Conveners
Accelerator Physics
- Vladimir Shiltsev (Fermilab)
- R. Joel England (SLAC)
Accelerator Physics
- R. Joel England (SLAC)
- Vladimir Shiltsev (Fermilab)
Accelerator Physics
- Vladimir Shiltsev (Fermilab)
- R. Joel England (SLAC)
Accelerator Physics
- Vladimir Shiltsev (Fermilab)
- R. Joel England (SLAC)
Accelerator Physics
- Vladimir Shiltsev (Fermilab)
- R. Joel England (SLAC)
Accelerator Physics
- Vladimir Shiltsev (Fermilab)
- R. Joel England (SLAC)
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Mr Valeri Lebedev (FNAL)8/9/11, 2:00โฏPMAccelerator PhysicsParallel contributionThe success of Tevatron Run II is based on advances in accelerator physics, as well as on the excellence and advances in engineering, instrumentation and machine operation. We review the main advances in accelerator physics which contributed to the luminosity growth and/or improvement of the Tevatron complex operations, and discuss their applicability to future colliders.Go to contribution page
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Dr Wolfram Fischer (BNL)8/9/11, 2:30โฏPMAccelerator PhysicsParallel contributionThe Relativistic Heavy Ion Collider (RHIC) at Brookhaven National Laboratory has now operated for a decade. Over this time the 2 physics programs at RHIC, based on heavy ion and polarized proton collisions respectively, have seen a substantial increase in performance and a variety of operating modes. The performance increases are presented with the dominant limiting effects, and upgrade plans...Go to contribution page
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Dr Walter Wittmer (SLAC)8/9/11, 3:00โฏPMAccelerator PhysicsParallel contributionThe SuperB international team continues to optimize the design of an electron-positron collider, which will allow the enhanced study of the origins of flavor physics. The project combines the best features of a linear collider (high single-collision luminosity) and a storage-ring collider (high repetition rate), bringing together all accelerator physics aspects to make a very high luminosity...Go to contribution page
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Dr vitaly yakimenko (bnl)8/9/11, 4:00โฏPMAccelerator PhysicsParallel contributionFew representative experimental results from a 20 year old history of the dedicated advanced accelerator R&D user facility will start the presentation. Evolution of the facility, its current capabilities and experimental program will be discussed in details. Monoenergetic Ion beam generation in laser plasma interaction and observation of Coherent Synchrotron Radiation suppression with...Go to contribution page
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Dr Gil Travish (UCLA)8/9/11, 4:30โฏPMAccelerator PhysicsParallel contributionOf the various advanced accelerator schemes that promise high accelerating gradients, optical-scale structures offer a distinct set of performance parameters along with their own challenges. In addition to the promise of an order of magnitude improvement in accelerating gradients (to ~GV/m) over conventional structures, these devices produce low charge, femto- to atto-second bunches at very...Go to contribution page
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Giulio Stancari (Fermi National Accelerator Laboratory)8/9/11, 5:00โฏPMAccelerator PhysicsParallel contributionThe hollow electron beam collimator is a novel concept of controlled halo removal for intense high-energy beams in storage rings and colliders. It is based on the interaction of the circulating beam with a 5-keV, magnetically confined, pulsed hollow electron beam in a 2-m-long section of the ring. The electrons enclose the circulating beam, kicking halo particles transversely and leaving the...Go to contribution page
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Dr John Byrd (LBNL)8/9/11, 5:30โฏPMAccelerator PhysicsParallel contributionTo meet the energy and luminosity requirements of future HEP machines, advances are required in accelerator instrumentation and technology in many diverse areas, such as: acceleration, component alignment and stability, fast timing instrumentation and optics, photocathodes, pulsed power components, photon detectors, halo monitors, collimators, lasers, insertion devices, noninvasive profile...Go to contribution page
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Bob Tschirhart (-Fermilab)8/10/11, 2:00โฏPMAccelerator PhysicsParallel contributionFermilab is leading an international consortium to develop the design of โProject-Xโ which is an accelerator complex based on a new H- linac that will drive a broad range of experiments at the Intensity Frontier. Project X will provide multi-MW beams from the Main Injector over the energy range 60-120 GeV, simultaneous with mult-MW beams at 3 GeV. The Project-X research program includes...Go to contribution page
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8/10/11, 2:30โฏPMAccelerator PhysicsParallel contributionWe preยญsent the deยญsign of fuยญture high-enยญerยญgy high-luยญmiยญnosยญiยญty elecยญtron-hadron colยญlidยญer at RHIC called eRHIC. We plan on adding 20 (poยญtenยญtialยญly 30) GeV enยญerยญgy reยญcovยญery linacs to acยญcelยญerยญate and to colยญlide poยญlarยญized and unยญpoยญlarยญized elecยญtrons with hadrons in RHIC. The cenยญter-of-mass enยญerยญgy of eRHIC will range from 30 to 200 GeV. The luยญmiยญnosยญiยญty exยญceedยญing 1034...Go to contribution page
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Dr Michael Zisman (Lawrence Berkeley National Laboratory)8/10/11, 3:00โฏPMAccelerator PhysicsParallel contributionA muon collider would be a powerful tool for exploring the energy-frontier with leptons, and would complement the studies now under way at the LHC. Such a device would offer several important benefits. Muons, like electrons, are point particles so the full center-of-mass energy is available for particle production. Moreover, on account of their higher mass, muons give rise to very little...Go to contribution page
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Prof. Sami Tantawi (SLAC)8/10/11, 4:30โฏPMAccelerator PhysicsParallel contributionResearch on the basic physics of high-gradient, high frequency accelerator structures and the associated RF/microwave technology are essential for the future of discovery science, medicine and biology, energy and environment, and national security. We will review the state-of-the-art for the development of high gradient linear accelerators.Go to contribution page
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Dr Alexander Zlobin (Fermilab)8/10/11, 5:00โฏPMAccelerator PhysicsParallel contributionFor a fixed size of a circular collider, its energy is limited by the strength of bending dipole magnets. Moreover, for both linear and circular machines, their maximum luminosity is determined (among other factors) by the strength of quadrupole magnets used for the final beam focusing. That is why there has been a permanent interest to higher-field and higher-field gradient accelerator...Go to contribution page
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Prof. Jean Delayen (Old Dominion University)8/10/11, 5:30โฏPMAccelerator PhysicsParallel contributionThe superconducting RF (SRF) technology is increasingly becoming the technology of choice for a wide range of particle accelerators. It has found applications in high energy and nuclear physics accelerators, spallation neutron sources, and light sources. The opportunities offered by the SRF technology, and its challenges, will be presented and reviewed.Go to contribution page
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Jose Alonso (MIT-LNS)8/10/11, 6:00โฏPMAccelerator PhysicsParallel contributionNeutrino physics from muon decay is very much at the forefront of today's physics research. Large detectors installed in deep underground locations perform neutrino mass, CP violation, and oscillation studies using long- and short-baseline beams of neutrinos from muons decaying in flight. DAEdALUS looks at neutrinos from stopped muons, โDecay At Rest (DAR)โ neutrinos. The DAR neutrino spectrum...Go to contribution page
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Ulisse Bravar8/11/11, 10:30โฏAMAccelerator PhysicsParallel contributionThe muon ionization cooling experiment (MICE) is a strategic R&D project intending to demonstrate the only practical solution to prepare high brilliance beams necessary for a neutrino factory or muon colliders. MICE is under development at the Rutherford Appleton Laboratory (UK). It comprises a dedicated beam line to generate a range of input emittance and momentum, with time-of-flight and...Go to contribution page
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Eric Torrence (University of Oregon)8/11/11, 11:00โฏAMAccelerator PhysicsParallel contributionA precision luminosity measurement is of critical importance for the ATLAS physics program, both for searches for new physics as well as for precision measurements of Standard Model cross-sections. The calibration of the luminosity is based on three so-called van der Meer scans that were performed in 2010. These scans determine the convolved beam sizes in the vertical and horizontal...Go to contribution page
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Dr John Flanagan (KEK)8/11/11, 11:30โฏAMAccelerator PhysicsParallel contributionThe KEKB B factory is being upgraded to search for physics beyond the Standard Model, with a target luminosity of 8x10^35 cm^-2 s^-1, a factor of 40 times greater than the world record luminosity achieved at KEKB. To achieve this target luminosity the upgraded machine, SuperKEKB, will require the use of new advances in accelerator technology, among them the development of a low-emittance,...Go to contribution page
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Dr Wim Leemans (LBNL)8/12/11, 8:00โฏAMAccelerator PhysicsParallel contributionAccelerators are essential tools of discovery and have many practical uses. More than three decades ago, lasers were proposed as power sources for driving novel accelerators based on plasmas as the accelerating medium. An overview will be presented of the basic principles of laser plasma accelerators (LPA) and of the research at LBNL. This includes the 2004 demonstration of high quality...Go to contribution page
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Dr Robert Byer (Stanford University)8/12/11, 8:30โฏAMAccelerator PhysicsParallel contributionThe dielectric laser acceleration (DLA) concept leverages well-established industrial fabrication capabilities and the commercial availability of tabletop lasers to reduce cost, while offering significantly higher accelerating gradients, and therefore a smaller footprint. In contrast to other novel accelerator schemes, desirable luminosities would be obtained by operating with very low charge...Go to contribution page
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Patric Muggli (University of Southern California)8/12/11, 9:00โฏAMAccelerator PhysicsParallel contributionThe plasma wakefield accelerator (PWFA) concept is experiencing renewed interest thanks to the recent experimental results that showed that ultrarelativistic electrons can gain as much as 42GeV in only 85cm of plasmas. In the PWFA a short particle bunch drives large amplitude wakefields in a neutral plasma. The wakefields can have a very large longitudinal component (>10GV/m) that leads to...Go to contribution page