2005
DOI: 10.1142/s0217751x05024304
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Bekenstein-Spectrum, Temperature and Specific Heat of Black Holes From Chains

Abstract: We study the thermodynamic consequences of a recently proposed description for a Schwarzschild black hole based on Euclidean (D3, D3) + (D3, D3) brane pairs described in terms of chain-like excitations. A discrete mass-spectrum of Bekensteintype is inferred and upon identification of the black hole mass with the chain's energy the leading corrections to both Hawking-temperature and specific heat of the black hole are obtained. The results indicate that for small black holes the evaporation process will be cons… Show more

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Cited by 5 publications
(7 citation statements)
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“…In the framework of String-Theory one can identify microscopic BHs with long chains living on the worldvolume of two dual Euclidean brane pairs [35]. This leads to a discrete Bekenstein-like energy spectrum for the Schwarzschild black hole [36]. The Bekenstein-like energy spectrum is present also in canonical quantization [37].…”
Section: Discussion and Conclusion Remarksmentioning
confidence: 99%
“…In the framework of String-Theory one can identify microscopic BHs with long chains living on the worldvolume of two dual Euclidean brane pairs [35]. This leads to a discrete Bekenstein-like energy spectrum for the Schwarzschild black hole [36]. The Bekenstein-like energy spectrum is present also in canonical quantization [37].…”
Section: Discussion and Conclusion Remarksmentioning
confidence: 99%
“…One therefore expects that when the branes are separated into three SU(3) branes, two SU(2) branes and one U(1) brane, as in our case, that one should be able to recover the spectrum of a supersymmetric GUT with gauge group SU(6), or a subgroup thereof, broken spontaneously to the SM gauge group. This identification can indeed be carried out for SU (6) but is complicated by the fact that the Higgs and matter content required for a supersymmetric SU(6) GUT is quite involved and includes several SU(3)×SU(2)×U(1) singlets [57]. We will therefore focus on the supersymmetric SU(5) GUT theory which has in its minimal formulation a quite succinct field content.…”
Section: Su(5) Grand Unificationmentioning
confidence: 99%
“…Let us finally point out yet another way to break, with the help of additional D7branes, N = 4 to N = 1 supersymmetry. The generic tangent space group of a 6dimensional compactification manifold is SO (6). The D3-branes were all transverse to the compactification manifold and will therefore not influence its tangent space group.…”
Section: Supersymmetry Breakingmentioning
confidence: 99%
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“…This describes a compactification from ten to d dimensions. For the uncharged, non-dilatonic Schwarzschild-Tangherlini black holes one would consider a doublet of Euclidean (D3, D3) + (D3, D3) brane pairs [30], [32], each wrapped around…”
Section: Space-filling Chainsmentioning
confidence: 99%