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Likin_Poster_APS 2003 - HSX - University of Wisconsin–Madison
Likin_Poster_APS 2003 - HSX - University of Wisconsin–Madison

arXiv:1606.09570v1 [physics.gen-ph] 29 Jun 2016
arXiv:1606.09570v1 [physics.gen-ph] 29 Jun 2016

... to the Pauli exclusion principle which does not allow more than two particles (e.g. neutrinos) to occupy the same state. b. A central mass consisting of one or rarely two leptons. These lepton(s) can be charged (e.g. e+ in the case of a proton or e− in the case of the Σ− or Ξ− baryons), and are stab ...
Slides - Indico
Slides - Indico

The Physics of Energy sources Nuclear Fusion
The Physics of Energy sources Nuclear Fusion

... !   Same Coulomb barrier than D-D reaction but with a larger cross-section !   Pb: requires tritium which is radioactive and needs to be produced through fusion reaction ...
Diagnostic research of highly ionized plasma generated by an ECR
Diagnostic research of highly ionized plasma generated by an ECR

... One of the research directions of the ATOMKI-ECRIS is the systematic investigation of the con"ned plasma. In our laboratory we have the instrumentation background for two plasma research methods: X-ray and visible light diagnostics is possible outside the plasma chamber and the plasma can be investi ...
PS - USTC, ICTS
PS - USTC, ICTS

... But just say you use another gauge invariant one, it is not physical, because it includes unphysical gluon field. • We also appreciate P.M. Zhang, D. Pak and Y.M. Cho’s effort. They claim their approach can avoid the Gribov ambiguity. • We appreciate X. Ji’s criticism which pushed us very much to un ...
Slide 1 - Indico
Slide 1 - Indico

... When antimatter meets its matter twin They annihilate in flash of light ...
OAM12-Yuan
OAM12-Yuan

Low energy Electron Collision with Polar Molecules HCl and HBr in
Low energy Electron Collision with Polar Molecules HCl and HBr in

arXiv:1501.03541v1 [hep
arXiv:1501.03541v1 [hep

McLerran.pdf
McLerran.pdf

... Matter at low energy densities is composed of electrons, protons and neutrons. If we heat the system, we might produce thermal excitations which include light mass strongly interacting particles such as the pion. Inside the protons, neutrons and other strongly interacting particles are quarks and gl ...
Sample pages 2 PDF
Sample pages 2 PDF

teachers` resource book on fundamental particles and
teachers` resource book on fundamental particles and

... called o, /3 and 7 rays. We now know that the o ray is ...
Recycling strange stars to millisecond periods
Recycling strange stars to millisecond periods

... n −→ 2d + u, followed by the weak-interaction process u + d −→ s + u. These reactions lead to an additional heat release (deconfinement heating) at the crust-strange matter interface, of some 30–40 MeV per accreted nucleon. ...
Neutral beam plasma heating
Neutral beam plasma heating

... A high density and high temperature environment is required for fusion of two light atoms to happen and magnetic confinement is one of a very few possibilities to confine plasma, since the high temperatures would melt any material wall. First fusion experiments took place back in 1930, but it was no ...
Pulsar slow glitches in a solid quark star model
Pulsar slow glitches in a solid quark star model

... of the energy released turns into heat and melts the debris, while the other part turns to the kinetic energy of the fluid. It is suggested in this model that the broken material will turn into viscous fluid and is therefore able to flow slowly and change the shape of the star towards the equilibriu ...
matter - Osborne High School
matter - Osborne High School

Curriculum Vitae - Department of Physics, Panjab University
Curriculum Vitae - Department of Physics, Panjab University

... Professional Experience and Research interests My research interests are focused on improving our present day understanding of the hadronic structure of matter. Hadrons are the basic building blocks of all matter and are envisaged to be composed of truly elementary particles called quarks and gluons ...
accelerating
accelerating

Weakton Model of Elementary Particles and Decay Mechanisms
Weakton Model of Elementary Particles and Decay Mechanisms

... questions given at the beginning of the Introduction. We end this Introduction by mentioning that there have been numerous studies on sub-quark and sub-lepton models; see among others [9, 1, 11, 4] The paper is organized as follows. A brief introduction to the current understanding of elementary par ...
Numerical simulation of the Helicon Double Layer Thruster
Numerical simulation of the Helicon Double Layer Thruster

... obtained by a helicon-source plasma expansion along a diverging magnetic field. Their findings can lead eventually to development of innovative space propulsion system.5–7 Similarities were met by independent researchers: Hairapetian,8 Cohen,9 Sun10, 11 and Plihon;12, 13 while a first 1D-MCC-PIC mod ...
Lecture 7
Lecture 7

QCD Factorization for Semi
QCD Factorization for Semi

... simplification to the collinear factorization  Extends to the region where collinear fails  Simplifies the kinematics ...
Extension of Lorentz Group Representations for Chiral Fermions
Extension of Lorentz Group Representations for Chiral Fermions

CTF-3 - CARE-HHH
CTF-3 - CARE-HHH

... this effect would suggest that the total distance travelled through the plasma cannot be more than one or a few radiation lengths for example X0~10 m for 4x1022 e/cm3 using the rough estimate of 30 GV/m for 1x1017e/cm3 this gives an ultimate energy of ~200 TeV ...
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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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