THE CSU ADVANCED BEAM LABORATORY (ABL) Sandra Biedron 1.

Slides:



Advertisements
Similar presentations
Vulcan Front End OPCPA System
Advertisements

Ultrafast Experiments Hao Hu The University of Tennessee Department of Physics and Astronomy, Knoxville Course: Advanced Solid State Physics II (Spring.
KEK : Novel Accelerator TYL Workshop M. Yoshida, M. Nozaki, K. Koyama, High energy research organization (KEK) -Collaboration -IZEST (CEA) :
Coherent Radiation from High-Current Electron Beams of a Linear Accelerator and Its Applications S. Okuda ISIR, Osaka Univ Research Institute.
AREAL Laser overview Advanced Research Electron Accelerator Laboratory Aghasi Lorsabyan.
1 Enhancements to the Linac Coherent Light Source.
Thomson Scattering X-ray Source at Tsinghua University
UCLA The X-ray Free-electron Laser: Exploring Matter at the angstrom- femtosecond Space and Time Scales C. Pellegrini UCLA/SLAC 2C. Pellegrini, August.
Before aperture After aperture Faraday Cup Trigger Photodiode Laser Energy Meter Phosphor Screen Solenoids Successful Initial X-Band Photoinjector Electron.
SLAC XFEL Short Bunch Measurement and Timing Workshop 1 Current status of the FERMI project (slides provided by Rene Bakker) Photoinjector laser system.
DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. THE CSU ACCELERATOR LABORATORY Stephen Milton 1.
Beam Diagnostics Collaboration Meeting March 18 th 2015 at Australian Synchrotron Mario Ferianis – Elettra.
The UCLA PEGASUS Plane-Wave Transformer Photoinjector G. Travish, G. Andonian, P. Frigola, S. Reiche, J. Rosenzweig, and S. Telfer UCLA Department of Physics.
Progress at the XFELs in Europe and Japan Hans-H. Braun, PSI 48 th ICFA Advanced Beam Dynamics Workshop on Future Light Sources March 1-5, 2010 SLAC National.
Photon Diagnostic Station For TAC IR-FEL Test Facility ILHAN TAPAN* *on behalf of the TAC collaboration Uludag Universitesi, Bursa,16059, TURKEY References.
Low Emittance RF Gun Developments for PAL-XFEL
R&D Towards X-ray Free Electron Laser Li Hua Yu Brookhaven National Laboratory 1/23/2004.
High Current Electron Source for Cooling Jefferson Lab Internal MEIC Accelerator Design Review January 17, 2014 Riad Suleiman.
LCLS Accelerator SLAC linac tunnel research yard Linac-0 L =6 m Linac-1 L  9 m  rf   25° Linac-2 L  330 m  rf   41° Linac-3 L  550 m  rf  0°
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.
FLASH II. The results from FLASH II tests Sven Ackermann FEL seminar Hamburg, April 23 th, 2013.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
Brief Introduction to (VUV/)Soft X-ray FELs R. P. Walker Diamond Light Source, UK ICFA Workshop on Future Light Sources March 5 th -9 th, 2012 Thomas Jefferson.
9/24-26/07 e- KOM Slide 1/20 ILC Polarized e- source RDR Overview A. Brachmann.
PBG Structure Experiments, AAC 2008 Photonic Bandgap Accelerator Experiments Roark A. Marsh, Michael A. Shapiro, Richard J. Temkin Massachusetts Institute.
Max Cornacchia, SLAC LCLS Project Overview BESAC, Feb , 2001 LCLS Project Overview What is the LCLS ? Transition from 3 rd generation light sources.
Measurements of the X-ray/pump laser pulse timing Valery Dolgashev, David Fritz, Yiping Feng, Gordon Bowden SLAC 48th ICFA Advanced Beam Dynamics Workshop.
Laboratoire de Chimie-Physique CNRS – Université Paris-Sud UMR ORSAY Cs 2 Te photocathodes at ELYSE.
MP - HIPPI General meeting, Abingdon October 28-30, Side Coupled Linac Design at CERN Side Coupled Linac Design at CERN M. Pasini, Abingdon September.
TOWARD GENERATION OF HIGH POWER ULTRAFAST WHITE LIGHT LASER USING FEMTOSECOND TERAWATT LASER IN A GAS-FILLED HOLLOW-CORE FIBER Walid Tawfik Physics and.
Workshop for advanced THz and Compton X-ray generation
Velocity bunching from S-band photoinjectors Julian McKenzie 1 st July 2011 Ultra Bright Electron Sources Workshop Cockcroft Institute STFC Daresbury Laboratory,
Commissioning and Utilisation of ERLP David Holder ASTeC, Daresbury Laboratory.
The Next Generation Light Source Test Facility at Daresbury Jim Clarke ASTeC, STFC Daresbury Laboratory Ultra Bright Electron Sources Workshop, Daresbury,
UCLA Claudio Pellegrini UCLA Department of Physics and Astronomy X-ray Free-electron Lasers Ultra-fast Dynamic Imaging of Matter II Ischia, Italy, 4/30-5/3/
WP8-HGA High Gradient Acceleration M. Biagini (INFN-LNF) WP8 coordinator Tiara Kickoff Meeting, CERN, Feb , 2011.
1 CTF3 CLEX day July 2006 CLEX day 2006 Introduction G.Geschonke CERN.
김 귀년 CHEP, KNU Accelerator Activities in Korea for ILC.
Awake electron beam requirements ParameterBaseline Phase 2Range to check Beam Energy16 MeV MeV Energy spread (  ) 0.5 %< 0.5 % ? Bunch Length (
Laser-driven Terahertz frequency transverse deflectors (?) Steven Jamison Accelerator Science and Technology Centre (ASTeC) STFC Daresbury Laboratory S.P.
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.
Room-temperature Burst-mode GHz and THz Pulse Rate Photoinjector for Future Light Sources Yen-Chieh Huang * Chia-Hsiang Chen, Kuan-Yan Huang, Fu-Han Chao.
X-band Based FEL proposal
1 st TIARA Steering Committee A. Gallo – INFN Frascati deputy of TIARA WP8 leader STATUS OF TIARA WP8.
NLCTA Facility Capabilities E. R. Colby 5/18/09. NLCTA Overview RF PhotoInjector Ti:Sapphire Laser System Next Linear Collider Test Accelerator Cl. 10,000.
November 17, 2008 A. Brachmann Slide 1 ILC polarized Electron Source R&D Update LCWS 2008 A. Brachmann, J. Sheppard, F. Zhou - SLAC National Accelerator.
High-efficiency L-band klystron development for the CLIC Drive Beam High-efficiency L-band klystron development for the CLIC Drive Beam CLIC workshop,
Coherent THz radiation source driven by pre-bunched electron beam
Development of High Brightness Electron Photoinjectors at ASTeC B.L. Militsyn Accelerator Science and Technology Centre Science & Technology Facility Council,
1 NGLS Outline and Needs in Superconducting RF Materials Development John Corlett SRFMW, July 16, 2012 Office of Science.
Solid State Lasers and Applications Proposed for Brookhaven’s ATF-II
Status of the SPARC laser and “dazzler” experiments
Linac beam dynamics Linac dynamics : C. Bruni, S. Chancé, L. Garolfi,
PHIL: A TEST BEAMLINE AT LAL Specifications of PHIL
Abstract EuSPARC and EuPRAXIA projects
Sara Thorin, MAX IV Laboratory
Timing and synchronization at SPARC
Tunable Electron Bunch Train Generation at Tsinghua University
Gu Qiang For the project team
Paul Scherrer Institut
Injection facility for Novosibirsk Super Charm Tau Factory
SuperB project. Injection scheme design status
MIT Compact X-ray Source
F. Villa Laboratori Nazionali di Frascati - LNF On behalf of Sparc_lab
SLAC ARD Test Facilities
Advanced Research Electron Accelerator Laboratory
Brief Introduction to (VUV/)Soft X-ray FELs
Compact linear accelerator FLUTE: status update
LCLS FEL Parameters Heinz-Dieter Nuhn, SLAC / SSRL April 23, 2002
Proposal for Smith-Purcell radiation experiment at SPARC_LAB
Presentation transcript:

THE CSU ADVANCED BEAM LABORATORY (ABL) Sandra Biedron 1

ABL: Two Primary Focus Area Accelerator Science and Technology Leads: Sandra Biedron and Stephen Milton Lasers Jorge Rocca, Menoni, Mario Marconi Main Concept Merge Accelerator Technologies with Laser Technologies to create new technologies with performance capabilities not possible with only one. 2

The Advanced Beam Laboratory CSU Board of Governors approved construction and expenditure of the money needed to build of the new building. CSU President has chosen to move forward with the construction and has developed a funding plan. 3

ABL Timeline Accelerated Delivery Made possible by an existing construction contract to build what is called Engineering II. We are using the same Architect and General Contractor Timeline (Abbreviated) 12 November 2012 – Fence off construction yard 19 November 2012 – Begin site preparation work February 2013 – Walls go up 31 July 2013 – Building ready for move in 4

ABL: Current Status Footings and Slab Complete 5 Iron work going up

ABL Basic Layout and Initial Capabilities 6 Laser Lab 1 Laser Lab 2 Accelerator Lab Drive Laser Laboratory Accelerator Control Room Terawatt Ti:Sapphire laser system. Wavelength: 0.8 micrometers, Energy before compression: 13 Joules. Repetition rate: up to 5 Hz. Plans to scale to 0.5 Petawatt 1 J, 5 picosecond, 100 Hz repetition rate diode-pumped laser (100 W average power) Wavelength: 1.03 micrometers. Highest repetition rate diode-pumped chirped-pulse- amplification laser in the world. Can be scaled in repetition rate and pulse energy, future parameters depend on funding. 6 MeV Photocathode Driven Electron Linac L- Band (1.3 GHz) Two Klystrons Available (One needed for PC Gun) 15 us pulse durations at 10 Hz Up to MHz pulse rates available

High energy femtosecond Ti:Sapphire laser (> 100 TW, up to 5 Hz repetition rate) Profs. Jorge Rocca, Carmen Menoni

Energy Pre-compression= 13 J Std div. = 1.5 % High repetition rate Titanium-Sapphire laser

Unique high power diode-pumped solid state lasers pump table-top soft x-ray lasers at 100 Hz repetition rate Laser Diode Drivers Soft X-Ray Plasma Amplifier Solid State Ultrashort Pulse High Power Laser Ag nm laser e B. Reagan et al., Optics Letters, 37, 3624, ( 2012)

Compact high power diode-pumped CPA laser generates 1 J, 5 ps, pulses at 100 Hz repetition rate B. Reagan et al., Optics Letters, 37, 3624, ( 2012) 1 J, 5 ps, 100 Hz

Laser Pumped SXRL λ= 8.8– 32.6 nm Discharge Pumped SXRL λ=46.9 nm 100 nm lines 82 nm holes Chemical spectroscopies Microscopy Nanomachining Interferometry Compact plasma-based soft x-ray lasers for application (J.J. Rocca, C.S Menoni. M. Marconi) Plasma diagnostics 58 nm pillars Nanopatterning High pulse energy (µJ-mJ) High monochromaticity (λ/Δλ < ) High peak spectral brightness

Gain-saturated table-top SXRLs cover 8.8 nm - 47 nm wavelength region Pr Saturated Seeded  D. Alessi et al. Phys. Rev X, 1, , (2011)

CSU Accelerator Laboratory 13 Donated by the Univ. of Twente Donated by the Boeing Corp.

Linac Performance Parameters 14 Linac Characteristics Energy6 MeV Number of Cells5 ½ RF Frequency1.3 GHz Shunt Impedance 50 M  /m Q-Value18,000 Axial Electric Field Cell no. 126 MV/m Cell No MV/m Cell No. 3 – MV/m Solenoid Field Strength1,200 G

System Performance Parameters 15 Major System Parameters Linac Frequency1.3 GHz Repetition Rate10 Hz Mircopulse Rep. Rate81.25 MHz (max.) Klystron TypeTH 2022C (Thales) Power20 MW Modulator TypePFN Pulse Duration 15  sec Undulator TypeHybrid: NdFeB K1 (at 8 mm gap) Period25 mm Periods50

Cathode Preparation Chamber A Variety of Cathodes Can be Used Cathode preparation chamber Used in the past CeK 2 Sb, K 3 Sb, and Copper The choice is dependent on what the experiment demanded A Variety of Cathodes Can be Used Cathode preparation chamber Used in the past CeK 2 Sb, K 3 Sb, and Copper The choice is dependent on what the experiment demanded 16

ABL Initial Capabilities/Explorations Laser Laboratories: Initial and Historical Functions Soft x-ray lasers (driven by the optical lasers in previous slide) Wavelength range: 8.8 nm to 47 nm. Picosecond pulse duration. Pulse energy = 2-10 microjoule. Average power: up to 0.15 mW (world highest average power table top soft x-ray lasers) Side Note: These soft x-ray lasers are made possible by the generation of very uniform, high density plasmas. Ancillary Capabilities of Group Laser design and fabrication High power optics development and production Nano patterning 17

ABL Initial Capabilities/Explorations Accelerator Laboratories: Initial and Historical Functions Compact, High-power THz FEL Tunable between microns About 1 MW peak power from 900 MW available peak beam power (6 MeV, 150 A peak current) Average: a few mW (81.25 MHz rep rate, 15 microsecond macropulse,25-ps micropulse) Specialized beam diagnostics Electro Optical Sampling System System intended for tests at JLab FEL If JLab not ready then we will test it at CSU Laser/Plasma/e- Beam Interaction Studies Continuation of an experiment started at University of Twente 18

A Smattering of Current Projects Soft X-ray compact laser development High-Power THz FEL Neural Network Control of Accelerators X-band Technologies High Power Optics Development Nanopatterning High Density Plasma Theory, Simulation, and Production Electro-Optical Sampling Diagnostic for High-Power Beams Photocathode studies Laser/Plasma/e- Beam interactions Compact source design and development Study of LSC/CSR and the Microbunching Instability Medical Applications of Accelerator System Two-Beam Systems FEL Harmonic Control 19 Blue indicates areas potentially relevant to HEP programs

Other Intriguing Areas We Are Beginning to Pursue Capillary Discharge 20 Electron Density Profile Near Field Far Field The potential to use this technology for high-gradients is tremendous and CSU IS the world leader in this.

Summary The CSU Advanced Beam Laboratory The Coupling of Accelerator Expertise and Existing Accelerator System 6 MeV photocathode linac system with state-of-the-art drive laser Laser/Plasma Expertise and Existing Laser, Plasma and Ancillary Systems/Areas Unique state-of-the-art laser systems Plasma Sources EUV/Soft x-ray Microscopy/Spectroscopy expertise Multilayer Optics expertise Will be used for Basic beam (Laser, particle and combined beam) research and development Purpose-Built Building Ready for move in 31 July