'Vacuum chamber' diaporamas de présentation

Machine Group Summary

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The LHC Machine

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Is It Dead O r Alive?

Is It Dead O r Alive?. By: Diantha Smith. Living things have characteristics that distinguish them from nonliving things. Living things use energy respond to their environment grow and develop produce waste reproduce.

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Design and Development of a CubeSat De-Orbit Device

Design and Development of a CubeSat De-Orbit Device. Team Members. An Kim Cian Branco David Warner Edwin Billips Langston Lewis Thomas Work Mackenzie Webb Benjamin Cawrse (CS) Jason Harris (TCC). Introduction. Thousands of man made objects in earth orbit (mostly junk).

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Undulator Systems Stephen V. Milton, ANL May 21, 2003

Undulator Systems Stephen V. Milton, ANL May 21, 2003. Hi Steve! A checklist of items to be covered . System Overview Undulator Prototype data recap If Liz is coming, do you want her to do this? We could make it after lunch thursday List of long-lead procurements

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CLIC Vacuum Issues (2) Paolo Chiggiato Vacuum, Surfaces and Coatings TE department

CLIC seminars. CLIC Vacuum Issues (2) Paolo Chiggiato Vacuum, Surfaces and Coatings TE department. Content: Vacuum problems in CLIC. Known solutions: Bakeout. Lumped pumping. Linear pumping. Distributed pumping: NEG coatings. Amorphous carbon coatings.

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Beamline update

Overview of the beamline Beam diagnostics Silicon Protection New options for location of HPS. The Beginning. Beamline update. Beamlines to Hall A Hall B. Ken Moffeit 5 June 2013.

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Rutgers 12-inch Cyclotron

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Maher Attal On behalf of : SESAME Technical Staff

SESAME Booster Status. Maher Attal On behalf of : SESAME Technical Staff. TAC 2013, 22-23 Nov., SESAME, Maher Attal. Answers to the last TAC Recommendations . By changing working point (2.22, 2.13) (2.22, 1.31), vertical amplification factor is reduced by ~ factor 2. .

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Lecture 4

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R eview of Collective Effects for Low Emittance Rings

R eview of Collective Effects for Low Emittance Rings. ICFA Beam Dynamics Mini Workshop on Low Emittance Rings 2011, 3-5 October 2011, Heraklion , Crete, Greece R . Nagaoka, Synchrotron SOLEIL, Gif- sur -Yvette, France. R. Nagaoka. LER2011, 3-5 October 2011: 2/20.

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Francesco Cerutti , Luigi S. Esposito, Anton Lechner , Alessio Mereghetti

1st WORKSHOP COLLIDER-EXPERIMENT INTERFACE Nov 30, 2012 CERN. ENERGY DEPOSITION AND TAS DIAMETER. Francesco Cerutti , Luigi S. Esposito, Anton Lechner , Alessio Mereghetti. OUTLINE. the TAS role (as intended, imagined, and actual) looking around the present and future triplet

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In-situ K- Ar dating using LIBS in the VUV range

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Using Tune Shifts to Evaluate Electron Cloud Effects on Beam Dynamics at CesrTA

Using Tune Shifts to Evaluate Electron Cloud Effects on Beam Dynamics at CesrTA. Jennifer Chu Mentors: Dr. David Kreinick and Dr. Gerry Dugan. Outline. Review of Electron Clouds and Tune Shifts Simulations of New Data Varying the Simulation Parameters. Electron Clouds.

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Brazing technique

Brazing technique. Eric Vigeolas , Didier Ferrere , Serge Mathot , Theodore Todorov , Pierre Delebecque LSWG Cooling meeting May the 31th 2012. Foreword. Here is an interesting summary made by Parker company concerning the joining techniques

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Warm Up October 21, 2013

Warm Up October 21, 2013. Mrs. Hurwitz has an uninflated balloon. She fills the balloon with a gas and ties it closed. When she lets go, the balloon floats up into the sky. She wonders what happened to the mass of the balloon. What do you think? The floating balloon has more mass

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Particle Studio and MAFIA c omparison

Particle Studio and MAFIA c omparison. Olav Berrig with a lot of help by Benoit Salvant. The comparison is done for the SPS pumping port between MBA and MBB magnets. SPS pumping port design. PARTICLE STUDIO. MAFIA. The SPS tunnel, with visible pumping port.

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Title Date

Title Date. Author for the C ESR TA Collaboration. Shielded Pickup Measurements in June, 2011 Ryan Badman , Jim Crittenden, John Sikora. The TiN-coated vacuum chamber at 15W was installed in September, 2010. The diamond-like carbon-coated chamber at 15E was installed in January, 2011.

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Resistive Wall Instability in the Drive Beam Formation system

Resistive Wall Instability in the Drive Beam Formation system. B. Jeanneret CLIC Beam Dyn Meeting 10 March 2010. Basics. Amplitude or emmitance growth : . P roblem : train 240 ns long and I = 100 A Need Copper chamber ( high conductivity ) Large radius magnet cost

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