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Initial Energy Density of root s = 7 and 8 TeV p-p Collisions at the LHC

M. CsanádDepartment of Atomic Physics, Eötvös Loránd University, H–1117 Budapest, Pázmány P. s. 1/A, HungaryT. CsörgőEKU KRC, H–3200 Gyöngyös, Mátrai út 36, HungaryZe-Fang JiangInstitute of Particle Physics, Central China Normal University, 152 Luoyu Road, Wuhan 430079, ChinaC. B. YangInstitute of Particle Physics, Central China Normal University, 152 Luoyu Road, Wuhan 430079, China
2017en
ABI

Annotatsiya

Results from the Relativistic Heavy Ion Colloder (RHIC) and the Large Hadron Collider (LHC) experiments show that in relativistic heavy ion collisions, a new state of matter, a strongly interacting perfect fluid, is created. Accelerating, exact and explicit solutions of relativistic hydrodynamics allow for a simple and natural description of this medium. A finite rapidity distribution arises from these solutions, leading to an advanced estimate of the initial energy density of high energy collisions. These solutions can be utilized to describe various aspects of proton–proton collisions, as originally suggested by Landau. We show that an advanced estimate based on hydrodynamics yields an initial energy density in s = 7 and 8 TeV proton–proton (p–p) collisions at the LHC on the same order as the critical energy density from lattice Quantum Chromodynamics (QCD). The advanced estimate yields a corresponding initial temperature that is around the critical temperature from QCD and the Hagedorn temperature. The multiplicity dependence of the estimated initial energy density suggests that in high multiplicity p–p collisions at the LHC, there is large enough initial energy density to create a non-hadronic perfect fluid.

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