Pepperpot Emittance Measurements of the FETS Ion Source

Slides:



Advertisements
Similar presentations
Imperial College London 1 3. Beam extraction 3. Extraction of particle beams 3.1 The space charge limit and Child-Langmuirs law 3.2 External and internal.
Advertisements

AWAKE Electron Spectrometer Simon Jolly 7 th March 2013.
Pepperpot Emittance Measurements of the FETS Ion Source
ATF2 Interaction Point Beam Size Monitor (Shintake Monitor) Status T. Yamanaka, M. Oroku, Y. Yamaguchi, S. Komamiya ( Univ. of Tokyo ), T. Suehara, Y.
J. Rudolph, Helmholtz-Zentrum Berlin EuCARD 2nd ANNUAL MEETING Slice emittance measurements at the ELBE superconducting RF photoinjector.
SPEC(troscopy) -Trap Outline of talk Introduction – motivation for two cross continent traps Imperial College Group – areas of interest and expertise SPECTRAP/SPECTRAP’
AWAKE Electron Spectrometer Design Simon Jolly 4 th September 2012.
Matching and Synchrotron Light Diagnostics F.Roncarolo, E.Bravin, S.Burger, A.Goldblatt, G.Trad.
Electron Spectrometer Progress Report Simon Jolly 19 th October 2012.
What’s already existing?What’s already existing? Laser system & impacts on Optics TransportLaser system & impacts on Optics Transport –Laser power –Focusing.
Status Report on Mk.II Pepperpot Simon Jolly Imperial College 13 th June 2007.
Data Acquisition and Error Analysis for Pepperpot Emittance Measurements Simon Jolly Imperial College DIPAC ‘09.
Laser based Emittance Measurement for LINAC4 Project Overview & Current Status T. Hofmann, E. Bravin, U. Raich, F. Roncarolo, F.
Recent Progress in X-ray Emittance Diagnostics at SPring-8 S. Takano, M. Masaki, and H. Sumitomo * JASRI/SPring-8, Hyogo, Japan SES, Hyogo, Japan *
Noise Suppression Experiment - ATF A. Gover, A.Nause, E. Dyunin Tel-Aviv University Fac. Of Engin., Dept. of Physical Electronics, Tel-Aviv, Israel THANKS.
FETS meeting, 1st November 2006 Peter Savage The Front End Test Stand Collaboration 1 The mechanical engineering design of the Mk II emittance measurement.
Transverse emittance Two different techniques were used to measure the transverse emittance. The multislit mask in the injector 9 MeV Quadrupole scan for.
Uli Raich CERN BE/BI Instrumentation for the new H - Source Test Bench Linac-4 Ion Source Review 2011 Uli Raich CERN BE/BI Linac 4 ion source review, CERN.
RFQ CAD Model Beam Dynamics Studies Simon Jolly 3 rd August 2011.
05/05/2004Cyrille Thomas DIAMOND Storage Ring Optical and X-ray Diagnostics.
ATF1/2 laser-wires Stewart T. Boogert on behalf of UK Extraction line laserwire collaboration A. Aryshev, G. Blair, S. Boogert, A. Bosco, L. Corner, L.
Recent Experiments at PITZ ICFA Future Light Sources Sub-Panel Mini Workshop on Start-to-End Simulations of X-RAY FELs August 18-22, 2003 at DESY-Zeuthen,
Assessing Single Crystal Diamond Quality
Status of the Front End Test Stand April Infrastructure R8 refurbished Laser lab under construction Vacuum system for first section delivered Stands.
Development of a Gamma-Ray Beam Profile Monitor for the High-Intensity Gamma-Ray Source Thomas Regier, Department of Physics and Engineering Physics University.
G5 Beam Instrumentation D. Gassner, E. Pozdeyev 4-09.
Tests of AWAKE spectrometer screen and camera at PHIN Introduction Layout Procedure Setup, results (runs 1 – 5) Conclusions L. Deacon, S. Mazzoni, B. Biskup.
Simulations and Diagnostics for the Front End Test Stand Simon Jolly Imperial College 18 th April 2007.
1 Multi-Optical Transition Radiation System for ATF2 A.Faus-Golfe, J.Alabau, C.Blanch, J.V.Civera, J.J.García Garrigós IFIC (CSIC-UV) D.McCormick, G.White,
Current Status of Pepperpot Emittance Measurement System Simon Jolly Imperial College FETS Meeting, 22/02/06.
FETS Pepperpot Simon Jolly 10 th February The Pepperpot Beam segmented by intercepting screen with regular array of holes. Beamlets drift short.
Tests of spectrometer screens Introduction Layout Procedure Results Conclusions L. Deacon, B. Biskup, S. Mazzoni, M.Wing et. al. AWAKE collaboration meeting,
A.Shapovalov (DESY, Zeuthen) (MEPhI, Moscow, Russia)
Accelerator Science and Technology Centre Extended ALICE Injector J.W. McKenzie, B.D. Muratori, Y.M. Saveliev STFC Daresbury Laboratory,
R. Pani Department of Experimental Medicine and Pathology University of Rome La Sapienza-Italy. Flat Panel PMT: advances in position sensitive photodetection.
FETS RFQ Beam Dynamics Simulations for RFQSIM, CST and Comsol Field Maps Simon Jolly 2 nd June 2010.
Christoph Gabor, ASTeC HIPPI—Meeting (WP 5) 26 th – 28 th September 2007 Non—destructive transverse emittance measurement device The Front End Test Stand.
UK Neutrino Factory Meeting Front End Test Stand (F.E.T.S.) Engineering Status by P. Savage 22nd April 2009.
Developments of the FETS Ion Source Scott Lawrie.
Pepperpot Emittance Measurement System: Current Status Simon Jolly Imperial College FETS Meeting, 10/05/06.
Electron Spectrometer: Status July 14 Simon Jolly, Lawrence Deacon 1 st July 2014.
Progress of Mk.II Pepperpot: Camera, Scintillator and Data Analysis Simon Jolly Imperial College 24 th January 2007.
Tagger and Vacuum Chamber Design Jim Kellie Glasgow University.
FETS Ion Source Diagnostics: The Pepperpot
Measurement of Transverse Emittance in ASTA John Nocita Amber Johnson John Diamond August 8, 2013.
LumiCal High density compact calorimeter at the ILC Wojciech Wierba Institute of Nuclear Physics PAS Cracow, Poland.
Understanding Extraction And Beam Transport In The ISIS H - Ion Source D. C. Faircloth, A.P Letchford, C. Gabor, S. Lawrie M. O. Whitehead and T. Wood.
(Chapter 7) CHEM–E5225 Electron microscopy
Laser Geiger cell (update)
Emittance measurements for LI2FE electron beams
Strike Point Observation (SPO) Diagnostics on AUG
GSI IPMs.
Electron Beam Diagnostics at REGAE
GPT Simulations of the Ion Source Beam
Time-Reversed Particle Simulations In GPT (or “There And Back Again”)
at Royal Holloway Univ. London
Physics design on Injector-1 RFQ
LumiCal mechanical design, integration with LDC and laser alignment
Spectrometer Layout (Isometric View)
Status of the Front End Test Stand April 2007.
Optimisation of the FETS RFQ
Application of a Streak camera at PITZ
H- Ion Source Development
J.B. Rosenzweig and Scott Anderson UCLA Dept. of Physics and Astronomy
Pepperpot MkII assembly
Electron cloud studies at CESR
Mechanical Engineering progress for the Front End Test Stand
Simon Jolly UKNFIC Meeting 25th April 2008
Experience with photoinjector at ATF
Presentation transcript:

Pepperpot Emittance Measurements of the FETS Ion Source Simon Jolly Imperial College 3rd October 2007

The Pepperpot Emittance Scanner Current slit-slit scanners give high resolution emittance measurements, but at fixed z-position, with x and y emittance uncorrelated. Correlated, 4-D profile (x, y, x’, y’) required for accurate simulations. Pepperpot reduces resolution to make correlated 4-D measurement. Moving stage allows measurement at different z-locations: space charge information. Possible to make time-resloved measurements within a single pulse. Added bonus: make high resolution x-y profile measurements. 3/10/07 Simon Jolly, Imperial College

Simon Jolly, Imperial College Pepperpot Principle Beam segmented by tungsten screen. Beamlets drift ~10mm before producing image on quartz screen. Copper block prevents beamlets from overlapping and provides cooling. CCD camera records image of light spots. Calculate emittance from spot distribution. Quartz screen Copper block Fast CCD Camera H- Ion Beam Tungsten screen H- Beamlets 3/10/07 Simon Jolly, Imperial College

Simon Jolly, Imperial College Pepperpot Components Pepperpot head: Tungsten intercepting screen, 50mm holes on 3mm pitch in 41x41 array. Tungsten sandwiched between 2mm/10mm copper support plates. Quartz scintillator images beamlets. Camera system: PCO 2000 camera with 2048 x 2048 pixel, 15.3 x 15.6 mm CCD. Firewire connection to PC. 105 mm Micro-Nikkor macro lens. Bellows maintains light tight path from vacuum window to camera. Main support: Head and camera mounted at either end of 1100 mm linear shift mechanism, with 700 mm stroke. All mounted to single 400 mm diameter vacuum flange. 3/10/07 Simon Jolly, Imperial College

Simon Jolly, Imperial College FETS Pepperpot Design Beam profile head Tungsten mesh Pepperpot head Shutter Bellows Camera Moving rod Vacuum bellows Mounting flange 3/10/07 Simon Jolly, Imperial College

Pepperpot Installation 3/10/07 Simon Jolly, Imperial College

ISDR Diagnostics X and Y Slit-Slit Emittance Scanners Buffer Gas Delivery System Movable Scintillator with Interchangeable Pepperpot or Profile Head Beam Current Toriod Diagnostic Dipole Beam Shutter Diagnostics Vessel 3/10/07 Simon Jolly, Imperial College

Simon Jolly, Imperial College Pepperpot Data Image Raw data Calibration image Colour enhanced raw data image, 60 x 60 mm2. Calibration image: use corners of 126 x 126 mm square on copper plate to give image scaling, tilt and spot spacing. 3/10/07 Simon Jolly, Imperial College

Pepperpot Emittance Extraction Emittance profiles X Y Pepperpot image spots: hole positions (blue) and beam spots (red) 3/10/07 Simon Jolly, Imperial College

Pepperpot GUI and Data Analysis 3/10/07 Simon Jolly, Imperial College

Position Variation for 13 kV Extract 0 mm 200 mm ex = 1.36 ey = 1.47 p mm mrad ex = 1.82 ey = 1.96 p mm mrad 100 mm 300 mm ex = 1.65 ey = 1.78 p mm mrad ex = 1.90 ey = 2.04 p mm mrad 3/10/07 Simon Jolly, Imperial College

Pepperpot/Profile Comparison 3/10/07 Simon Jolly, Imperial College

Pepperpot vs. Slit-Slit: 11kV X Emittance 0.39 p mm mrad 3/10/07 Simon Jolly, Imperial College

Pepperpot vs. Slit-Slit: 11kV Y Emittance 0.45 p mm mrad 3/10/07 Simon Jolly, Imperial College

Emittance Cut Optimisation As with Slit-Slit scanner, pepperpot emittance measurement is sensitive to cut level. Have to impose some sort of cut due to inherent 100 count noise from camera and background noise. Need to optimise cut level to give consistent emittance measurement. 3/10/07 Simon Jolly, Imperial College

Simon Jolly, Imperial College Pepperpot 11kV: 119/250 Cut 119 cut 250 cut 3/10/07 Simon Jolly, Imperial College

Scintillator Problems Pepperpot rapidly became “scintillator destruction rig”. Scintillator requirements: Fast (down to 500ns exposure). High light output. Survives beam (<1 micron stopping distance). High energy density from Bragg peak causes severe damage. Finally chose Ce-Quartz. 3/10/07 Simon Jolly, Imperial College

Ce-Quartz Decay: 1000 Images 3/10/07 Simon Jolly, Imperial College

Simon Jolly, Imperial College Conclusions 2-D profiles with high resolution (70 mm) Medium resolved 4-D emittance measurements (3 mm, 7 mrad). Both data can be combined to produce 4-D data with high resolution. Clear correlation between pepperpot, profile and slit-slit emittance measurements. Emittance measurements at different z-positions allow investigation of space charge forces. Able to output data into GPT and LINTRA simulations. 3/10/07 Simon Jolly, Imperial College