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Particle physics tomorrow LHC
Particle physics tomorrow LHC

Plasma Accelerators
Plasma Accelerators

... For decades, particle colliders have used microwave cavities to propel particle beams to nearly the speed of light. That approach, exemplified by the 8.6-kilometer-diameter Large Hadron Collider, is reaching its technological and economic limits. A new technique, in which electrons or positrons gain ...
Classical tunes of Gluon Dynamics
Classical tunes of Gluon Dynamics

... The strange thing is, these phenomena reveal themselves in present-day experiments via hadrons (pions) with extremely small momenta k⊥ , where we are expecting to hit the non-perturbative domain — large coupling αs (k⊥ ) — and potential failure of the quark–gluon language as such. The fact that the ...
Particle Physics Part III Major Option 2008
Particle Physics Part III Major Option 2008

...  Empirically, the strong force is short range and therefore know that the physical gluons are confined. The colour singlet state does not exist in nature ! NOTE: this is not entirely ad hoc. In the context of gauge field theory (see minor option) the strong interaction arises from a fundamental SU( ...
PowerPoint file of HBM_part 2
PowerPoint file of HBM_part 2

bass
bass

L69 CONVERSION OF NEUTRON STARS TO
L69 CONVERSION OF NEUTRON STARS TO

... There is now compelling evidence to suggest that a substantial fraction of all gamma-ray bursts (GRBs) occur at cosmological distances (with a redshift z ∼ 1–3 ). In particular, the measured redshifts of z = 3.42 for GRB 971214 (Kulkarni et al. 1998) and z ∼ 1.6 for GRB 990123 (Kulkarni et al. 1999) ...
Accelerated Expansion of Space, Dark Matter, Dark Energy and Big
Accelerated Expansion of Space, Dark Matter, Dark Energy and Big

Interactions of Dust Bilayers in a GEC Plasma
Interactions of Dust Bilayers in a GEC Plasma

... appreciable shift in either layer when the two layers were placed in the cell simultaneously, as shown in Figure 6. The distances between layers for this pressure, as well as the distance from the top layer to the predicted location of the first potential maximum, are shown in Figure 7. As before, t ...
Computing Quark and Gluon Distribution Functions for Very Large
Computing Quark and Gluon Distribution Functions for Very Large

... they are of the Weiszacker-Williams form. We also show that there is an effective field theory with propagators modified from their vacuum form which allows for the systematic computation of corrections to the lowest order result. The problem ...
Delta isobars in neutron stars
Delta isobars in neutron stars

... is converted within a few milliseconds. Moreover, since the energy released in such a process is of the order of 1052 erg, it is clear that a similar event would provide very strong neutrino and electromagnetic signals, possibly connected with supernovae and gamma-ray-bursts [40, 42, 53–55]. An inte ...
slides - University of Toronto Physics
slides - University of Toronto Physics

rapid recombination of plasma jets
rapid recombination of plasma jets

... the plasma expands, moving along the lines of force with opening angle 2.9-m, tan J.m = 3vA/uc: the of the decaying field. We assume at the outset that plasma density goes as 1/ z 2 • the plasma magnetized by the field H0 moves into In estimating the cooling it is now convenient to the vacuum with a ...
DPF09_huangd
DPF09_huangd

High angle neutron-proton scattering
High angle neutron-proton scattering

NRE4610-notes - RTF Technologies
NRE4610-notes - RTF Technologies

... Coulomb scattering We now divide the plasma into 2 parts; inside and outside the Debye sphere. Inside the Debye sphere two charged particles can interact and scatter of each other. As one particle approaches another, it experiences a force due to coulomb repulsion. This will cause the particles to ...
DOE06Proposal25Sep2006CMS
DOE06Proposal25Sep2006CMS

... study the production and properties of this partonic state of matter. Additionally we will look for evidence of chiral symmetry restoration in these collisions. We also propose to carry these investigations to the next level, using the Compact Muon Solenoid (CMS) detector at the Large Hadron Collide ...
Plain text version - FCC Week 2016
Plain text version - FCC Week 2016

... The Future Circular Collider study (FCC) explores different designs of circular colliders for the postLHC era. The FCC collaboration will deliver a conceptual design report by the end of 2018, together with preliminary cost estimates and feasibility assessments that will lay the foundations for the ...
arXiv:1412.6954v1 [hep-ph] 22 Dec 2014
arXiv:1412.6954v1 [hep-ph] 22 Dec 2014

ppt - Fusion Technology Institute
ppt - Fusion Technology Institute

... efficiency while providing plasma jet that can start with large diameter but be narrowed directionally to focus. Analogous to planar electrostatic ion thruster "folded" into spherical form. Electrical efficiency match conventional plasma thrusters; ...
Mass_01 - StealthSkater
Mass_01 - StealthSkater

arXiv:1502.02576v1 [physics.ins
arXiv:1502.02576v1 [physics.ins

... much is known beyond the mean field, about hadronic correlations and their backreaction to the structure of the model QCD phase diagram and its thermodynamics. Here we will elaborate on the generalized Beth-Uhlenbeck form of the equation of state which is systematically extended from studying mesoni ...
Jens Juul Rasmussen
Jens Juul Rasmussen

Relativistic electron-positron plasmas
Relativistic electron-positron plasmas

Advanced Accelerators: Near and Far Future Options
Advanced Accelerators: Near and Far Future Options

... – Use of more exotic colliding particles (muons) – More elaborate sourcery and “cooling” techniques ...
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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.
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