Photon Diagnostic Station For TAC IR-FEL Test Facility ILHAN TAPAN* *on behalf of the TAC collaboration Uludag Universitesi, Bursa,16059, TURKEY References.

Slides:



Advertisements
Similar presentations
DL/RAL Joint Accelerator Workshop 21 st January 2009 Free Electron Laser Studies David Dunning MaRS ASTeC STFC Daresbury Laboratory.
Advertisements

C. McGuffey a, W. Schumaker a, S. Kneip b, F. Dollar a, A. Maksimchuk a, A. G. R. Thomas a, and K. Krushelnick a (a) University of Michigan, Center for.
05/03/2004 Measurement of Bunch Length Using Spectral Analysis of Incoherent Fluctuations Vadim Sajaev Advanced Photon Source Argonne National Laboratory.
1 Electron Beam Polarimetry for EIC/eRHIC W. Lorenzon (Michigan) Introduction Polarimetry at HERA Lessons learned from HERA Polarimetry at EIC.
Necessity of Moving from Green Book to White Book M. Hadi Hadizadeh Yazdi International Scientific Meetings Office Iran October 26, 2002 Amman, Jordan.
1 Extreme Ultraviolet Polarimetry Utilizing Laser-Generated High- Order Harmonics N. Brimhall, M. Turner, N. Herrick, D. Allred, R. S. Turley, M. Ware,
Sept. 18, 2008SLUO 2008 Annual Meeting Vision for SLAC Science Persis S. Drell Director SLAC.
FLASH Experiments with Photons High intensity laser light in the VUV spectral region Harald Redlin; HASYLAB.
1 A Grating Spectrograph for the LCLS Philip Heimann Advanced Light Source Observe the spontaneous radiation spectrum of the individual undulators Observe.
UCLA The X-ray Free-electron Laser: Exploring Matter at the angstrom- femtosecond Space and Time Scales C. Pellegrini UCLA/SLAC 2C. Pellegrini, August.
SLAC XFEL Short Bunch Measurement and Timing Workshop 1 Current status of the FERMI project (slides provided by Rene Bakker) Photoinjector laser system.
Slide 1 George R. Neil Associate Director Jefferson Lab Jefferson Avenue Newport News, Virginia VUV Program Directors Review Plans for a VUV.
Electromagnetic radiation sources based on relativistic electron and ion beams E.G.Bessonov 1.Introduction 2.Spontaneous and stimulated emission of electromagnetic.
BROOKHAVEN SCIENCE ASSOCIATES BIW ’ 06 Lepton Beam Emittance Instrumentation Igor Pinayev National Synchrotron Light Source BNL, Upton, NY.
W.S. Graves1 Seeding for Fully Coherent Beams William S. Graves MIT-Bates Presented at MIT x-ray laser user program review July 1, 2003.
Low Emittance RF Gun Developments for PAL-XFEL
Femto-second Measurements of Semiconductor Laser Diodes David Baxter
Properties of Synchrotron Radiation Presentation at JASS02 Seminar; Jordan, Oct , 2002 Herman Winick, SSRL/SLAC, Stanford University.
M.TURALICPP 2008, Boğaziçi University1 RESEARCH POTENTIAL OF TAC IR FEL FACILITY Müge TURAL Ankara University October 30, 2008.
Synchronisation Activities for 4GLS Supported by EUROFEL DS3 G J Hirst CCLRC Central Laser Facility.
First Lasing of the ALICE Free Electron Laser David Dunning On behalf of the ALICE FEL team (Jim Clarke, Neil Thompson, Mark Surman and Andy Smith), and.
Transverse Profiling of an Intense FEL X-Ray Beam Using a Probe Electron Beam Patrick Krejcik SLAC National Accelerator Laboratory.
W.S. Graves ASAC Review Sept 18-19, 2003 R&D at Bates William S. Graves MIT-Bates Laboratory Presentation to MIT X-ray laser Accelerator Science Advisory.
Free-Electron Laser at the TESLA Test Facility More than 50 institutes from 12 countries are involved in the TESLA Project The TESLA Collaboration: Three.
ESFRI & e-Infrastructure Collaborations, EGEE’09 Krzysztof Wrona September 21 st, 2009 European XFEL.
Beam Dynamics and FEL Simulations for FLASH Igor Zagorodnov and Martin Dohlus Beam Dynamics Meeting, DESY.
Turkish Accelerator and Radiation Laboratory at Ankara Suat ÖZKORUCUKLU İstanbul University.
Lighting the path to innovation Australian Synchrotron What is a synchrotron & how does it work?
The SPARX FEL Project a source for coherent radiation production in the soft X-ray energy range.
ERHIC with Self-Polarizing Electron Ring V.Ptitsyn, J.Kewisch, B.Parker, S.Peggs, D.Trbojevic, BNL, USA D.E.Berkaev, I.A.Koop, A.V.Otboev, Yu.M.Shatunov,
X-RAY LIGHT SOURCE BY INVERSE COMPTON SCATTERING OF CSR FLS Mar. 6 Miho Shimada High Energy Research Accelerator Organization, KEK.
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS-II Overview Satoshi Ozaki Director, Accelerator Systems Division NSLS-II Project March 27, 2007.
ERHIC design status V.Ptitsyn for the eRHIC design team.
Max Cornacchia, SLAC LCLS Project Overview BESAC, Feb , 2001 LCLS Project Overview What is the LCLS ? Transition from 3 rd generation light sources.
Basic Energy Sciences Advisory Committee MeetingLCLS February 26, 2001 J. Hastings Brookhaven National Laboratory LCLS Scientific Program X-Ray Laser Physics:
Adams Accelerator Institute 10 - E. Wilson - 1/24/ Slide 1 Lecture 14 ACCELERATOR PHYSICS MT 2004 E. J. N. Wilson.
DESY Deutsches Electron Synchrotron Shima Bayesteh.
Workshop for advanced THz and Compton X-ray generation
The Next Generation Light Source Test Facility at Daresbury Jim Clarke ASTeC, STFC Daresbury Laboratory Ultra Bright Electron Sources Workshop, Daresbury,
TAC SASE FEL Project Dr. Ömer Yavaş * Ankara University * On behalf of TAC SASE FEL Study Group Meeting on the Feasibility of X-Band Linac Based FEL Facility.
Lessons Learned From the First Operation of the LCLS for Users Presented by Josef Frisch For the LCLS March 14, 2010.
J. Corlett. June 16, 2006 A Future Light Source for LBNL Facility Vision and R&D plan John Corlett ALS Scientific Advisory Committee Meeting June 16, 2006.
Experience with Novosibirsk FEL Getmanov Yaroslav Budker INP, Russia Dec. 2012, Berlin, Germany Unwanted Beam Workshop.
Operational experience and recent results from FLASH (VUV FEL at DESY) E. Saldin, E. Schneidmiller and M. Yurkov for FLASH team Milestones Parameters of.
BINP tau charm plans and other projects in Turkey/China A. Bogomyagkov BINP SB RAS, Novosibirsk.
Coherent THz radiation source driven by pre-bunched electron beam
Overview Turkish Projects TAC / TARLA Avni Aksoy Ankara University Institute of Accelerator Technologies.
ESLS Workshop Nov 2015 MAX IV 3 GeV Ring Commissioning Pedro F. Tavares & Åke Andersson, on behalf of the whole MAX IV team.
Capabilities and Programmes of STFC’s Accelerator Science & Technology Centre (ASTeC)
Free Electron Laser Studies
Status of the SPARC laser and “dazzler” experiments
Contribution of Ankara University Accelerator Technology Institute
Paper: Acoustic Injectors for Drop-On-Demand Serial
MSc-Student Activities at the European XFEL
Tunable Electron Bunch Train Generation at Tsinghua University
Irradiation Facilities Questionnaire
Two color FEL experiment
Musings For Future Challenge
LCLS-II-HE FEL Facility Overview
Free Electron Lasers (FEL’s)
XAFS Spectroscopy Katarina Norén 23/11/2018.
LCLS-II-HE FEL Facility Overview
ERL accelerator review. Parameters for a Compton source
LCLS bunch length monitor utilizing coherent radiation
Jim Clarke ASTeC Daresbury Laboratory March 2006
WELCOME TO SOLEIL Amor Nadji On behalf of Synchrotron SOLEIL
X-Ray Transport, Optics, and Diagnostics WBS Alan J
PbWO4 Cherenkov light contribution to Hamamatsu S8148 and Zinc Sulfide–Silicon avalanche photodiodes signals F. KOCAK, I. TAPAN Department of Physics,
Optics John Arthur, SLAC & William W. Craig, LLNL April 24, 2002
Introduction to Free Electron Lasers Zhirong Huang
Presentation transcript:

Photon Diagnostic Station For TAC IR-FEL Test Facility ILHAN TAPAN* *on behalf of the TAC collaboration Uludag Universitesi, Bursa,16059, TURKEY References [1] S. Sultansoy et al., “The Status of Turkic Accelerator Complex Proposal”, Proceedings of PAC 05, p [2] W. Seidel et al., “Remote Controlled IR- Diagnostic Station For the FEL at Rossendorf ”, Proceedings of FEL 06, p General layout for the main parameters for the TAC IR FEL can be given as follows: - Wavelength region: between micron - Pulse structure: around ps - Micro pulse energy: around 13 MHz (S.c. RF) - Average power: few W - Average flux: around photons/s.eV Despite the strong competition from conventional lasers, the FEL is recognized as important tool for various scientific applications. Today, there are about 40 FEL facilities wordwide. The TAC IR-FEL test facility will be the first and unique one for Turkey and our region. In this presentation, the general plan for the TAC IR-FEL photon beam diagnostic station will be introduced. Acknowledgment This work is supported by Turkish State Planning Organization (DPT) under the grant DPT2006K Introduction The optical beam diagnostic station has been designed to properly characterize laser beam for user experiments and to diagnose beam properties for tuning of the undulators (undulator 1 and undulator 2). The IR-FEL photons generated by two undulators will be transported to the experimental hall through the respective two photon beam lines by using reflective optics. The high reflectivity IR mirrors coated with Al, Au, Ag will be use to transport and focus the beam with other optical lenses. The diagnostic station will be located in the experimental hall. Both FEL beam lines will be merged on the diagnostic table and delivered to eight user laboratories. Mirrors, crystal optics and beam splitters will be employed on a granite table to guide the photon beams to separate spectrometer and different kind of detectors. TAC IR-FEL Test Facility The TAC IR-FEL test facility will be an oscillator FEL that provides the laser beams in mid and far infrared region. It includes electron source, two RF modules to get 15 to 40 MeV electron beam and two undulators to obtain laser beam in the wavelength region of 1 to 200 microns. The schematic view of the TAC IR-FEL test laboratory The Turkic Accelerator Center (TAC) project was started as a regional facility for accelerator based fundamental and applied research [1]. The work has been ongoing by ten Turkish Universities collaboration with the support of State Planning Organization (DPT). The (TAC) project will include: - light sources (synchrotron radiation and free electron laser) - electron-positron collider - GEV scale proton accelerator As a first step of the project, a linac-based infrared free electron laser (IR- FEL) will be constructed as a TAC test facility to produce tuneable, coherent light with high flux which is around photons/s.eV and high brightness by the end of Photon Diagnostic Station The optical components and devices on the diagnostic table The TAC IR-FEL diagnostic table has been designed similar to that of the ELBE radiation source in Dresden[2]. According to this design: - A non-collinear background free autocorrelator will be used to characterize the optical micro pulse duration. By using a CdTe single-crystal for second harmonic generation, a broad wavelength coverage will be obtained. - A Czerny-Turner type spectrometer which contains a turret with three different gratings will be used for the spectrum measurements. - A long wavelength MCT (HgCdTe) detector and a Pyro detector will be used in the diagnostic system for gain and loss measurements with higher sensitivity in the whole range of the FEL spectrum. - A thin metal attenuators will be used to reduce average FEL power for the users.