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367_1.PDF
367_1.PDF

Document
Document

phys3313-fall12-112812
phys3313-fall12-112812

... Jaehoon Yu • Tested to a precision of 1 partDr. per ...
Abstract
Abstract

"Recent Progress in Tailoring Trap-based Positron Beams" (AIP Conf. Proc. 1521, AIP Press, Melville NY, 2013), p6104p. 154-164 M. R. Natisin, N. C. Hurst, J. R. Danielson and C. M. Surko (PDF)
"Recent Progress in Tailoring Trap-based Positron Beams" (AIP Conf. Proc. 1521, AIP Press, Melville NY, 2013), p6104p. 154-164 M. R. Natisin, N. C. Hurst, J. R. Danielson and C. M. Surko (PDF)

Slides - grapes-3
Slides - grapes-3

...  Particles follow a spiral in a constant magnetic field  A high frequency alternating voltage applied between D-electrodes causes acceleration as particles cross the gap  Advantages: compact design (compared to linear accelerators), continuous stream of particles  Limitations: synchronization lo ...
Energy doubling of 42 GeV electrons in a metre-scale
Energy doubling of 42 GeV electrons in a metre-scale

CERN and High Energy Physics
CERN and High Energy Physics

... CLIC @ CERN (Design study for a 3 TeV e+e- Linear Collider, site length 48 km) ...
Radiation from accelerated charged particles
Radiation from accelerated charged particles

Project_Report_1_12
Project_Report_1_12

... picoseconds only, and they always were directed perpendicularly to the target rear surface of the irradiated target. The mechanism briefly takes place as follows. Relativistic electrons accelerated by the intense laser light propagate through the target and build up a strong electric field in the or ...
Hadron Collider Summer School
Hadron Collider Summer School

mopor046
mopor046

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Slides

... avoid depolarization – betatron tunes and synchrotron tune – small momentum spread ...
M ‘R B
M ‘R B

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2.1 Coordinates - The Center for High Energy Physics

... We want a large Rs t so that required power for a given acceleration voltage is small. Power per unit distance Ploss /L= (V/L)2 / (Rs /L) Rs /L ~ w  It is advantageous to employ higher frequency rf such as x-band (w=11.4 GHz). The drawback is that the structure becomes small and wakefield effect b ...
CERN PARTICLE ACCELERATOR
CERN PARTICLE ACCELERATOR

Beam Line - SLAC - Stanford University
Beam Line - SLAC - Stanford University

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High-Intensity Proton Beam Facilities

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HIGH ENERGY PARTICLE COLLIDERS: PAST 20 YEARS, NEXT 20

2. 2d Particle accelerators_tcm4-665527
2. 2d Particle accelerators_tcm4-665527

... electronic trigger systems that precisely measure the passage time of a particle to accuracies in the region of a few billionths of a second. The trigger system also registers the location of the part icles to millionths of a metre. This incredibly quick and precise response is essential for ensurin ...
Prospects for the Use of Coated Conductors in High Energy Physics
Prospects for the Use of Coated Conductors in High Energy Physics

... •  “A very high-energy proton-proton collider is the most powerful future tool . . .” •  “endorses medium-term R&D on high-field magnets and materials . . .” ...
IAEA_FEC_FTP1-2_INOUEslide121005
IAEA_FEC_FTP1-2_INOUEslide121005

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Particle accelerator



A particle accelerator is a device that uses electromagnetic fields to propel charged particles to high speeds and to contain them in well-defined beams.Large accelerators are best known for their use in particle physics as colliders (e.g. the LHC at CERN, RHIC at Brookhaven National Laboratory, and Tevatron at Fermilab), FACET at SLAC National Accelerator. Other kinds of particle accelerators are used in a large variety of applications, including particle therapy for oncological purposes, and as synchrotron light sources for the study of condensed matter physics. There are currently more than 30,000 accelerators in operation around the world.There are two basic classes of accelerators: electrostatic and oscillating field accelerators. Electrostatic accelerators use static electric fields to accelerate particles. A small-scale example of this class is the cathode ray tube in an ordinary old television set. Other examples are the Cockcroft–Walton generator and the Van de Graaff generator. The achievable kinetic energy for particles in these devices is limited by electrical breakdown. Oscillating field accelerators, on the other hand, use radio frequency electromagnetic fields to accelerate particles, and circumvent the breakdown problem. This class, which was first developed in the 1920s, is the basis for all modern accelerator concepts and large-scale facilities.Rolf Widerøe, Gustav Ising, Leó Szilárd, Donald Kerst, and Ernest Lawrence are considered pioneers of this field, conceiving and building the first operational linear particle accelerator, the betatron, and the cyclotron.Because colliders can give evidence of the structure of the subatomic world, accelerators were commonly referred to as atom smashers in the 20th century. Despite the fact that most accelerators (but not ion facilities) actually propel subatomic particles, the term persists in popular usage when referring to particle accelerators in general.
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