Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | www.hzdr.de The HZDR Program towards a Helmholtz beamline at XFEL Roland Sauerbrey Helmholtz-Zentrum.

Slides:



Advertisements
Similar presentations
B. Kämpfer | Institut für Strahlenphysik | Hadronenphysik | Helmholtz-Zentrum Dresden-Rossendorf B. Kämpfer PW Laser Workshop, HZDR 2011 Strong-Field.
Advertisements

Vulcan Front End OPCPA System
Central Laser Facility
Petawatt Field Synthesizer
New hardware and setups New short pulse regime Experimental results TW power Future plans on laser development ATF CO 2 LASER progress Vitaly Yakimenko.
Collinear interaction of photons with orbital angular momentum Apurv Chaitanya N Photonics science Laboratory, PRL.
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.
R.6.2 Lasery Optoelektronika 2014 Dr hab. inż. B. B. Kosmowski 1.
Observation of the relativistic cross-phase modulation in a high intensity laser plasma interaction Shouyuan Chen, Matt Rever, Ping Zhang, Wolfgang Theobald,
Soft X-ray light sources Light Sources Ulrike Frühling Bad Honnef 2014.
Intense Terahertz Generation and Spectroscopy of Warm Dense Plasmas Kiyong Kim University of Maryland, College Park.
Lasers and Highly-Charged Heavy Ions at Günther RosnerHZDR Workshop, Rossendorf, 6/9/111.
Positronium Rydberg excitation in AEGIS Physics with many positrons International Fermi School July 2009 – Varenna, Italy The experimental work on.
The Intensity-Pulse Duration Conjecture: ELI’s Lynchpin ELI-NP: The Way Ahead Bucharest March 10, 2011 Gérard Mourou, Institut de Lumière Extrême 28/02/11mourou.
Scottish Universities Physics Alliance Progress and Plans of the SUPA Nuclear & Plasma Physics Theme Dino Jaroszynski Edinburgh, Glasgow, HWU, Strathclyde,
Janez Žabkar Advisers: dr. Marko Zgonik dr. Marko Marinček
2. High-order harmonic generation in gases Attosecond pulse generation 1. Introduction to nonlinear optics.
Pump Probe Measurements of Femto-second Pulses By David Baxter.
Diagnostics for Benchmarking Experiments L. Van Woerkom The Ohio State University University of California, San Diego Center for Energy Research 3rd MEETING.
OSU/UCSD/GA Experimental Program J. Pasley, E. Shipton, T. Ma, B. Bucher, S. Chen, F. Beg University of California at San Diego E. Chowdhury, L. Van Woerkom,
KeV Harmonics from Solid Targets - The Relatvisitic Limit and Attosecond pulses Matt Zepf Queens University Belfast B.Dromey et al. Queen’s 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.
Random phase noise effect on the contrast of an ultra-high intensity laser Y.Mashiba 1, 2, H.Sasao 3, H.Kiriyama 1, M.R.Asakawa 2, K.Kondo 1, and P. R.
TOF Mass Spectrometer &
High Harmonic Generation in Gases Muhammed Sayrac Texas A&M University.
Palaiseau - FRANCE Spatio-Temporal Chirped Pulse Amplification for Avoiding Spectral Modifications in Ultra-Short Petawatt Lasers C. Radier1,2, F. Giambruno1,3,
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
John Collier Science with High Power Lasers. Godfrey Stafford Celebration The Central Laser Facility Prof John Collier Director.
CLEO2004 K. L. Ishikawa No. 0 Enhancement in photoemission from He + by simultaneous irradiation of laser and soft x-ray pulses Kenichi L. Ishikawa Department.
High purity x-ray polarimetry Ingo Uschmann B. Marx, K. Schulze, S. Hoefer, R. Loetzsch, T. Kämpfer, O. Wehrhan, H. Marschner, E. Förster, M. Kaluza, H.
Photon Diagnostic Station For TAC IR-FEL Test Facility ILHAN TAPAN* *on behalf of the TAC collaboration Uludag Universitesi, Bursa,16059, TURKEY References.
Alvaro Sanchez Gonzalez Prof. Jon Marangos Prof. Jim Clarke
Cryogenic Gas Cooling of High Energy Lasers Paul Mason HEPTech – Cryogenics Meeting, Grenoble, France 4-5 th June 2015 STFC Rutherford.
Observation of ultrafast nonlinear response due to coherent coupling between light and confined excitons in a ZnO crystalline film Ashida Lab. Subaru Saeki.
About the possibility to build a 10-PW femtosecond laser for ELI-NP till 2015 Razvan Dabu National Institute for Lasers, Plasma and Radiation Physics Bucharest.
Classical and quantum electrodynamics e®ects in intense laser pulses Antonino Di Piazza Workshop on Petawatt Lasers at Hard X-Ray Sources Dresden, September.
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.
ESFRI & e-Infrastructure Collaborations, EGEE’09 Krzysztof Wrona September 21 st, 2009 European XFEL.
1 Warsaw, National Centre for Nuclear Research Nuclear research in Poland Reactor.
K. Z. Hatsagortsyan, G. Yu. Kryuchkyan*, A. Ipp, J. Evers and C. H. Keitel Max-Planck-Institut für Kernphysik, Heidelberg, Germany *Yerevan State University,
Max Cornacchia, SLAC LCLS Project Overview BESAC, Feb , 2001 LCLS Project Overview What is the LCLS ? Transition from 3 rd generation light sources.
Octoberfest! October 2014 Peter Tudor John Adams Institute for Accelerator Science Laser Wakefield Acceleration.
M. Hosaka a, M. Katoh b, C. Szwaj c, H. Zen b M. Adachi b, S. Bielawski c, C. Evain c M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto.
Extreme Light Infrastructure in Romania: progress Daniel URSESCU Technical contact point for ELI in Romania INFLPR, Magurele, Romania.
Hartmut Buettig | Institut FWKE(ELBE) | First Experience at ELBE with the new 1.3 GHz CW RF-System based on 10 kW Solid State Amplifiers Hartmut.
The Next Generation Light Source Test Facility at Daresbury Jim Clarke ASTeC, STFC Daresbury Laboratory Ultra Bright Electron Sources Workshop, Daresbury,
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.
Testing Quantum Electrodynamics at critical background electromagnetic fields Antonino Di Piazza International Conference on Science and Technology for.
International Conference on Science and Technology for FAIR in Europe 2014 APPA Cave Instrumentation for Plasma Physics Vincent Bagnoud, GSI and Helmholtz.
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Schematic of the noncollinear optical parametric amplification (NOPA) geometry.
Fastest Data Processing in Image Reconstruction for Compton Camera Imaging
Polarization Dependence in X-ray Spectroscopy and Scattering
ESS Innovation Procurement Workshop
Brief Introduction to ELBE
V. Bagnoud PHELIX, Plasma Physics department GSI Darmstadt
The scientific pillars of ELI
Biology at Advanced Laser Light Sources
Science parks and technological support at ELI Beamlines
Wakefield Accelerator
The contribution of the Wigner Research Center to the
Free Electron Lasers (FEL’s)
L. Obst, S. Göde, M. Rehwald, F. -E. Brack, J. Branco, S. Bock, M
Peking University: Jinqing Yu, Ronghao Hu, Haiyang Lu & Xueqing Yan
X-Ray Spectrometry Using Cauchois Geometry For Temperature Diagnostics
Emittance Partitioning between x (or y) and z dimensions
Short focal length target area: X-ray & ion sources and applications
Kansas Light Source Laser System J. R. Macdonald Laboratory
Complex Nanophotonics
Status of ELI Beamlines
Presentation transcript:

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | The HZDR Program towards a Helmholtz beamline at XFEL Roland Sauerbrey Helmholtz-Zentrum Dresden-Rossendorf

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director |  Member of the Helmholtz Association  Foundation (e.V.)  Employeesca. 800 including ca. 260 scientists doctoral students as well as employees and guest scientists from more than 40 countries  BudgetPublic funding (2011)ca. 84 Mio. € Saxon investment program ca. 70 Mio. € ( ) Third-party funding and other sourcesca. 20 Mio. € HZDR – Facts and Figures

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | Ion Beam Center Radiation Source ELBE Free-Electron-Lasers High-Intensity Laser Rossendorf Beamline ROBL at the ESRF TOPFLOW Facility High Magnetic Field Laboratory Dresden PET Center Advanced Materials Research How does matter behave in strong fields and at small dimensions? Nuclear Safety Research How can the public and the environment be protected from technical risks? Cancer Research How can cancerous tumors be identified in the early stages and treated effectively? Research Questions and Large-Scale Facilities

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | Concept: Unique combination of: high-power high-brilliance CW electron beams, synchronized with high rep-rate, ultra-high intensity lasers. Development of: new radiation sources, in unique combinations, enabling study of matter under extreme conditions & in new regimes. Will constitute a prototype for future facilities: National Center for Radiation Research in Oncology-Dresden, and Helmholtz beamline at XFEL, or FAIR. Center for high power radiation HZDR

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | ELBE Upgrades High Intensity Lasers Zentrum HSQ Center for high power radiation HZDR

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | Center for high power radiation sources

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | PW area Petawatt, Energy-Efficient Laser for Optical Plasma Experiments Development of a 2nd generation directly diode laser pumped short pulse PW laser (design: 150J in 150fs, >1Hz rep. Rate, active medium Yb:CaF2 discs ) based on the 1st generation project POLARIS at IOQ Jena Complemented by running 150TW Ti:Sapphire laser Draco (upgrade to PW level in progress)

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | 2 × 2 × 2 m 3 4 × 2 × 0.1 m³ (table top) (a) pump setup 4-pass pumping reduces reabsorption losses by 75% (c) laser material cooling Rod designSlab designActive Mirrors Repetition rate 1/min Repetition rate 1-10Hz (b) laser material Brightness: ~100kW/cm 2 /sr Wavelength: 940 nm Brightness: >1MW/cm 2 /sr Wavelength: 980 nm Yb:FP glass Yb:CaF 2 From POLARIS (IOQ Jena) to PEnELOPE (HZDR)

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | Nonlinear QED

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | QED regime: small photon energy (compared to m e c 2 ) highest intensity (yet low compared to I c =4·10 29 W/cm 2 ) dispersive effect (vacuum polarization) calculated in lowest non-trivial order O(I) and O(ω 2 probe ) -> birefringence phase shift Laser-induced vacuum birefringence

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | phase shift Resulting ellipticity measurable ellipticity (intensity measurement) brilliant X-ray probehigh intensity and interaction length TH. Heinzl, et al. Opt. Commun. 267, 318 (2006)

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | Proposed experimental realization highest intensity see talk by I. Uschmann

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director | High contrast x-ray analyzers (Hart 1991, Hasegawa 1999, Alp 2000): Multiple Bragg reflections from perfect crystals Contrast in the multi-keV range from 10 6 (measured) to possibly (calculated) Requiring perfect X-ray beam quality (in polarization and geometry) Detector (analyzer) technology

Prof. Dr. Dr. h. c. R. Sauerbrey | Scientific Director |