inline-formula>. Earlier on we called this the empty neighbourhood of a point or the empty set [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] . Continuing for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x30.png" xlink:type="simple"/></inline-formula> one finds then the truly completely empty set with the Hausdorff dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x31.png" xlink:type="simple"/></inline-formula> and the bidimension representation [<xref ref-type="bibr" rid="scirp.60214-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>]</p><disp-formula id="scirp.60214-formula88"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x32.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. An Exact Picture of Quantum Spacetime</title><p>We clearly live in a 3 + 1 = 4 dimensional world. These are three special dimensions plus a temporal dimension preventing things from happening all at once in some folkloristic philosophy. Einstein’s special and general relativity takes the time dimension far more seriously as a dimension which one can put on equal footing as the space dimension if not even more [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] . Inserting n = 4 in our bijection formula one finds [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>]</p><disp-formula id="scirp.60214-formula89"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x33.png"  xlink:type="simple"/></disp-formula><p>Consequently we have [<xref ref-type="bibr" rid="scirp.60214-ref12">12</xref>]</p><disp-formula id="scirp.60214-formula90"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x34.png"  xlink:type="simple"/></disp-formula><p>This means the fractal Hausdorff dimension is larger than the corresponding Menger-Urysohn topological dimension by the amount <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x35.png" xlink:type="simple"/></inline-formula> which we will see later on that it is equal to the intrinsic so called latent topological Casimir pressure of empty spacetime [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] . Now having found <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x36.png" xlink:type="simple"/></inline-formula> is an important result but we would like to scrutinize this result and analyse it in a far deeper way.</p><p>Let us look back at our spacetime as being made of an infinite mixture of all possible Cantor sets. That means starting from the unit set, i.e. classical line <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x37.png" xlink:type="simple"/></inline-formula> and the zero set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x38.png" xlink:type="simple"/></inline-formula> until we reach the totally empty set. The sum of all these sets is clearly [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] .</p><disp-formula id="scirp.60214-formula91"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x39.png"  xlink:type="simple"/></disp-formula><p>Now since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x40.png" xlink:type="simple"/></inline-formula> represents for us a random Mauldin-Williams triadic Cantor set [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] living in one dimension, then gaging the sum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x41.png" xlink:type="simple"/></inline-formula> in terms of this Cantor set, we can say that the dimension of our mixture of Cantor sets is simply [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref74">74</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref76">76</xref>] .</p><disp-formula id="scirp.60214-formula92"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x42.png"  xlink:type="simple"/></disp-formula><p>which is the Hausdorff dimension of our spacetime. However there is a still more profound interpretation of these results because <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula> is the inversion of the Hausdorff dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x44.png" xlink:type="simple"/></inline-formula> of a quantum particle while <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x45.png" xlink:type="simple"/></inline-formula> is the inversion of the Hausdorff dimension of the quantum wave<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x46.png" xlink:type="simple"/></inline-formula>. In other words <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x47.png" xlink:type="simple"/></inline-formula> is both the intersection between the particle like behaviour given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x48.png" xlink:type="simple"/></inline-formula> and the wave like behaviour dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x49.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60214-formula93"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x50.png"  xlink:type="simple"/></disp-formula><p>as well as the union of the two, namely</p><disp-formula id="scirp.60214-formula94"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x51.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x52.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x53.png" xlink:type="simple"/></inline-formula> are the un-normed probability of particle and wave respectively. In other words our space is blind to the union and intersection and cannot tell them apart which is the deepest explanation possible for the particle-wave duality of quantum mechanics [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] . Armed with all the preceding results let us see if we can construct a simple exact picture of micro spacetime.</p><p>We start with the zero set pre-particle. This is</p><disp-formula id="scirp.60214-formula95"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x54.png"  xlink:type="simple"/></disp-formula><p>Surrounding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x55.png" xlink:type="simple"/></inline-formula> is its cobordism or the guiding quantum wave which means the empty set [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>]</p><disp-formula id="scirp.60214-formula96"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x56.png"  xlink:type="simple"/></disp-formula><p>The cobordism, or surface of the guiding Bohm-Einstein quantum wave, is clearly <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x57.png" xlink:type="simple"/></inline-formula> which is given by [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>]</p><disp-formula id="scirp.60214-formula97"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x58.png"  xlink:type="simple"/></disp-formula><p>Now something quite remarkable happens at this point. The particle wave entity is floating in spacetime with an average dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x59.png" xlink:type="simple"/></inline-formula> which means a normed average dimension<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x60.png" xlink:type="simple"/></inline-formula>. That means spacetime is the cobordism, i.e. the surface of the guiding Bohm-Einstein, ergo ghost quantum wave and consequently the surface of the quantum wave is given by the expectation value [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>]</p><disp-formula id="scirp.60214-formula98"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x61.png"  xlink:type="simple"/></disp-formula><p>In other words our quantum spacetime is nothing but a zero set pre-quantum particle surrounded by an empty set pre-quantum wave floating in the surface of the quantum wave given by the expectation value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x62.png" xlink:type="simple"/></inline-formula>. The ghost is no ghost at all unless we consider spacetime to be a ghost. In the next section we will see how all of that relates to Casimir energy and dark energy [<xref ref-type="bibr" rid="scirp.60214-ref2">2</xref>] .</p></sec><sec id="s6"><title>6. The Casimir Local Topological Pressure</title><p>If two plates which are conducting but uncharged are put very close vis-&#224;-vis each other, it is an experimental fact that they are pulled together by what is known as the Casimir effect [<xref ref-type="bibr" rid="scirp.60214-ref94">94</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref120">120</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref121">121</xref>] . The E-infinity set theoretical explanation advanced some time ago is as follows: The nano distance between the two plates is as near as we can come to create an empty set. That means inside the plates we have a topological pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x63.png" xlink:type="simple"/></inline-formula> stemming from the state of the entropy-like disorder measured by the Hausdorff dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x64.png" xlink:type="simple"/></inline-formula> of the empty set. Outside, adjacent to the plates, we have the zero set of the quantum particles. Consequently the net topological pressure is the difference between the empty set quantum wave <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x65.png" xlink:type="simple"/></inline-formula> and the zero set quantum particle which means <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x66.png" xlink:type="simple"/></inline-formula> giving us the intrinsic latent topological pressure of empty spacetime which by inversion, leads to the Hausdorff dimension<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x67.png" xlink:type="simple"/></inline-formula>. In other words the Casimir topological pressure is the same at the counter factual part in the general formula for Hardy’s quantum entanglement, namely [<xref ref-type="bibr" rid="scirp.60214-ref58">58</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref68">68</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref71">71</xref>]</p><disp-formula id="scirp.60214-formula99"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x68.png"  xlink:type="simple"/></disp-formula><p>and setting the number of particles n = 0 we are left with the global part [<xref ref-type="bibr" rid="scirp.60214-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref34">34</xref>]</p><disp-formula id="scirp.60214-formula100"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-4800319x69.png"  xlink:type="simple"/></disp-formula><p>Thus we could think of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula> as the excess in the fluctuation of spacetime dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula> over the average topological dimension 4 causing the extra pressure of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x72.png" xlink:type="simple"/></inline-formula> which manifests itself locally as the Casimir effect. A pedestrian way to understand that is the following: The un-normalized probability due to quantum particles is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x73.png" xlink:type="simple"/></inline-formula> and for the quantum wave is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x74.png" xlink:type="simple"/></inline-formula>. The minimal integer approximation of the sum of both is clearly 1 + 2 = 3 and the maximal is 3 + 2 = 5. Consequently the average integer value is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x75.png" xlink:type="simple"/></inline-formula>. On the other hand D is not 4 but <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x76.png" xlink:type="simple"/></inline-formula> showing that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x77.png" xlink:type="simple"/></inline-formula> is indeed a measure for topological dimensional or entropic fluctuation in full agreement with all previous conclusions which we made earlier on [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref11">11</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref20">20</xref>] .</p></sec><sec id="s7"><title>7. Dark Energy Is Global Dvoretzky Concentration of Casimir Energy</title><p>The two Casimir plates of the classical Casimir effect experiment, plays obviously the role of a boundary condition. What happens then when this boundary is pushed to infinity? The answer is it becomes the boundary of the holographic boundary of the universe [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] . This boundary is obviously a one sided boundary with nothing outside to push back to create a statical balance. It is a M&#246;bius-like multi-dimensional boundary and consequently the universe must expand into the insubstantial nothingness surrounding our universe which is a clopen (which means open and closed topologically) and a multiverse of its own self. Considering that this E-infinity multiverse universe has formally infinite dimensions, we see that the Dvoretzky theorem [<xref ref-type="bibr" rid="scirp.60214-ref140">140</xref>] will apply and as a result 95.5% of the energy of this universe will be concentrated at the edge of the universe. Consequently the difference between the Casimir energy and dark energy is the difference between local and global as well as two sided and one sided boundary conditions [<xref ref-type="bibr" rid="scirp.60214-ref120">120</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref127">127</xref>] .</p></sec><sec id="s8"><title>8. How to Build a Nano Casimir-Dark Energy Reactor</title><p>From the preceding discussion it is an inescapable conclusion that we could build a nano universe using nano technology and that such a universe will constitute a unit cell of a nano Casimir-dark energy reactor [<xref ref-type="bibr" rid="scirp.60214-ref94">94</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref96">96</xref>] [<xref ref-type="bibr" rid="scirp.60214-ref120">120</xref>] from which we can extract an infinite amount of clean energy using empty spacetime as our fuel.</p><p>To start we can use a large amount of C<sub>60</sub> Fullerene [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] nano particles which are the smallest dodecahedron [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] known to exist at present. There are many reasons to suspect that the universe geometry and topology resembles that of a dodecahedron so that each C<sub>60</sub> particle is an approximately universe prototype geometrically and topologically speaking [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] . Each two faces of the C<sub>60</sub> powder will act as a Casimir cell and the complexity of the heap will produce an artificial local high dimensionality for which Dvoretzky’s theorem applies [<xref ref-type="bibr" rid="scirp.60214-ref140">140</xref>] . Adding a large number of these artificial nano universes we end up with a macroscopic multiverse from which energy can in principle be extracted from its most outer surface. The rest is technological details. However we are more than aware that the devil lies in the detail. Nevertheless all that we can say at this point is that we will use in principle the same technology used to minimize the usually harmful effects of the Casimir effect on nano devices only this time in a reversed fashion, i.e. trying to maximise these effects rather than minimizing it [<xref ref-type="bibr" rid="scirp.60214-ref120">120</xref>] - [<xref ref-type="bibr" rid="scirp.60214-ref127">127</xref>] .</p></sec><sec id="s9"><title>9. A Set Theoretical Resolution of the Black Hole Information Paradox</title><p>We started by discussing black holes, then moved from there to Casimir energy, dark energy and nano reactors [<xref ref-type="bibr" rid="scirp.60214-ref140">140</xref>] . With the benefit of hindsight let us see what the connection is between these seemingly very different problems. Maybe it is good for a deep understanding of the problem at hand to ask oneself can we really solve a mind teaser like the information paradox without knowing really what space is, what time is and worse still, what the word nothingness means. The present author admits that he thought that this is not possible and that was exactly his point of departure. First of all totally empty space is not nothing but something substantial even without any fluctuation or pair creation and annihilation. Empty spacetime is a multidimensional empty set. The empty set is far from being nothing. As soon as you mention the word set then the word nothing is not there. Insubstantial nothingness is not even a set. The border line is the totally empty set given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x78.png" xlink:type="simple"/></inline-formula> to the power of (infinity). The empty set on the other hand is given by two dimensions, namely minus one and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-4800319x79.png" xlink:type="simple"/></inline-formula> both of which are not zero or nothing. Consequently by shrinking a spherical black hole indefinitely it can never become a zero point with a zero surface area because quantum space has no ordinary (na&#239;ve) classical point exactly as the pointless spaces of von Neumann’s noncommutative geometry and E-infinity Cantorian spacetime [<xref ref-type="bibr" rid="scirp.60214-ref7">7</xref>] . The information density becomes extremely large but not infinity as the black hole becomes extremely small but never zero so that at the end about 95.5% of the information encoded on the surface of the black hole is never lost and only 4.5% of the information inside the black hole becomes inaccessible to us. Paradoxically for us living inside this giant black hole we call the universe, the situation is reversed for something related to information, via entropy which we call energy [<xref ref-type="bibr" rid="scirp.60214-ref120">120</xref>] -[<xref ref-type="bibr" rid="scirp.60214-ref127">127</xref>] . Only 4.5% of the energy of the universe is accessible to us while 95.5% of the energy of the universe cannot be measured directly and we known that it is there only because of observing its effect manifested via the accelerated cosmic expansion [<xref ref-type="bibr" rid="scirp.60214-ref140">140</xref>] .</p></sec><sec id="s10"><title>10. Conclusion</title><p>Actual empty spacetime is far from being nothing and is a multi-dimensional empty set, which is a substantial something. This spacetime is pointless and what appears to be a point is, upon magnification, a complete random Cantor set. In such spacetime a black hole will always have a non-zero surface area no matter how small it shrinks and will never vanish and have a zero surface area. In such a situation, and by a well known brilliant theorem due to the great late A. Dvoretzky who was at a time the President of the Wiseman Institute, at least 95.5% of the information of a black hole will not be lost. The situation is analogous to that of the ordinary and the dark energy of the universe and could be used as a guiding principle in the design of a nano Casimir-dark energy reactor. In the end analysis we think that our inability to give a waterproof definition to the words point, line and so on coupled with mildly ignoring the impact of nonlinear dynamics, chaos and fractals on fundamental quantum physics contributes to a delay of the development of black hole research and related subjects. We hope the present work has at a minimum helped positively in this direction.</p></sec><sec id="s11"><title>Cite this paper</title><p>Mohamed S.El Naschie, (2015) A Resolution of the Black Hole Information Paradox via Transfinite Set Theory. World Journal of Condensed Matter Physics,05,249-260. doi: 10.4236/wjcmp.2015.54026</p></sec></body><back><ref-list><title>References</title><ref id="scirp.60214-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Marek-Crnjac, L. (2013) Cantorian Space-Time Theory: The Physics of Empty Sets in Connection with Quantum Entanglement and Dark Energy. 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