Recent development of the Supersonic Gas-Jet Beam profile monitor

Slides:



Advertisements
Similar presentations
Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.
Advertisements

High Pressure Plasma with a third electrode James Roberts Physics TSP 2002 Supervised by Dr Kerrie Balla.
Joe Vinen Workshop on New Experimental Techniques for the Study of Quantum Turbulence, ICTP, Trieste, June 2005 Metastable He molecules and laser-induced.
Ta-Te Lin, Yi-Chung Chang
Laboratory experiments on positive streamer properties S. Nijdam 1, E.M. van Veldhuizen 1, U. Ebert 1,2 1 ) Eindhoven University of Technology, Department.
A Proof-of Principle Study of 2D optical streaking for ultra-short e-beam diagnostics using ionization electrons & circular polarized laser Lanfa Wang.
PS wirescanner calibration Student Meeting 10/03/2014 Carolina Bianchini BE-BI-BL.
LHC Collimation Working Group – 19 December 2011 Modeling and Simulation of Beam Losses during Collimator Alignment (Preliminary Work) G. Valentino With.
D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,
Excited state spatial distributions Graham Lochead 20/06/11.
HIGH RESOLUTION INFRARED SPECTROSCOPY OF N 2 O-C 4 H 2 AND CS 2 −C 2 D 2 DIMERS MAHDI YOUSEFI S. SHEYBANI-DELOUI JALAL NOROOZ OLIAEE BOB MCKELLAR NASSER.
The 2nd Tevatron Electron Lens and tests of a new electron gun in the framework of Beam-Beam Compensation project Yu. Alexahin, V. Kamerdzhiev, G. Kuznetsov,
Beam profile measurements based on modern vertex detectors and beam-gas interactions Slides from: Colin Barschel - TIPP 2014 third international conference.
Pre-formed channels for laser-plasma accelerators Euroleap kickoff meeting May, 2006, Orsay, France N. C. Lopes Grupo de Lasers e Plasmas Instituto Superior.
Pro-Science 4 th International Conference of Hydrogen Safety, September 12-14, 2011, SAN FRANCISCO, USA EXPERIMENTAL STUDY OF IGNITED UNSTEADY HYDROGEN.
1 Plans for KEK/ATF 1. Introduction 2. Related Instrumentations at ATF 3. Experimental Plans for Fast Kicker R&D at ATF Junji Urakawa (KEK) at ILC Damping.
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 *
Ultra-thin Gas Jet for Non-Invasive Beam Halo Measurement Adam Jeff CERN & University of Liverpool Workshop on Beam Halo Monitoring 19th September 2014.
BROOKHAVEN SCIENCE ASSOCIATES BIW ’ 06 Lepton Beam Emittance Instrumentation Igor Pinayev National Synchrotron Light Source BNL, Upton, NY.
A. Doyuran, L. DiMauro, W. Graves, R. Heese, E. D. Johnson, S. Krinsky, H. Loos, J.B. Murphy, G. Rakowsky, J. Rose, T. Shaftan, B. Sheehy, Y. Shen, J.
Transverse Profiling of an Intense FEL X-Ray Beam Using a Probe Electron Beam Patrick Krejcik SLAC National Accelerator Laboratory.
1 Ab initio and Infrared Studies of Carbon Dioxide Containing Complex Zheng Su and Yunjie Xu Department of Chemistry, University of Alberta, Edmonton,
Beam diagnostics in the beamlines
Assessing Single Crystal Diamond Quality
Institute of Atomic and Molecular Sciences, Academia Sinica, Taiwan National Taiwan University, Taiwan National Central University, Taiwan National Chung.
Nonlinear Optics in Plasmas. What is relativistic self-guiding? Ponderomotive self-channeling resulting from expulsion of electrons on axis Relativistic.
Experimental and Numerical studies on Bulk Micromegas SINP group in RD51 Applied Nuclear Physics Division Saha Institute of Nuclear Physics Kolkata, West.
Shan Liu, Philip Bambade, Sha Bai, Dou Wang, Illia Khvastunov ECFA, Hamburg, 29 May, 2013.
Mitglied der Helmholtz-Gemeinschaft Calibration of the COSY-TOF STT & pp Elastic Analysis Sedigheh Jowzaee IKP Group Talk 11 July 2013.
Tests of AWAKE spectrometer screen and camera at PHIN Introduction Layout Procedure Setup, results (runs 1 – 5) Conclusions L. Deacon, S. Mazzoni, B. Biskup.
PULSE LASER WIRE Laser pulse storage in an optical cavity as a beam monitor & an X-ray source Kaori Takezawa Kyoto Univ. 2nd Mini-Workshop on Nano Project.
E-217 FACET users meeting 9/15/14 Ken Marsh. What happens to the experiment when laser fires full power in Lithium? Do we ionize the helium buffer zones?
The 21st International Conference on Ultrarelativistic nucleus-nucleus collisions, March 30 – April 4, Knoxville, TN Results from cosmics and First LHC.
ATF2 background and beam halo study D. Wang(IHEP), S. Bai(IHEP), P. bambade(LAL) February 7, 2013.
A Stark decelerator for ammonia molecules
Christoph Gabor, ASTeC HIPPI—Meeting (WP 5) 26 th – 28 th September 2007 Non—destructive transverse emittance measurement device The Front End Test Stand.
 The zigzag readout board is divided into eight η-sectors; each sector has a length of ~12 cm and comprises 128 zigzag strips; zigzag strips run in radial.
02/04/2009 AS-TAGL Mtg Global Design Effort 1 CesrTA Update Mark Palmer CLASSE.
Zone plates for gas-jet focusing
- 9 th Sep Introduction Gas-Jet Simulations Experimental Setup Massimiliano Putignano Development of a Beam Profile Monitor Based on a Supersonic.
Abstract Beam Test of a Large-area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System V. Bhopatkar, M. Hohlmann, M. Phipps, J. Twigger,
Mitglied der Helmholtz-Gemeinschaft Jörg Wolters, Michael Butzek Focused Cross Flow LBE Target for ESS 4th HPTW, Malmö, 3 May 2011.
1 Fast kicker study Machine Time 2011/10/18~10/29(2 weeks) TB meeting 2011/01/14 T.Naito.
Electron Spectrometer: Status July 14 Simon Jolly, Lawrence Deacon 1 st July 2014.
A Stark decelerator for ammonia molecules Ruth Buning Master research project February 23, 2007.
1 BROOKHAVEN SCIENCE ASSOCIATES Vibrations effect on 1nm focussing K. Evans-Lutterodt NSLS-II VTG Januaury
1 James N. Bellinger Robert Handler University of Wisconsin-Madison 11-Monday-2009 Laser fan non-linearity James N. Bellinger 20-March-2009.
3M Drug Delivery Systems 3 Chris Blatchford & Gemma Nixon, 3M Drug Delivery Systems, Morley St, Loughborough, UK. Graham Hargrave, Tim Justham & Edward.
Cluster-Jet Target Target TDR Alfons Khoukaz Institut für Kernphysik, WWU Münster, Germany PANDA Collaboration Meeting December 8-12, 2008.
Systematic studies on pellet beam production M.Büscher, A.Gerasimov, V.Chernetsky, P.Fedorets, A.Dolgolenko,V.Balanutsa, A.Boukharov, L.Gusev, S. Mineev,
Benchmarking simulations and observations at the LHC Octavio Domínguez Acknowledgments: G. Arduini, G. Bregliozzi, E. Métral, G. Rumolo, D. Schulte and.
ESS | Non-Invasive Beam Profile Measurements| | C. Böhme Non-Invasive Beam Profile Measurement Overview of evaluated methods.
Best Practice T-Scan5 Version T-Scan 5 vs. TS50-A PropertiesTS50-AT-Scan 5 Range51 – 119mm (stand- off 80mm / total 68mm) 94 – 194mm (stand-off.
Optical Diagnostics State of the art and Future Trends Prof. Carsten P. Welsch.
Dissociation of Molecular Ions Studied by
Dr Andrew French P5/6 Winchester College
Gas jet based diagnostics for beam monitoring
Resume of the experimental program up to date
HPR activities at INFN Milan
DITANET Conference, Seville, Spain
Summary of activities of the pellet target development
Production and commissioning of the 2nd BGC
IHEP group Shashlyk activity towards TDR
Numerical model for simulation of the Micro-Channel Plates
High harmonic generation in a large-volume capillary for seeding of free-electron lasers Siew Jean Goh.
Transverse size and distribution of FEL x-ray radiation of the LCLS
Linac Diagnostics Commissioning Experience
BGC Collaboration Meeting –
Design Studies of a Microwave-driven Ion Source
Presentation transcript:

Recent development of the Supersonic Gas-Jet Beam profile monitor Dr. Hao Zhang

Outline Motivation Experimental Setup Skimmer size and resolution Jet distribution measurement

Motivation Diagnose the particle beam non-invasively Preserve the vacuum more effectively Better understand the gas-jet dynamics when using this monitor

Get-jet Monitor Setup

Generation of Supersonic Gas jet* Pb For our case, P0 = 5 bar, Pb ~ 1.0e-3 mbar => xM/d = 1500; d =30mm=> xM = 45 mm *

Skimmers & MCP V. Tzoganis, et al. IPAC2013

2-dimentional profile imaging Y X V. Tzoganis, et al. IPAC2013

Resolution VS 3rd skimmer size Beam size mm sx (Gas jet) 0.42 0.56 sy (Gas jet) 1.23 0.53 sx (Residual Gas) 1.01 1.52 Skimmer size 7.2×1.8 mm2 4×0.4 mm2 Oriental angle 45˚ 32˚

Smaller 3rd skimmer Skimmer size 4×0.4 mm2 Oriental angle 32˚ Beam size mm sx (Gas jet) 0.56 ± 0.02 sy (Gas jet) 0.53 ± 0.03 sx (Residual Gas) 1.52 ± 0.07

Can we go even smaller?? Fresnel zone plate Largest hole size is less than 2 micron for our case Fresnel zone plate Photon sieve,

Fresnel zone plate Currently installed to replace the 3rd skimmer. But initial test shows no image from the micron jet. Possible reason: The gas is not fully monochromatic. We might not get the focus in the electron beam region. The focus length f ~ 1/ λ ~ sqrt(m*T), so lower the gas temperature, lower the focus length. The supersonic gas molecule's temperature is unknown. The density of the gas jet is too low to detect.

Resolution problem Particle beam Beam size 1 Beam size 2 Gas jet curtain ?! The gas curtain distribution will affect the resolution of this method. Having a method to know the pressure distribution of the system will help us understand the gas curtain distribution better.

Last update: Moveable Through Gauge module Alignment is based on both the laser and gas-jet image, but the measured pressure curve is still due to the pressure raising of the chamber as a whole instead of the jet itself New Moveable gauge chamber is added

Measurement from the previous through Gauge Plot of the max-min pressure of the subtracted data VS the Gauge horizontal location

Newly installed compression gauge module Slit Compression Gauge Module Gas jet curtain Slit size 10.0 × 2.0 mm2

First meaningful result The blue curve represent the case when partial of the jet enters the compression gauge module through the slit, while the purple one shows the case that there is no jet entering the slit and the pressure bump is from the overall pressure change due to the jet flowing into the first dump chamber

Vertical Scan

Gaussian fit s (mm) 1.01

Automation for moveable Gauge Scan Scope Camera Master Trigger PC Pico-Current Meter Pulse Generator Relay Pulse Valve 24V DC Voltage Supply Moveable Gauge

Time Sequence Take photos (Matlab controlled software trigger) Pulse valve open (Pulse generator) Move gauge position by step motor(Matlab Controlled) 4.0 s delay (pulse generator) 10.0 s delay 4.0 s delay Scope start (Matlab Controlled) Pulse generated by Camera strobe (Matlab Controlled) Scope stop and transfer data (Matlab Controlled)

2D Scan 7.5 mm About 32˚ 6.0 mm

Mach Disc study Pb For our case, P0 = 5 bar, Pb ~ 1.0e-3 mbar => xM/d = 1500; d =30mm=> xM = 45 mm From

Gauge pressure VS Nozzle skimmer distance This curve give a Mach disk about 25 mm, which is in the same order of magnitude with the calculation.

Conclusion and Future Work Summary By reducing the 3rd skimmer size, we improve the resolution of the jet image. Developed a moveable compression gauge module to measure the jet distribution. Automated the moveable gauge measurement process Preliminary result of the jet distribution agree with the setup Gas dynamics study about the Mach disk.

Any Questions? Thank you