Optical BPM Progress A0 Photoinjector July 17th, 2009

Slides:



Advertisements
Similar presentations
Pulsed Fiber Laser Autocorrelator
Advertisements

Design and construction of a mid-IR SPIDER apparatus 09/10/2012 Malte Christian Brahms Imperial College London 09/10/20121.
Beam-based Measurements of HOMs in the HTC Adam Bartnik for ERL Team, Daniel Hall, John Dobbins, Mike Billing, Matthias Liepe, Ivan Bazarov.
Ray matrices The Gaussian beam Complex q and its propagation Ray-pulse “Kosten- bauder” matrices The prism pulse compressor Gaussian beam in space and.
Transparent Ring Interconnection Using Multi-wavelength Photonic switches WP 5 Transmultiplexers.
LC-ABD P.J. Phillips, W.A. Gillespie (University of Dundee) S. P. Jamison (ASTeC, Daresbury Laboratory) A.M. Macleod (University of Abertay) Collaborators.
05/03/2004 Measurement of Bunch Length Using Spectral Analysis of Incoherent Fluctuations Vadim Sajaev Advanced Photon Source Argonne National Laboratory.
Sub-picosecond Megavolt Electron Diffraction International Symposium on Molecular Spectroscopy June 21, 2006 Fedor Rudakov Department of Chemistry, Brown.
EOS at SPPS Adrian L Cavalieri, David M Fritz, SooHeyong Lee, Philip H Bucksbaum, David A Reis (FOCUS Center, University of Michigan) Holger Schlarb (DESY)
Ultrafast XUV Coherent Diffractive Imaging Xunyou GE, CEA Saclay Director : Hamed Merdji.
Philippe Hering October 30, 2007 Drive Laser Commissioning Results and Plans 1 Drive Laser Commissioning results and plans Philippe.
Part IV: Optical Spectroscopy of Solids
1 Injector Lasers Overview Sasha Gilevich, SLAC April 29, 2004 Drive Laser Specifications Challenges System Description Laser Procurement R&D Effort UV.
NLC - The Next Linear Collider Project  IR background issues and plans for Snowmass Jeff Gronberg/LLNL Linear Collider Workshop October 25, 2000.
Sasha GilevichFacilities Advisory Committee October Injector Drive Laser Update 1 Facilities Advisory Committee Meeting.
Autocorrelator:.
EMLAB 1 Power Flow and PML Placement in FDTD. EMLAB 2 Lecture Outline Review Total Power by Integrating the Poynting Vector Total Power by Plane Wave.
John Arthur LCLS Diagnostics and Commissioning September 22, 2004 Summary of Related Topics from the Miniworkshop on.
Fiber Bragg Gratings.
1 §5 Multiplexed and distributed sensors 1.Basic sensor array topologies 2.Time division multiplexing (TDM) 3.Wavelength division multiplexing (WDM) 4.Optical.
Optical Design Work for a Laser-Fiber Scanned
DMP Product Portfolio Femtosecond Lasers Trestles Ti:Sapphire lasers …… fs; nm, mW Mavericks Cr:Forsterite lasers
A 5 fs high average power OPCPA laser system for attosecond pulse production Philip Bates, Yunxin Tang, Emma Springate and Ian Ross Central Laser Facility,
Max-Born-Institut M.Boyle, A.Thoß, N.Zhavaronkov, G.Korn Max Born Institute; Max-Born-Str. 2A, Berlin, Germany T.Oksenhendler, D. Kaplan Fastlite,
CTF3 photo injector laser status CERN 17 July 2009 CLIC meeting.
PACS FM-ILT SPECTROMETER SPATIAL CALIBRATION A. Contursi (H. Feuchtgruber) PACS Science Verification Review – 8/9 November 2007 MPE-Garching.
Intra-cavity Pulse Shaping of Mode-locked Oscillators Shai Yefet, Naaman Amer and Avi Pe’er Department of physics and BINA Center of nano-technology, Bar-Ilan.
C. Vicario LCLS ICW SLAC Oct. 9-11, THE DRIVE LASER: EXPERIENCE AT SPARC Carlo Vicario for SPARC collaboration.
Femto-second Measurements of Semiconductor Laser Diodes David Baxter
SPPS, Beam stability and pulse-to-pulse jitter Patrick Krejcik For the SPPS collaboration Zeuthen Workshop on Start-to-End Simulations of X-ray FEL’s August.
AAC February 4-6, 2003 Protons on Target Ioanis Kourbanis MI/Beams.
Status Brussels GANTRY Ê Try to assemble modules with good precision 4 different calibration plates (Karlsruhe and Bari) 4 determination of pin positions.
PACS Spectrometer Spatial Calibration plan in PV phase A.Contursi D. Lutz and U. Klaas.
ACFA-7; Taipei, Nov 2004 H.Weerts status Si licon D etector Status H.Weerts Fermilab/Michigan State Univ. (Progress on Si-tracker layout)
EO sampling technique for femtosecond beam characterization
July 19, 2006VLCW-06 Vancouver1 Scint/MAPMT Muon Prototype Operation Robert Abrams Indiana University.
Managed by UT-Battelle for the Department of Energy Analysis of 2008 Beam Instability Data S. Cousineau, V. Danilov, M. Plum HB2008.
Femtosecond Laser Spectroscopy of C 60 Nieuwegein, The Netherlands August 21, 2001 Eleanor Campbell, Göteborg University & Chalmers, Sweden R.D. Levine,
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 Shaping with MIIPS SASS 8/22/2012 David Nicholson.
Laser system for ILC diagnostics Sudhir Dixit: The John Adams Institute (Oxford)
Extreme Light Infrastructure in Romania: progress Daniel URSESCU Technical contact point for ELI in Romania INFLPR, Magurele, Romania.
W.S. Graves 2002 Berlin CSR workshop 1 Microbunching and CSR experiments at BNL’s Source Development Lab William S. Graves ICFA CSR Workshop Berlin, Jan.,
Workshop for advanced THz and Compton X-ray generation
Electro-optic Longitudinal Profile Diagnostics S P Jamison, Accelerator Science and Technology Centre, STFC Daresbury Laboratory S.P. Jamison, Daresbury.
Space-time analogy True for all pulse/beam shapes
XBSM Analysis - Dan Peterson Review of the optics elements: Pinhole (“GAP”), FZP, Coded Aperture Extracting information from the GAP what is the GAP width?
WACH4 26/11/2002Julien Cogan CERN/EP/CMA-1- THERMAL STEPS ANALYSIS Goals & Means : –apply a “step function” on the cooling water –look at : APD response.
Single-shot, Sub-picosecond, EO bunch measurements at FELIX Steven Jamison, Giel Berden, Allan MacLeod Allan Gillespie, Jingling Shen, Dino Jaroszynski,
10fs laser pulse propagation in air Conclusion The properties of femtosecond laser pulse propagation over a long distance (up to 100m) were studied for.
Laser Arm for Photo-injector Mikhail Martyanov, Valentin Fedosseev, Christoph Hessler AWAKE PEB meeting , CERN.
LASER SYSTEM STATUS G.Gatti, A. Ghigo, C.Vicario, P.Musumeci, M. Petrarca, S. Cialdi, D. Filippetto REVIEW COMMITTEE 16/11/05.
SRI 2007: CLS Optical Metrology Facility- Overview
Status of the SPARC laser and “dazzler” experiments
Seeding in the presence of microbunching
SPARC Review Committee
Analysis of 14/20 mrad Extraction Line Energy Chicane
Kansas State University
Milano Laser Pulse Shaping group
Electro Optic Sampling of Ultrashort Mid-IR/THz Pulses
Introduction to MOSAIC, SHG-FROG, and GRENOUILLE
Principle of Mode Locking
Kansas Light Source Upgrade
Laser-assisted photoionization for attosecond pulse measurements
XFEL bunch compressors
Space-time analogy True for all pulse/beam shapes
LASER SYSTEM STATUS G.Gatti , A. Ghigo , C.Vicario , P.Musumeci ,
Linac Diagnostics Patrick Krejcik, SLAC April 24, 2002
Breakout Sessions SC1/SC2 – Accelerator Physics
LCLS Injector Laser System Paul R. Bolton, SLAC April 24, 2002
Presentation transcript:

Optical BPM Progress A0 Photoinjector July 17th, 2009 Tim Maxwell, Jinhao Ruan, Philippe Piot & Mike Church

Optics Status and Roadmap 1) Laser Autocorrelator (SHG) For single-shot laser pulse duration measurement Also for synchronizing laser pulses Now assembled and functioning 2) Frequency Resolved Optical Gating (FROG) An autocorrelator with a diffraction grating Measures λ vs. t shot-to-shot (duration and chirp) Kit awaiting assembly pending study of autocorrelator

Optics Status and Roadmap 3) Fiber Transport For IR laser transport line from laser room to cave Fibers and launch optics ready Need FROG to characterize fiber dispersion effects 4) Laser pulse stretcher (and compressor) Introduce chirp for EO spectral encoding Help compensate for fiber dispersion Above experiments needed to proceed Fiber measurements to determine compensation needed FROG to verify performance

Single-shot autocorrelator Autocorrelator based on ~SHG and spatial encoding When pulses cross simultaneously (brightest and centered blue spot) blue stripe is autocorrelation of pulse Split laser pulse, duration (thickness) exaggerated BBO Crystal

Single-shot autocorrelator Second-best layout Half angle between lasers at crystal of ~19° ~ Revised layout Half angle between lasers at crystal of ~9° ~ ~ ~ ~

Single-shot autocorrelator

Single-shot autocorrelator For single-shot mode, scan delay to find peak signal and find… First result last night (7/16/09)

Single-shot autocorrelator Finding time axis calibration factor Convert micro controller position to time delay: Δt = 2 Δx / c Scan stepper recording spot centroid as a function of delay Slope of centroid position vs. delay yields conversion pix to sec Centroid calculated two ways: Brightest horizontal trace X projection Projection shows roll off in this result (no background correction). Used linear region of “Trace” Preliminary calibration: 2.5 fs / pix

Preliminary first results Revisiting peak horizontal trace and x projection from earlier: RMS laser pulse length 140 fs …if only I had also measured the bandwidth for comparison.

Conclusions Autocorrelator up and running and seems to work well so far Clean up the control and analysis scripts (Matlab) Compare single-shot method (shown here) with scanning method Vary Ti:Sapph bandwidth and measure pulse length We had to cut incidence angle in half Should be able to use bigger angle according to theory Did I just not see the dot in original set up? Want bigger angle for in-pipe autocorrelator! When done with initial exploration, attempt larger angle again? Extend into Frequncy Resolved Optical Gating with the kit Assemble and test remaining optics for EO experiment, as mentioned Somewhat unrelated: Also still looking into wake filed calculations for the proposed EO pipe section…