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• W2144329369 abstract "The production of large extra dimension (LXD) black holes (BHs), with a new, fundamental mass scale of M f = 1 TeV , has been predicted to occur at the Large Hadron Collider, LHC, with the formidable rate of 10 8 per year in p-p collisions at full energy, 14 TeV, and at full luminosity. We show that such LXD-BH formation will be experimentally observable at the LHC by the complete disappearance of all very high p t (> 500 GeV) back-to-back correlated Di-Jets of total mass M > M f = 1 TeV , in the large detectors ALICE, ATLAS and CMS. We suggest complementing this clear cut-off signal at M > 2*500 GeV in the di-jet-correlation function by detecting the subsequent, Hawking-decay products of the LXD-BHs, namely either multiple high energy (> 100 GeV) SM Mono-Jets (i.e. away-side jet missing), sprayed off the evaporating BHs isentropically into all directions or the thermalization of the multiple overlapping Hawking-radiation in a Heckler–Kapusta-plasma: The extreme energy density of the Hawking Radiation may yield a Heckler–Kapusta–Hawking quark–gluon plasma of SM — and SUSY — particles at temperatures above the electroweak phase transition, which hydrodynamically (isentropically) evolves and cools until the quark–hadron phasetransition and chemical freezeout at T ~ 100 MeV is reached. Microcanonical quantum statistical calculations of the Hawking evaporation process for these LXD-BHs show that cold black hole remnants (BHRs) of mass ~ M f remain leftover as the ashes of these spectacular di-jet-suppressed events. The BHRs are charged and can be detected as a track in the Central TPC of ALICE. Strong di-jet suppression is also expected with heavy ion beams at the LHC, due to quark–gluon-plasma induced jet attenuation at medium to low jet energies, p t < 200 GeV . The (mono-) jets in these events can be used to trigger tsunami-emission of secondary compressed QCD-matter at well defined Mach-angles, both at the trigger side and at the awayside (missing) jet. The Machshock angles allow for a direct measurement of both the equation of state EoS and the speed of sound c s via supersonic bang in the big bang matter. We discuss the importance of the underlying strong collective flow — the gluon storm — of the QCD matter for the formation and evolution of these Machshock cones. We predict a significant deformation of Mach shocks from the gluon storm in central Au + Au collisions at RHIC and LHC energies, as compared to the case of weakly coupled jets propagating through a static medium. A possible complete stopping of p t > 50 GeV jets at the LHC in 2–3 fm yields nonlinear high density Mach shocks in the quark–gluon plasma, which can be studied in the complex emission and disintegration pattern of the possibly supercooled matter. We report on first full three-dimensional fluid dynamical studies of the strong effects of a first order phase transition on the evolution and the tsunami-like Mach shock emission of the QCD matter." @default.
• W2144329369 created "2016-06-24" @default.
• W2144329369 creator A5085065741 @default.
• W2144329369 date "2007-02-01" @default.
• W2144329369 modified "2023-09-26" @default.
• W2144329369 title "STABLE TeV BLACK HOLE REMNANTS AT THE LHC: DISCOVERY THROUGH DI-JET SUPPRESSION, MONO-JET EMISSION AND A SUPERSONIC BOOM IN THE QUARK–GLUON PLASMA" @default.
• W2144329369 cites W1558611441 @default.
• W2144329369 cites W1593860783 @default.
• W2144329369 cites W1964008532 @default.
• W2144329369 cites W1965682740 @default.
• W2144329369 cites W1966137622 @default.
• W2144329369 cites W1970736407 @default.
• W2144329369 cites W1972194477 @default.
• W2144329369 cites W1985525718 @default.
• W2144329369 cites W1990392550 @default.
• W2144329369 cites W1990447741 @default.
• W2144329369 cites W1995987344 @default.
• W2144329369 cites W1996146995 @default.
• W2144329369 cites W1998943464 @default.
• W2144329369 cites W2001361225 @default.
• W2144329369 cites W2017554302 @default.
• W2144329369 cites W2027413505 @default.
• W2144329369 cites W2045949130 @default.
• W2144329369 cites W2046987624 @default.
• W2144329369 cites W2048269255 @default.
• W2144329369 cites W2050777706 @default.
• W2144329369 cites W2053040715 @default.
• W2144329369 cites W2054457171 @default.
• W2144329369 cites W2056882964 @default.
• W2144329369 cites W2060066417 @default.
• W2144329369 cites W2062898898 @default.
• W2144329369 cites W2063300605 @default.
• W2144329369 cites W2064037652 @default.
• W2144329369 cites W2064777467 @default.
• W2144329369 cites W2070804753 @default.
• W2144329369 cites W2070968545 @default.
• W2144329369 cites W2071531712 @default.
• W2144329369 cites W2074066011 @default.
• W2144329369 cites W2077218847 @default.
• W2144329369 cites W2077756896 @default.
• W2144329369 cites W2081515245 @default.
• W2144329369 cites W2083592503 @default.
• W2144329369 cites W2084061843 @default.
• W2144329369 cites W2084642125 @default.
• W2144329369 cites W2087927249 @default.
• W2144329369 cites W2089868571 @default.
• W2144329369 cites W2090386790 @default.
• W2144329369 cites W2090585499 @default.
• W2144329369 cites W2095721433 @default.
• W2144329369 cites W2095810352 @default.
• W2144329369 cites W2097455345 @default.
• W2144329369 cites W2098439977 @default.
• W2144329369 cites W2100168895 @default.
• W2144329369 cites W2103982528 @default.
• W2144329369 cites W2108973526 @default.
• W2144329369 cites W2114527502 @default.
• W2144329369 cites W2119905532 @default.
• W2144329369 cites W2130309361 @default.
• W2144329369 cites W2131101882 @default.
• W2144329369 cites W2137320474 @default.
• W2144329369 cites W2143665736 @default.
• W2144329369 cites W2153051659 @default.
• W2144329369 cites W2156513515 @default.
• W2144329369 cites W2164431045 @default.
• W2144329369 cites W2165154082 @default.
• W2144329369 cites W2165154917 @default.
• W2144329369 cites W2592408616 @default.
• W2144329369 cites W2602692428 @default.
• W2144329369 cites W2783903576 @default.
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• W2144329369 doi "https://doi.org/10.1142/s0218271807009930" @default.
• W2144329369 hasPublicationYear "2007" @default.
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