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Theoretical particle physics Represented by Theory group: Faculty
Theoretical particle physics Represented by Theory group: Faculty

2.9 Periodic Trends
2.9 Periodic Trends

Linear Accelerators
Linear Accelerators

C1 and C2 are threshold Cerenkov counters filled with CO 2 , for
C1 and C2 are threshold Cerenkov counters filled with CO 2 , for

... • 10 - 400 GeV/c, up to 108 particles/spill (π+) • H4 can be set-up for very clean electron beam (up to ~300 GeV/c) • H2/H4 originate from same (T2) target – due to beam optics, H2 and H4 should run with opposite polaritiy beams – e.g. H2: protons or π+, H4: electrons – beam conditions of H2 and H4 ...
e - National Centre for Physics
e - National Centre for Physics

... The scattering crossection is the product of Rutherford scattering for a point particle multiplied by form factors F(Q2 ) and G(Q2 ) which are functions of virtual photon mass Q2 . These form factors are related roughly to average shape of a proton. For a particle with no structure the crossection ...
rhic - Wayne State University
rhic - Wayne State University

16_04_2013 - IB Phys.. - hrsbstaff.ednet.ns.ca
16_04_2013 - IB Phys.. - hrsbstaff.ednet.ns.ca

[a,b]! - Nikhef
[a,b]! - Nikhef

...  K0-K0, B0-B0 and neutrino oscillations: CP violation (origin of matter!)  Large-Hadron-Collider (LHC): electro-weak symmetry breaking (origin of mass!)  Fantasy land (order TeV ee and  colliders, neutrino factories, …) ...
Screen-Based Graphic Design: Tips for non
Screen-Based Graphic Design: Tips for non

... – Head-on collisions between protons at energies ~20TeV are required to produce a Higgs Boson.Such energies can only be achieved by particle accelerators like the Large Hadron Collider at CERN – The Higgs Boson was found in July 2012 at CERN with a rest mass ~ 126 GeV/c2 ...
Superconductive Stabilization System for Charging Particle
Superconductive Stabilization System for Charging Particle

... in this direction are opened by the application of superconductive systems with using the effects of magnetic potential well.Without restricting the generality of the problem, as a particular case, we have considered the stability and stationary motion conditions for charged particles in the electro ...
Cap3
Cap3

Section 2.0a: the four fundamental interactions, leptons and hadrons
Section 2.0a: the four fundamental interactions, leptons and hadrons

Lecture 14 - Experimental Achievements in Physics
Lecture 14 - Experimental Achievements in Physics

... - Henri Becquerel (1852-1908) knew of Rontgen’s experiments, and decided to investigate phosphorescent materials (materials that would glow) - He took a photographic plate and wrapped it in heavy black paper, blocking exposure to sunlight - He then took a thin crust of potassium uranyl sulphate crys ...
Insights on Jet Physics & High- Energy Emission Processes from Optical Polarimetry
Insights on Jet Physics & High- Energy Emission Processes from Optical Polarimetry

Synchrotron Radiation Sources for the Future
Synchrotron Radiation Sources for the Future

mc2007_ATLAS_Neil
mc2007_ATLAS_Neil

Option 212: UNIT 2 Elementary Particles - X
Option 212: UNIT 2 Elementary Particles - X

No Slide Title
No Slide Title

JLab 12 GeV upgrade (3) [C3]
JLab 12 GeV upgrade (3) [C3]

... capabilities for the study of QCD well beyond those available at existing facilities worldwide and complementary to those planned for the next generation of accelerators in Europe and Asia.” ...
A radiant invention - Arktis Radiation Detectors Ltd
A radiant invention - Arktis Radiation Detectors Ltd

Standard Model
Standard Model

Searches for NP : non-SUSY scenarios
Searches for NP : non-SUSY scenarios

No Slide Title - University of Manchester
No Slide Title - University of Manchester

2009S-FindingHiggs
2009S-FindingHiggs

... •Main incentive is Electroweak Unification •Weak force makes the Lagrangian unrenormalizable because of W and Z masses •To fix this: γ, W+, W-, and Z are at high energies mixed together to be new fields W1, W2, W3, and B •To solve mass problem, Higgs field hypothesized, with a nonzero vacuum expecta ...
Lecture 12 – Asymptotic freedom and the electrodynamics of quarks
Lecture 12 – Asymptotic freedom and the electrodynamics of quarks

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DESY



The Deutsches Elektronen-Synchrotron (english German Electron Synchrotron) commonly referred to by the abbreviation DESY, is a national research center in Germany that operates particle accelerators used to investigate the structure of matter. It conducts a broad spectrum of inter-disciplinary scientific research in three main areas: particle and high energy physics; photon science; and the development, construction and operation of particle accelerators. Its name refers to its first project, an electron synchrotron. DESY is publicly financed by the Federal Republic of Germany, the States of Germany, and the German Research Foundation (DFG). DESY is a member of the Helmholtz Association and operates at sites in Hamburg and Zeuthen.
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