'Injection energy' presentation slideshows

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Optimizing Cost and Minimizing Energy Loss for Race-Track LHeC Design

Optimizing Cost and Minimizing Energy Loss for Race-Track LHeC Design

Optimizing Cost and Minimizing Energy Loss for Race-Track LHeC Design. Jake Skrabacz University of Notre Dame Univ. of Michigan CERN REU 2008 CERN AB-department. My Problem: Conceptually. LHeC : linear electron collider

By isra
(165 views)

sLHC

sLHC

sLHC. SUMMARY FROM WG4 ( BEAM DYNAMICS) Coordinated by A. Lombardi (CERN ) Summary Future activities. sLHC. Participants to the WG - CERN/BE/ABP : end-to-end multiparticle tracking; layout definition/validation; WG coordination.

By abeni
(161 views)

R. Garoby for the LIU Project Team

R. Garoby for the LIU Project Team

LHC Injectors Upgrade Project Overview. R. Garoby for the LIU Project Team. OMCM workshop - 22/06/2011. Introduction Planned actions Status of investigations Estimated beam characteristics Planning Summary. Objectives § Organization. Mandate

By favian
(101 views)

Early History of Supernovae

Early History of Supernovae

Early History of Supernovae . S. R. Kulkarni Caltech Optical Observatories. Key Papers. “On Supernovae” Baade & Zwicky (1934a) “Cosmic Rays From Supernovae” Baade & Zwicky (1934b) “On the Search for Supernovae” Zwicky (1938). Baade & Zwicky (1934a). Novae Facts known by 1934.

By hewitt
(136 views)

Premature Dumps in 2011

Premature Dumps in 2011

M.Albert LHC Beam Operation Workshop December 2011. Premature Dumps in 2011. Acknowledgements: A.Macpherson , G.Papotti , M.Zerlauth. Outline. Introduction Data extraction Dump statistics by mode Dump causes Dumps in STABLE BEAMS Summary. Introduction.

By deanne
(162 views)

Alice overview New detector and chamber

Alice overview New detector and chamber

Alice overview New detector and chamber. ALICE TC. The ALICE smaller diameter beampipe.

By addison
(119 views)

Session Presentations: What will PS2 + SPL provide for LHC? 		Michael Benedikt

Session Presentations: What will PS2 + SPL provide for LHC? Michael Benedikt

Chamonix 2010 Summary of Session 7: Future Upgrade Scenarios for the Injector Complex P. Collier /BE (V. Mertens /TE). Session Presentations: What will PS2 + SPL provide for LHC? Michael Benedikt

By nevan
(89 views)

Shock geometry and particle injection at shocks

Shock geometry and particle injection at shocks

Shock geometry and particle injection at shocks. WG3 Session#7 Thursday PM :. Discussion: M. Desai vs H. Cane --- Do flare particles “see” CME shocks at all?

By nyoko
(103 views)

SLHC-PP kick-off meeting , CERN 9 April 2008

SLHC-PP kick-off meeting , CERN 9 April 2008

SLHC Accelerator and Injector Upgrades. Lyn Evans. SLHC-PP kick-off meeting , CERN 9 April 2008. Peak Luminosity. N b number of particles per bunch n b number of bunches f r revolution frequency  n normalised emittance  * beta value at Ip F reduction factor due to crossing angle

By vine
(125 views)

LHC Machine Advisory Committee , CERN 12th June 2008

LHC Machine Advisory Committee , CERN 12th June 2008

Current Status of LHC Project and Upgrade Plan. Lyn Evans. LHC Machine Advisory Committee , CERN 12th June 2008. Summary LHC Cryogenics. Cooldown status. Sector 56. Sector 67. Sector 78. Sector 81. Cooldown status. Sector 12. Sector 23. Sector 34. Sector 45.

By gwyn
(132 views)

On behalf of the team working on and contributing to the study:

On behalf of the team working on and contributing to the study:

Review on PS Booster with Linac4 Booster Beam Dynamics Christian Carli 15 th January 2009. On behalf of the team working on and contributing to the study: M. Aiba did most ORBIT simulations (Booster modelling …. injection)

By fruma
(123 views)

Operational availability Optimizing LHC

Operational availability Optimizing LHC

Operational availability Optimizing LHC. L. Ponce With the (un) intentiona lcontribution of all OP crew. What do I call “Operational availability”?. “ everything which is not an equipment fault“ It includes: dumps due to exceeded thresholds Hidden effects (no PM, no fault):

By elmo
(120 views)

Initial Results from the Scintillator Fast Lost Ion Probe

Initial Results from the Scintillator Fast Lost Ion Probe

Initial Results from the Scintillator Fast Lost Ion Probe. D. Darrow NSTX Physics Meeting February 28, 2005. Goal & Motivations. Goal: Predict fast ion losses from ST plasmas Motivations: Dimensionless parameters of beam ions similar to 3.5 MeV a s in NSST (good model system)

By opal
(92 views)

A method to rapidly predict the injection rate in Dye Sensitized Solar Cells

A method to rapidly predict the injection rate in Dye Sensitized Solar Cells

A method to rapidly predict the injection rate in Dye Sensitized Solar Cells. Daniel R. Jones and Alessandro Troisi PG Symposium 2009. Outline. Introduction What is a dye sensitized solar cell? How can theory help? Theory How do we compute the rate of electron transfer? Results

By april
(200 views)

Linac4 to PSB transfer line (slides by M. Garcia-Tudela & A. Lombardi slightly adapted)

Linac4 to PSB transfer line (slides by M. Garcia-Tudela & A. Lombardi slightly adapted)

Status of the LINAC4 to PSB beam dynamics studies and open questions Christian Carli 25 th May 2011 On behalf of many people contributing. Linac4 to PSB transfer line (slides by M. Garcia-Tudela & A. Lombardi slightly adapted)

By trent
(112 views)

Restrictions on the injection energy of positrons annihilating near the GC

Restrictions on the injection energy of positrons annihilating near the GC

Restrictions on the injection energy of positrons annihilating near the GC. D.O. Chernyshov , K.S. Cheng, V.A. Dogiel , C.M. Ko , W.H. IP. Annihilation: line VS continuum. Newborn fast positrons should annihilate in flight: - continuum emission > 1 MeV. COMPTEL:

By adora
(60 views)

HE-LHC Machine Overview

HE-LHC Machine Overview

HE-LHC Machine Overview. o n behalf of the HE-LHC study group. Frank Zimmermann, FCC Week 2018 Amsterdam, 9 April 2018.

By smolen
(0 views)

LHC Upgrades

LHC Upgrades

LHC Upgrades. PPAP 14th July 2009 Steve Myers. 1. Peak Luminosity. N b number of particles per bunch n b number of bunches f r revolution frequency  n normalised emittance  * beta value at Ip F reduction factor due to crossing angle N b ,  n injector chain  * LHC insertion

By calvinr
(2 views)


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