'Space charge' diaporamas de présentation

DC Gun

DC Gun. The Jlab UV FEL Driver ERL. IR Wiggler. SRF Linac. Bunching Chicane. UV FEL Transport Line. Dump. Design Requirements. Power recovery from exhaust beam Transverse, longitudinal matching Collective effect/instability control space charge, BBU, FEL/RF interaction

614 views • 50 slides

Beam instability theory and modeling

Beam instability theory and modeling. Oliver Boine-Frankenheim. Contents: Introduction Longitudinal instabilities (1D): Microbunching and multi-stream instabilities. Transverse instabilities (2D): Resistive wall instability and Landau damping

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556 views • 39 slides

511 views • 33 slides

Losses at PS Injection

Losses at PS Injection. S. Aumon , W. Bartmann , H. Bartosik , J. Borburgh, S. Gilardoni, B. Goddard, O. Hans, F. Peters, R. Steerenberg. Contents. Motivations Losses due to the incoming beam Possible cures Turn by turn losses Aperture Scan. Motivations.

410 views • 28 slides

Kazi Md. Shahiduzzzaman , NUB, EEE Spring 2011

Electronic Devices Tutorial Series DIODES. Kazi Md. Shahiduzzzaman , NUB, EEE Spring 2011. Table of Contents. What are diodes made out of?____________________slide 3 N-type material_________________________________slide 4 P-type material_________________________________slide 5

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SLAC Accelerator Development Program: X-Band Applications

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Lessons Learned from Real Data

Lessons Learned from Real Data. Xin Qian BNL. Outline. Space Charge effect for LArTPCs on surface Field Response Calibration How to deal with noises and dead channels. Space Charge. It is possible that the electric field in LArTPC is distorted

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Linac4 Summary (including schedule and performance)

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Electromagnetically Trapped Dusty Plasma Ring

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CHAPTER 6 THE X-RAY BEAM SPECIFIC OBJECTIVES NOTED IN THIS POWER POINT BEGIN ON PAGE 110-117.

CHAPTER 6 THE X-RAY BEAM SPECIFIC OBJECTIVES NOTED IN THIS POWER POINT BEGIN ON PAGE 110-117. . Four timers. 1) Synchronous-min time is 1/60. Increase in equal multiples 2) Electronic-most accurate/controlled by microprocessor Where are 1 and 2 located in the circuit?

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354 Chapt . 6 X-ray Tube

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59 th Hadron Synchrotron Incoherent effects section meeting

59 th Hadron Synchrotron Incoherent effects section meeting. August 9 th , 2019. Agenda. Information and Round Table. SLM. Need to send feedback on the Fermilab experiment (already contacted Frank and participants) Updated APT until 2026

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Damping of instability with octupoles

Damping of instability with octupoles. How much tune spread we can introduce with octupole correctors? How is it effective with space charge? 3. How much tune spread do we need with space charge? 4. Does it introduce significant beam loss due to octupole resonances?. Octupole correctors.

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A Quick Look at Some Systematic Errors in the TPC

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METHODS FOR MEASURING THE BEAM PROFILE IN HIGH INTENSITY BEAMS

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Space Charge Study Group

Space Charge Study Group. Mandate Webpage Kick-off Meetings concerning PTCORBIT First impressions about PTCORBIT (PS, SPS). Mandate.

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B atch C ompression M akes S ense

B atch C ompression M akes S ense. S . Hancock. Motivation. Luminosity scales as Assuming a fixed percentage of losses downstream, the intensity per Booster ring is

225 views • 9 slides

Experiments on EMMA Requiring Minimal or No Modifications

Experiments on EMMA Requiring Minimal or No Modifications. J. Scott Berg Brookhaven National Laboratory 18 March 2010. Outline of Existing Experiments. Find linear parameters vs. energy Adjust lattice to desired configuration Accelerate beam from 10 to 20 MeV Scan longitudinal phase space

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Simon Jolly Progress & Plans

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