'Bunch compression' presentation slideshows

Bunch compression - PowerPoint PPT Presentation


Accelerator Physics Topic VIII Coherent Synchrotron Radiation

Accelerator Physics Topic VIII Coherent Synchrotron Radiation

Accelerator Physics Topic VIII Coherent Synchrotron Radiation. Joseph Bisognano Engineering Physics & Synchrotron Radiation Center University of Wisconsin. Coherent Synchrotron Radiation.

By andrew
(507 views)

LCLS Commissioning Schedule and Startup Plan

LCLS Commissioning Schedule and Startup Plan

LCLS Commissioning Schedule and Startup Plan. Schedule Overview. Start XTOD commissioning. Time Now. 1st beam on Linac axis. Start Undulator commissioning. Start of Operations (X-Rays to Far Hall). UV Beam To cathode. Start LTU commissioning. CD-2a. CD-2b. FY2010. FY2003.

By lani
(163 views)

Longitudinal Dynamics - Longitudinal Phase Space Manipulation -

Longitudinal Dynamics - Longitudinal Phase Space Manipulation -

Longitudinal Dynamics - Longitudinal Phase Space Manipulation -. Introduction Bunch Length Manipulation Energy Spread Manipulation Transverse and Longitudinal Emittance Exchange and Control Summary. Introduction. e +/- :  =momentum compaction factor

By eddy
(211 views)

Bunch Compression and CSR Study in ASTA

Bunch Compression and CSR Study in ASTA

Bunch Compression and CSR Study in ASTA. Dhruv Kedar Fermilab University of Chicago July 24 th , 2012. Overview. ASTA (Advanced Superconducting Test Accelerator) Develop SRF technology International Linear Collider c omponent design Beams with ILC parameters. Goals:

By gauri
(77 views)

Bunch Compression using Static Fields

Bunch Compression using Static Fields

Bunch Compression using Static Fields. Weishi Wan Advanced Light Source L awrence Berkeley National Laboratory. FEIS 2013 - Femtosecond Electron Imaging and Spectroscopy. Key West, Florida Dec. 11, 2013. Time Varying vs Static Fields. Advantages of the static field Simpler technology

By wyatt
(108 views)

Proton Driven Plasma Wakefield Accelerator FNAL 27-10-2009

Proton Driven Plasma Wakefield Accelerator FNAL 27-10-2009

Proton Driven Plasma Wakefield Accelerator FNAL 27-10-2009. Lasers: Centimeters instead of Kilometers ?. If we take a Petawatt laser pulse, I=10 21 W/cm 2 then the electric field is as high as E =10 14 eV/m =100 TeV/m.

By gustav
(92 views)

Proton Driver for the Neutrino Factory J. Pasternak, Imperial College, London / RAL STFC

Proton Driver for the Neutrino Factory J. Pasternak, Imperial College, London / RAL STFC

Proton Driver for the Neutrino Factory J. Pasternak, Imperial College, London / RAL STFC. Outline of the talk. Introduction and ISS recommendations. Current options for NF proton driver. Towards proton driver compatible with neutron production (ISIS MW upgrade).

By yachi
(106 views)

Neutrino Factory by Zunbeltz , Davide , Margarita, Wolfgang

Neutrino Factory by Zunbeltz , Davide , Margarita, Wolfgang

Neutrino Factory by Zunbeltz , Davide , Margarita, Wolfgang. IDS proposal. Neutrino Factory - Our Specs. 4 MW beam power 2 - 8 GeV kinetic energy 5 bunches of 3 ns length 50-60 Hz rep rate. Target. Neutrino Factory: ¿our? Approach. Compressor Ring. 5 GeV. Accumulator Ring. H- Linac.

By tulia
(120 views)

Velocity Bunching Studies at FLASH Bolko Beutner, DESY XFEL Beam Dynamics Meeting 4.6.2007

Velocity Bunching Studies at FLASH Bolko Beutner, DESY XFEL Beam Dynamics Meeting 4.6.2007

Velocity Bunching Studies at FLASH Bolko Beutner, DESY XFEL Beam Dynamics Meeting 4.6.2007. Contents. Introduction ASTRA simulations Semi-Analytic Model CSR microbunch instability studies Experiments at FLASH Summary and Outlook. Introduction.

By alesia
(122 views)

CSR Workshop - Zeuthen January, 17 2002

CSR Workshop - Zeuthen January, 17 2002

Experimental Results and Computational Modeling of Pulse Compression and High Gain at the VISA SASE FEL (and related topics). James Rosenzweig UCLA Department of Physics and Astronomy. CSR Workshop - Zeuthen January, 17 2002. Acknowledgments.

By duer
(150 views)

Simulation of Longitudinal Beam Dynamics

Simulation of Longitudinal Beam Dynamics

Fachgebiet Theoretische Elektrotechnik und Numerische Feldberechnung PD Dr. Markus Clemens. DESY Beam Dynamics Meeting. Simulation of Longitudinal Beam Dynamics. Sebastian Lange, Markus Clemens Chair for Theory in Electrical Engineering and Computational Electromagnetics

By lukas
(161 views)

Free Electron Laser Projects X-FEL and the others S. Bertolucci INFN

Free Electron Laser Projects X-FEL and the others S. Bertolucci INFN

Free Electron Laser Projects X-FEL and the others S. Bertolucci INFN. European Initiatives. Scientific case: new research frontiers in. Atomic, molecular and cluster physics Plasma and warm dense matter Condensed matter physics Material science Femtosecond chemistry Life science

By kat
(156 views)

Development of micro-bunching beams and application to rare K decay experiments

Development of micro-bunching beams and application to rare K decay experiments

Development of micro-bunching beams and application to rare K decay experiments. K.A. Brown (M. Sivertz) Collider Accelerator Department, BNL (M. Tomizawa) JPARC Project, KEK. Physics Motivations Parameters from KOPIO Micro-bunching at BNL AGS Micro-bunching at J-PARC

By lee-reese
(100 views)

~40-60 M$

~40-60 M$

Sector 0 FEL R&D Test Facility – Future?. 135 MeV. 250 MeV. ~40-60 M$. 135 MeV : Gun brightness optimization Test new guns Multi-bunch tests. Low charge diagnostics Emittance exchange (with added equipment). 250 MeV : Compression Studies Velocity bunching Nonlinear optics

By brittany-harrell
(89 views)

Peter Spiller, Heavy Ion Fusion Symposium Princeton June 7-11, 2004

Peter Spiller, Heavy Ion Fusion Symposium Princeton June 7-11, 2004

Accelerator Plans at GSI for Plasma Physics Applications. Peter Spiller, Heavy Ion Fusion Symposium Princeton June 7-11, 2004. Plasma Physics Requirements. 1 . Maximum number of particles : 1-2 x 10 12 /cycle) 2. Beam energy : 400 – 2715 MeV/u

By calvin-holcomb
(92 views)

Electron Model for a 3-10 GeV, NFFAG Proton Driver

Electron Model for a 3-10 GeV, NFFAG Proton Driver

Electron Model for a 3-10 GeV, NFFAG Proton Driver. G H Rees, RAL. Proton Driver: Linac, Booster & NFFAG Layout. 3 GeV RCS booster. 66 cells. 10 GeV NFFAG. H°, Hˉ. Hˉ collimators. 200 MeV Hˉ linac. Aims of the Electron Model. The aims of the model are to check the following:

By jpleasant
(1 views)

Development of micro-bunching beams and application to rare K decay experiments

Development of micro-bunching beams and application to rare K decay experiments

Development of micro-bunching beams and application to rare K decay experiments. K.A. Brown (M. Sivertz) Collider Accelerator Department, BNL (M. Tomizawa) JPARC Project, KEK. Physics Motivations Parameters from KOPIO Micro-bunching at BNL AGS Micro-bunching at J-PARC

By rolandsmith
(0 views)

Peter Spiller,  Heavy Ion Fusion Symposium Princeton  June 7-11, 2004

Peter Spiller, Heavy Ion Fusion Symposium Princeton June 7-11, 2004

Accelerator Plans at GSI for Plasma Physics Applications. Peter Spiller, Heavy Ion Fusion Symposium Princeton June 7-11, 2004. Plasma Physics Requirements. 1 . Maximum number of particles : 1-2 x 10 12 /cycle) 2. Beam energy : 400 – 2715 MeV/u

By dmccowan
(1 views)


View Bunch compression PowerPoint (PPT) presentations online in SlideServe. SlideServe has a very huge collection of Bunch compression PowerPoint presentations. You can view or download Bunch compression presentations for your school assignment or business presentation. Browse for the presentations on every topic that you want.