<?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">NS</journal-id><journal-title-group><journal-title>Natural Science</journal-title></journal-title-group><issn pub-type="epub">2150-4091</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ns.2015.710049</article-id><article-id pub-id-type="publisher-id">NS-60672</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Counterintuitive Increase of Information Due to Extra Spacetime Dimensions of a Black Hole and Dvoretzky’s Theorem
 
</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>23</day><month>10</month><year>2015</year></pub-date><volume>07</volume><issue>10</issue><fpage>483</fpage><lpage>487</lpage><history><date date-type="received"><day>20</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>25</month>	<year>October</year>	</date><date date-type="accepted"><day>28</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>
 
 
  As per Hawking and Bekenstein’s work on black holes, information resides on the surface and there is a limit on it amounting to a bit for every Planck area. It would seem therefore that extra dimensions would logically lead to a hyper-surface for a black hole and consequently a reduction of the corresponding information density due to the dilution effect of these additional dimensions. The present paper argues that the counterintuitive opposite of the above is what should be expected. This surprising result is a consequence of a well known theorem on measure concentration due to I. Dvoretzky.
 
</p></abstract><kwd-group><kwd>Higher Dimensional Black Holes</kwd><kwd> Dvoretzky’s Theorem</kwd><kwd> Information Paradox</kwd><kwd> E-Infinity Theory</kwd><kwd> Counterintuitive Geometry</kwd><kwd> Bekenstein Limit</kwd><kwd> Hawking Radiation</kwd><kwd> ‘tHooft-Susskind Black Holes</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It would be intuitively reasonable to suppose that in the case of black holes [<xref ref-type="bibr" rid="scirp.60672-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref10">10</xref>] with high dimensionality, i.e. extra dimensions [<xref ref-type="bibr" rid="scirp.60672-ref8">8</xref>] , the horizon i.e. the hyper quasi surface of the black hole horizon will also be of higher dimensionality. Therefore it would seem to follow that the information that resides only on the surface will be, so to speak, diluted because the Bekenstein limit is supposed to remain the same [<xref ref-type="bibr" rid="scirp.60672-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref3">3</xref>] . In other words the net effect is that the information density will decrease or so it would seem initially [<xref ref-type="bibr" rid="scirp.60672-ref10">10</xref>] .</p><p>In the present short work we show that due to the well known theorem on measure concentration the above conclusion is fallacious [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] . The said theorem due to the legendary Ukrainian-Israeli mathematician and past time President of the famous Weizmann Institute, I. Dvoretzky [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] leads to the definite conclusion that in sufficiently high dimensional spaces such as our quantum spacetime [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref14">14</xref>] , about 96% of the volume resides on the surface or very near to it while a near to only 4% remains in the deceptive bulk [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] . An almost identical result may be obtained using E-infinity theory [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref14">14</xref>] with regard to energy where the 96% energy residing on the surface is identified with the supposedly missing so called dark energy [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref13">13</xref>] . Noting the well know connection between information, entropy and thus thermodynamics and energy [<xref ref-type="bibr" rid="scirp.60672-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref7">7</xref>] we see that our conclusion has an indirect actual cosmic measurement and observational justification, in fact, confirmation [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] . In addition we note parenthetically that the Bekenstein wonderful result [<xref ref-type="bibr" rid="scirp.60672-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref8">8</xref>] upon which we are basing ourselves still needs an extension to a fractal version [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] by means of which the reduction in the information density will also be excluded [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] . It is thought that in this form the Bekenstein real limit on information will become topological and measure theoretical universality which dispels the black hole information paradox [<xref ref-type="bibr" rid="scirp.60672-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] in an unheard of simplicity conserving the most important feature of the theory of Hawking on the one side and ‘tHooft-Susskind on the other without violating any fundamental laws of physics [<xref ref-type="bibr" rid="scirp.60672-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] .</p></sec><sec id="s2"><title>2. Analysis</title><p>In the present analysis we will follow two converging roads to show the counterintuitive results of measure concentration due to very high dimensionality. We start first by Dvoretzky’s theorem [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] then we do the same using the wave-particle duality of E-infinity theory [<xref ref-type="bibr" rid="scirp.60672-ref14">14</xref>] .</p><sec id="s2_1"><title>2.1. Dvoretzky’s Theorem</title><p>The moral which we can learn, in fact relearn from this theorem is a well known wisdom from many counterintuitive results of geometry in higher dimensions, namely that we should in general never generalize an obvious conclusion from a low dimensional space to a higher one. For instance on a flat two dimensional space any two lines will intersect in a point unless they are parallel. However the spectacular failure of this simple obvious result in three dimensional space is embarrassingly clear. Now let us start with an Euclidean ball</p><disp-formula id="scirp.60672-formula1044"><label>. (1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x5.png"  xlink:type="simple"/></disp-formula><p>Working in the usual way to find the volume of this n dimensional ball we arrive via gamma function and Stirling formula to [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1045"><label>. (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x6.png"  xlink:type="simple"/></disp-formula><p>That means for V = 1 the radius is a very large one equal approximately to</p><disp-formula id="scirp.60672-formula1046"><label>. (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x7.png"  xlink:type="simple"/></disp-formula><p>Now we proceed to the distribution of the mass, i.e. how the “volume” of this ball is distributed. To do that we estimate first the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x8.png" xlink:type="simple"/></inline-formula> volume of a slice through the center of the unit ball. Since the radius of the ball [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] is</p><disp-formula id="scirp.60672-formula1047"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x9.png"  xlink:type="simple"/></disp-formula><p>Then the volume of the slice <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x10.png" xlink:type="simple"/></inline-formula> dimensional ball is given by [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1048"><label>. (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x11.png"  xlink:type="simple"/></disp-formula><p>Using the Stirling formula again we find that the slice has the volume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x12.png" xlink:type="simple"/></inline-formula> for very large n. The next question is what is the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x13.png" xlink:type="simple"/></inline-formula> dimensional volume of a parallel slice? The slice at distance x from the center is an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x14.png" xlink:type="simple"/></inline-formula> dimensional ball with radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x15.png" xlink:type="simple"/></inline-formula> so that the volume of the smaller slice is given approximately by [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1049"><label>. (6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x16.png"  xlink:type="simple"/></disp-formula><p>Since r is approximately [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1050"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x17.png"  xlink:type="simple"/></disp-formula><p>one finds [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1051"><label>. (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x18.png"  xlink:type="simple"/></disp-formula><p>That means we obtain “mass” distribution that is almost Gaussian, with variance which surprisingly does not depend upon n:</p><disp-formula id="scirp.60672-formula1052"><label>. (9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x19.png"  xlink:type="simple"/></disp-formula><p>That way we conclude the following remarkable result, namely that almost all the “volume” stays within a flab of fixed width and our result announced in the introduction of the present paper follows that about 96% of the “mass”, i.e. the volume lies in the slab [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1053"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x20.png"  xlink:type="simple"/></disp-formula><p>That means 96% is concentrated near the subspace <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x21.png" xlink:type="simple"/></inline-formula> which may be regarded as the hyper surface of an n dimensional black hole. This is a clear failure of our low dimensional intuition to anticipate what happens in high dimensional cases [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>] .</p></sec><sec id="s2_2"><title>2.2. E-Infinity Particle-Wave Duality</title><p>In E-infinity theory the pre-quantum particle as well as the pre-quantum wave follows from the fundamental equation fixing the invariants of the noncommutative E-infinity spacetime [<xref ref-type="bibr" rid="scirp.60672-ref15">15</xref>]</p><disp-formula id="scirp.60672-formula1054"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x22.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x23.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x24.png" xlink:type="simple"/></inline-formula>. Setting a = b = 0 one finds the absolutely empty set D = 0. By contrast for a = 0 and b = 1 one finds the zero set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-8302657x25.png" xlink:type="simple"/></inline-formula> which models the particle while its cobordism, i.e. the surface is nothing but the empty set [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref15">15</xref>]</p><disp-formula id="scirp.60672-formula1055"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x26.png"  xlink:type="simple"/></disp-formula><p>which models the quantum wave. Transferring this result to Kaluza-Klein “quantum” spacetime we note that the “inner” volume must be correlated, i.e. intersectional which is appropriate for a volume and leads to [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref15">15</xref>]</p><disp-formula id="scirp.60672-formula1056"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x27.png"  xlink:type="simple"/></disp-formula><p>where D (Kaluza-Klein) = 5. The outer surface, i.e. the quantum wave on the other hand is additive and non- correlated so that the union operation is what leads to the volume [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref15">15</xref>]</p><disp-formula id="scirp.60672-formula1057"><label>. (14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x28.png"  xlink:type="simple"/></disp-formula><p>A typical volume representative for both would be clearly the arithmetic mean</p><disp-formula id="scirp.60672-formula1058"><label>. (15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x29.png"  xlink:type="simple"/></disp-formula><p>In turn looking at the above as energy density we see that</p><disp-formula id="scirp.60672-formula1059"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x30.png"  xlink:type="simple"/></disp-formula><p>for m = c = 1 while</p><disp-formula id="scirp.60672-formula1060"><label>. (17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x31.png"  xlink:type="simple"/></disp-formula><p>In other words E(O) is our familiar ordinary measurable energy density of the quantum particle [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1061"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x32.png"  xlink:type="simple"/></disp-formula><p>while E(D) is our dark energy density of the quantum wave which we cannot measure [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1062"><label>. (19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x33.png"  xlink:type="simple"/></disp-formula><p>Adding both together we obtain the celebrated result [<xref ref-type="bibr" rid="scirp.60672-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.60672-ref17">17</xref>]</p><disp-formula id="scirp.60672-formula1063"><label>. (20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-8302657x34.png"  xlink:type="simple"/></disp-formula><p>Now remembering that energy and information are directly related via entropy, the preceding result is confirmation of what we obtained earlier on using Dvoretzky’s theorem, namely that 96% of the information is drawn to the surface higher dimensionality rather than “diluted” by it. Needless to say, the preceding results remain valid for a rotating Kerr black hole [<xref ref-type="bibr" rid="scirp.60672-ref18">18</xref>] .</p></sec></sec><sec id="s3"><title>3. Conclusion</title><p>The mathematical literature abounds with examples demonstrating the failure of our low dimensional intuition to extrapolate from low dimensional results to higher dimensional ones [<xref ref-type="bibr" rid="scirp.60672-ref16">16</xref>] . The holographic boundary and the horizon of a higher dimensional black hole is no exception. Rather than diluting the density of information, a higher dimensional black hole surface has a higher information density than a lower dimensional one.</p></sec><sec id="s4"><title>Cite this paper</title><p>Mohamed S.El Naschie, (2015) The Counterintuitive Increase of Information Due to Extra Spacetime Dimensions of a Black Hole and Dvoretzky’s Theorem. Natural Science,07,483-487. doi: 10.4236/ns.2015.710049</p></sec></body><back><ref-list><title>References</title><ref id="scirp.60672-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Frolov, V.P. and Zelnikov, A. (2011) Introduction to Black Hole Physics. Oxford University Press, Oxford, UK.  
&lt;br&gt;http://dx.doi.org/10.1093/acprof:oso/9780199692293.001.0001</mixed-citation></ref><ref id="scirp.60672-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Bardeen, J.M., Carter, B. and Hawking, S.W. (1973) The Four Laws of Black Hole Mechanics. Communications in Mathematical Physics, 31, 161-170. &lt;br&gt;http://dx.doi.org/10.1007/BF01645742</mixed-citation></ref><ref id="scirp.60672-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Bekenstein, J.D. (1980) Black Hole Thermodynamics. Physics Today, 33, 24-31. &lt;br&gt;http://dx.doi.org/10.1063/1.2913906</mixed-citation></ref><ref id="scirp.60672-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Meisner, C.W., Thorne, K.S. and Wheeler, J.A. (1973) Gravitation. W.H. Freeman &amp; Company, San Francisco.</mixed-citation></ref><ref id="scirp.60672-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Weinberg, S. (2008) Cosmology. Oxford University Press, Oxford, UK.</mixed-citation></ref><ref id="scirp.60672-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Susskind, L. and Lindesay, J. (2005) Black Holes, Information and the String Theory Revolution (The Holographic Universe). World Scientific, New Jersey.</mixed-citation></ref><ref id="scirp.60672-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Susskind, L. (2008) The Black Hole War. Back Bay Books, New York.</mixed-citation></ref><ref id="scirp.60672-ref8"><label>8</label><mixed-citation publication-type="book" xlink:type="simple">Horowitz, G.T. (Ed.) (2012) Black Holes in Higher Dimensions. Cambridge University Press, Cambridge, UK.  
&lt;br&gt;http://dx.doi.org/10.1017/CBO9781139004176</mixed-citation></ref><ref id="scirp.60672-ref9"><label>9</label><mixed-citation publication-type="book" xlink:type="simple">Wheeler, A. (1990) Information, Physics, Quantum: The Search for Links. In: Zurek, W., Ed., Complexity Entropy and the Physics of Information, Addison-Wesley, New York, 3-18.</mixed-citation></ref><ref id="scirp.60672-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">G. ‘tHooft (2015) G. ‘tHooft Asks a Question about General Relativity on ResearchGate, Questions and Answers, October. &lt;br&gt;https://www.researchgate.net/post/In_GR_can_we_always_choose_the_local_speed_of_light_to_be&lt;br&gt;_everywhere_smaller_that_the_coordinate_speed_of_light_Can_this_be_used_in_a_theory</mixed-citation></ref><ref id="scirp.60672-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">El Naschie, M.S. (2006) Fractal Black Holes and Information. Chaos, Solitons &amp; Fractals, 29, 23-35.  
&lt;br&gt;http://dx.doi.org/10.1016/j.chaos.2005.11.079</mixed-citation></ref><ref id="scirp.60672-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">El Naschie, M.S. (2015) If Quantum “Wave” of the Universe Then Quantum “Particle” of the Universe: A Resolution of the Dark Energy Question and the Black Hole Information Paradox. International Journal of Astronomy &amp; Astrophysics, 5, 243-247. &lt;br&gt;http://dx.doi.org/10.4236/ijaa.2015.54027</mixed-citation></ref><ref id="scirp.60672-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">El Naschie, M.S. (2015) A Resolution of the Black Hole Information Paradox via Transfinite Set Theory. World Journal of Condensed Matter Physics, 5, 249-260. &lt;br&gt;http://dx.doi.org/10.4236/wjcmp.2015.54026</mixed-citation></ref><ref id="scirp.60672-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">El Naschie, M.S. (2004) A Review of E-Infinity and the Mass Spectrum of High Energy Particle Physics. Chaos, Solitons &amp; Fractals, 19, 209-236. &lt;br&gt;http://dx.doi.org/10.1016/S0960-0779(03)00278-9</mixed-citation></ref><ref id="scirp.60672-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Connes, A. (1994) Noncommutative Geometry. Academic Press, San Diego.</mixed-citation></ref><ref id="scirp.60672-ref16"><label>16</label><mixed-citation publication-type="book" xlink:type="simple">Levy, S. (Ed.) (1997) Flavors of Geometry. Cambridge University Press, Cambridge, UK.</mixed-citation></ref><ref id="scirp.60672-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">El Naschie, M.S. (2015) Banach Spacetime-Like Dvoretzky Volume Concentration as Cosmic Holographic Dark Energy. International Journal of High Energy Physics, 2, 13-21. &lt;br&gt;http://dx.doi.org/10.11648/j.ijhep.20150201.12</mixed-citation></ref><ref id="scirp.60672-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">El Naschie, M.S. (2015) Kerr Black Hole Geometry Leading to Dark Matter and Dark Energy via E-Infinity Theory and the Possibility of Nano Spacetime Singularity Reactor. Natural Science, 7, 210-225.  
&lt;br&gt;http://dx.doi.org/10.4236/ns.2015.74024</mixed-citation></ref></ref-list></back></article>