Test RF gun cavity Takuya Natsui.

Slides:



Advertisements
Similar presentations
The development of ultra bright electron sources: An overview B.L. Militsyn Accelerator Science and Technology Centre Science & Technology Facility Council,
Advertisements

RF-Gun beam based alignment at PITZ/FLASH
30 th September 2004 High Power RF Couplers James Rogers High Power RF Couplers ELSRF Daresbury Laboratory.
RF-Gun cavity for high charge electron generation Takuya Natsui.
TaCo Tuner-adjustable waveguide Coupler A new generation of waveguide couplers for standing wave cavities Publication: CERN-ATS-Note Frank Gerigk,
Normal-Conducting Photoinjector for High Power CW FEL Sergey Kurennoy, LANL, Los Alamos, NM, USA An RF photoinjector capable of producing high continuous.
Before aperture After aperture Faraday Cup Trigger Photodiode Laser Energy Meter Phosphor Screen Solenoids Successful Initial X-Band Photoinjector Electron.
RF Synchronization, control and stability Takuya Natsui.
Proton Improvement Plan Bob Zwaska August 3, 2015 All-Experimenters Meeting.
POSTECH PAL Development of S-band RF gun and advanced diagnostics in PAL 박용운 (Yong Woon Park, Ph.D.) 포항 가속기 연구소 (Pohang Accelerator Laboratory, PAL) 포항공과대학교.
1 Low-energy RHIC electron Cooler (LEReC) cost estimate December 2, 2014.
1 C-Band Linac Development Satoshi Ohsawa 2004.Feb.19LCPAC.
Photocathode 1.5 (1, 3.5) cell superconducting RF gun with electric and magnetic RF focusing Transversal normalized rms emittance (no thermal emittance)
Summary of issues. RF-Gun cavity – Disk and washer (DAW) : very fast RF ageing, 2 MeV is not enough. – Quasi travelling wave side couple structure : Lower.
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
2.1GHz cavity without cell-to-cell coupling slots – 1.875” beam pipe Binping Xiao Aug
Development of Dielectric PETS Chunguang Jing and Wei Gai ANL and Euclid CLIC workshop 2013.
EuCARD is co-funded by the European Commission within the Framework Programme 7 under Grant Agreement no Reach of NC and SC Technologies, 50 …
PROPOSAL G.I.A.F. (HYBRID GUN AT HIGH FREQUENCY) INFN-LNF – UNIVERSITY OF ROME “LA SAPIENZA”- UCLA D. Alesini (T), M. Ferrario (R), A. Gallo (T),
Status of Scaling FFAG Phase Rotation ICOOL Simulations Ajit Kurup ISS Machine Group Meeting 27 th July 2006.
Electron Source Configuration Axel Brachmann - SLAC - Jan , KEK GDE meeting International Linear Collider at Stanford Linear Accelerator Center.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
RF scheme of electron linear accelerator with energy MeV Levichev A.E. Budker Institute of Nuclear Physics SB RAS.
PBG Structure Experiments, AAC 2008 Photonic Bandgap Accelerator Experiments Roark A. Marsh, Michael A. Shapiro, Richard J. Temkin Massachusetts Institute.
Laser stability Takuya Natsui. Oscillator phase lock stability.
Laser System Upgrade Overview
Laboratoire de Chimie-Physique CNRS – Université Paris-Sud UMR ORSAY Cs 2 Te photocathodes at ELYSE.
PHIN Fabrication of a photo-injector for the CTF3 accelerator and for the NEPAL test stand WP 4 of the JRA2 PHIN 1.Status of the construction of RF guns.
Round-to-Flat Beam Transformation and Applications Yine Sun Accelerator System Division Advanced Photon Source Argonne Nation Lab. International Workshop.
Ports: purpose –vacuum, rf location –accelerating cavity, coupling cavity dimensions … Already discussed, but some points need to be double checked …
S. Bettoni, R. Corsini, A. Vivoli (CERN) CLIC drive beam injector design.
13/Nov/ mm STF2 Coupler Design Content 1.Motivation 2.40mm Design 3.“Preliminary” Result by HFSS 4.“Tentative” Conclusion 5.Future.
Round-to-Flat Beam Transformation and Applications
Construction, Commissioning, and Operation of Injector Test Facility (ITF) for the PAL-XFEL November 12, 2013 S. J. Park, J. H. Hong, C. K. Min, I. Y.
Multipacting Simulation for the PITZ RF Photo Gun Igor Isaev Unwanted Beam Workshop 2012 Humboldt-University Berlin, The PITZ RF Photo Gun.
325 MHz Superconducting Spoke Cavity Coupler status. T. Khabiboulline Power Coupler design for Superconducting Spoke cavities. Originally.
A. Matveenko: Beam halo modeling in the BERLinPro Injector Halo beam transport: Generated from cathode Tracked with /wo collimators & apertures Improved.
An Electron source for PERLE
How does a klystron work? TE-MPE Section Meeting Karolina Kulesz
S.M. Polozov & Ko., NRNU MEPhI
Phil Oxford , june 18 Photoinjector at.
examples of dual-mode (3 GHz + 6 GHz) cavities
Linac beam dynamics Linac dynamics : C. Bruni, S. Chancé, L. Garolfi,
Beam dynamics simulation with 3D Field map for FCC RF gun
RadiaBeam Technologies, Santa Monica CA
Awake Electrons Gun Introduction. - How works an electrons gun
Preliminary injector linac design
Operating SRF in a "dirty" machine
Injection facility for Novosibirsk Super Charm Tau Factory
RF modes for plasma processing
RF-Gun for Phase-II RF Gun 10, June, 2016.
Needle Cathodes for RF Guns
Electron Source Configuration
Field Analysis in four different rf gun structures
CEPC 650MHz Klystron Development
A high-repetition rate low-emittance thermionic RF gun
Electron sources for FCC-ee
A-1 RF gun Takuya Natsui.
Cooler e-source Magnetized Beam LDRD Progress Report
Simulation of Emittance
Accelerator Physics Particle Acceleration
High Charge Low Emittance RF Gun for SuperKEKB
DC Photocathode Gun (JLAB)
小型X線源の性能確認実験計画 高輝度・RF電子銃研究会 広島大学 高エネルギー加速器研究機構 浦川順治
Minimized emittance for high charge with multi cell superconducting guns and solenoidal focusing D. Lipka, BESSY.
Injector for the Electron Cooler
SuperKEKB required (e+ / e-)
Cooler e-source Magnetized Beam LDRD Progress Report
Experience with photoinjector at ATF
Plasma : high electic field can accelerate electron and proton laser plasma accelerator can reduced size of future accelerator can produced particle beam.
Presentation transcript:

Test RF gun cavity Takuya Natsui

Simple cavity RF gun is developed for test Cut Disk Structure (CDS)

New CDS cavity RF gun has single standing wave cavity. shrinkage fit RF contact 0°injection RF input 1st QTW ✓ metal ✕ 20 2nd QTW choke CDS 7 New CDS cavity RF gun has single standing wave cavity. This cavity is used for cathode fix structure test or 0 deg injection. Required RF power is low, conditioning will be quickly.

Acceleration cavity This cavity is also annual coupling.

Reduce multipactoring choke structure design weak field good vacuum conduction ABS E ABS B

This gun is able to test with 60 deg or 0 deg laser injection Cathode diameter is 6 mm Aperture is 8 mm

In the simulation, 5 nC beam generation is possible

Cavity cells is under manufacturing.