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Unit 9 Electromagnetic design Episode II

Unit 9 Electromagnetic design Episode II

Unit 9 Electromagnetic design Episode II. Helene Felice , Soren Prestemon Lawrence Berkeley National Laboratory (LBNL) Paolo Ferracin and Ezio Todesco European Organization for Nuclear Research (CERN). QUESTIONS.

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466 views • 38 slides
MAGNET TECHNOLOGIES FOR LHC UPGRADES episode II

MAGNET TECHNOLOGIES FOR LHC UPGRADES episode II

CERN, 31 st July 2013 Summer student lectures. MAGNET TECHNOLOGIES FOR LHC UPGRADES episode II. E. Todesco Magnet, Superconductors and Cryostats Group Technology Department CERN, Geneva, Switzerland. CONTENTS. The challenge of superconducting cables

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466 views • 34 slides
Decay Solenoid Status

Decay Solenoid Status

Decay Solenoid Status. MJD Courthold MJ Hills JH Rochford. Important Fact. The Decay Solenoid now works !! And has been tested to 5 Tesla. Main Decay Solenoid Parameters. Parameters: Central field 5T Open inner Radius 60mm Coil inner Radius 65mm Coil length 8m

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451 views • 28 slides
A Chiral Random Matrix Model for 2+1 Flavor QCD at Finite Temperature and Density

A Chiral Random Matrix Model for 2+1 Flavor QCD at Finite Temperature and Density

A Chiral Random Matrix Model for 2+1 Flavor QCD at Finite Temperature and Density. Takashi Sano (University of Tokyo, Komaba ), with H. Fujii , and M. Ohtani.

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389 views • 26 slides
Superconducting magnets for particle accelerators - 4

Superconducting magnets for particle accelerators - 4

Superconducting magnets for particle accelerators - 4. Ezio Todesco Accelerator Technology Department European Organization for Nuclear Research (CERN). CONTENTS. Accelerator magnets Limits to highest field in Nb -Ti Hints on Nb 3 Sn Hints on detector magnets Luminosity and operation

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420 views • 23 slides
GA workplan

GA workplan

GA workplan. Primary: design and build the complex targets needed for experiments. targets that can be accurately modeled in simulation codes. targets suitable for electron transport measurements in cryogenic D 2 .

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166 views • 4 slides

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