Investigation of Atmospheric Pressure Plasma Source for CO Dissociation
... The CO can be filtered out for use in the chemical industry, or CO can be further combined in the plasma system with other gases such as hydrogen or water vapor to produce usable hydrocarbons. The design and use of a surface wave discharge excited by microwaves is experimentally examined here for th ...
... The CO can be filtered out for use in the chemical industry, or CO can be further combined in the plasma system with other gases such as hydrogen or water vapor to produce usable hydrocarbons. The design and use of a surface wave discharge excited by microwaves is experimentally examined here for th ...
Flavor Beyond Standard Model
... 5th Georgian –German School and Workshop in Basic Science, Tbilisi 2012 G.G. Devidze COMET (COherent Muon to Electron Transition), to search for coherent neutrino-less conversion of muons to electrons (μ−−e− conversion), in the presence of a nucleus, μ− + N(A,Z) → e− + N(A,Z), with a single event s ...
... 5th Georgian –German School and Workshop in Basic Science, Tbilisi 2012 G.G. Devidze COMET (COherent Muon to Electron Transition), to search for coherent neutrino-less conversion of muons to electrons (μ−−e− conversion), in the presence of a nucleus, μ− + N(A,Z) → e− + N(A,Z), with a single event s ...
71_1.PDF
... in the finite bunch case, we notice a saturation of energy coupling at high charge, which shows up in both the energy loss and peak energy gain in the plasma. Although the finite
... in the finite bunch case, we notice a saturation of energy coupling at high charge, which shows up in both the energy loss and peak energy gain in the plasma. Although the finite
Measurement of the nuclear modification factor RAA with ALICE
... transverse direction as indicated in the left panel of Fig. 1. A collision with small impact parameter b (which can be as small as zero) is called a central collision, while more grazing collisions with large b (which can be as large as two times the radius of the colliding nuclei) is called a peri ...
... transverse direction as indicated in the left panel of Fig. 1. A collision with small impact parameter b (which can be as small as zero) is called a central collision, while more grazing collisions with large b (which can be as large as two times the radius of the colliding nuclei) is called a peri ...
Measurements of Lambda, Lambda-bar and K0s from Pb
... probe nuclear matter under extreme conditions of temperature and density. Experiments are performed with the hope of creating an entirely new form of matter and observing it in the laboratory. This new form of matter is the Quark-Gluon Plasma (QGP), which according to predictions, will be created by ...
... probe nuclear matter under extreme conditions of temperature and density. Experiments are performed with the hope of creating an entirely new form of matter and observing it in the laboratory. This new form of matter is the Quark-Gluon Plasma (QGP), which according to predictions, will be created by ...
On the Electrodynamics of the Big Bang Universe - SLAC
... (CMB), predicted by Gamow, Alpher and Herman around 1950, and first observed about 1964, was emitted at Combination Time. Only, so the conventional story goes, by the effect of Gravity acting to pull matter onto very tiny density fluctuations that, allegedly, amazingly, survived, left over from far ...
... (CMB), predicted by Gamow, Alpher and Herman around 1950, and first observed about 1964, was emitted at Combination Time. Only, so the conventional story goes, by the effect of Gravity acting to pull matter onto very tiny density fluctuations that, allegedly, amazingly, survived, left over from far ...
Constraining the nuclear matter equation of state around twice
... and compact stars. Calculation of the nuclear matter EOS from first principles is a complex task and the results need to be confronted to experimental data. Heavy ion collisions provide the only tool to explore densities larger than the nuclear saturation density ρ0 in the laboratory, as in the cours ...
... and compact stars. Calculation of the nuclear matter EOS from first principles is a complex task and the results need to be confronted to experimental data. Heavy ion collisions provide the only tool to explore densities larger than the nuclear saturation density ρ0 in the laboratory, as in the cours ...
Grau_FrancisMarion_2.. - Nevis Laboratories
... Quark Gluon Plasma has occurred: it is a strongly-interacting, perfect fluid! Insights to calculating non-perturbative QCD ...
... Quark Gluon Plasma has occurred: it is a strongly-interacting, perfect fluid! Insights to calculating non-perturbative QCD ...
A Direct Empirical Proof of the Existence of Dark Matter
... (details of this fit will be given elsewhere). The emission in the Chandra energy band (mostly optically-thin ther mal bremsstrahlung) is proportional to the square of the plasma density, with a small correction for the plasma temperature (also measured from the X-ray spectra), which gives the plasm ...
... (details of this fit will be given elsewhere). The emission in the Chandra energy band (mostly optically-thin ther mal bremsstrahlung) is proportional to the square of the plasma density, with a small correction for the plasma temperature (also measured from the X-ray spectra), which gives the plasm ...
Dust Visualisation in TJ-II with Intensified Visible Fast - Docu
... The image intensifier allowed to make very fast filtered movies: 15 μs with Lithium filter (TJ-II is a lithium coated reactor) and down to 1 μs with H-alpha filter. First observations indicate that without filtering the dust light is very punctual (localised as spots) and its intensity is much highe ...
... The image intensifier allowed to make very fast filtered movies: 15 μs with Lithium filter (TJ-II is a lithium coated reactor) and down to 1 μs with H-alpha filter. First observations indicate that without filtering the dust light is very punctual (localised as spots) and its intensity is much highe ...
The Large Hadron Collider (LHC), the Higgs boson and
... for the LHC Project, (about 1700 large superconducting magnets operating in superfluid helium). The Magnet system is the main part of the LHC (worth of 1200 M€, more than 50% of the total LHC material budget) and its most complex and technological advanced system. It is the largest enterprise in sup ...
... for the LHC Project, (about 1700 large superconducting magnets operating in superfluid helium). The Magnet system is the main part of the LHC (worth of 1200 M€, more than 50% of the total LHC material budget) and its most complex and technological advanced system. It is the largest enterprise in sup ...
Experimental Observation Of Lepton Pairs Of Invariant Mass Around
... This paper reports the observation of four e+e- pairs which have the signature of a two-body decay of a particle of mass mZ = (95.2 ± 2.5) GeV/c2 . ...
... This paper reports the observation of four e+e- pairs which have the signature of a two-body decay of a particle of mass mZ = (95.2 ± 2.5) GeV/c2 . ...
Search for Scalar Top Quark Partners and Parton Shower Tuning in
... was known that neutrinos come in three flavours (νe , νµ , ντ ). Neutrinos can be produced in various ways apart from nuclear reactors. Most neutrinos on Earth originate from nuclear processes inside the Sun (pp chain, 7 Be, 8 B, etc. [6]). Another very intensive source of neutrinos is a supernova w ...
... was known that neutrinos come in three flavours (νe , νµ , ντ ). Neutrinos can be produced in various ways apart from nuclear reactors. Most neutrinos on Earth originate from nuclear processes inside the Sun (pp chain, 7 Be, 8 B, etc. [6]). Another very intensive source of neutrinos is a supernova w ...
Strangeness production
Strangeness production is a signature and a diagnostic tool of quark–gluon plasma (or QGP) formation and properties. Unlike up and down quarks, from which everyday matter is made, strange quarks are formed in pair-production processes in collisions between constituents of the plasma. The dominant mechanism of production involves gluons only present when matter has become a quark–gluon plasma. When quark–gluon plasma disassembles into hadrons in a breakup process, the high availability of strange antiquarks helps to produce antimatter containing multiple strange quarks, which is otherwise rarely made. Similar considerations are at present made for the heavier charm flavor, which is made at the beginning of the collision process in the first interactions and is only abundant in the high-energy environments of CERN's Large Hadron Collider.