TTF FEL Results Jacek Krzywinski TTF FEL Performance FEL Physics Experiments FELIS (Free Electron Laser - Interaction with Solids Cluster Experiment

Size: px
Start display at page:

Download "TTF FEL Results Jacek Krzywinski TTF FEL Performance FEL Physics Experiments FELIS (Free Electron Laser - Interaction with Solids Cluster Experiment"

Transcription

1 TTF FEL Results Jacek Krzywinski TTF FEL Performance FEL Physics Experiments FELIS (Free Electron Laser - Interaction with Solids Cluster Experiment

2 TTF FEL Performance Photon Beam Diagnostic Team Scientists: Josef Feldhaus Christofer Gerth Ulrich Hahn Rasmus Ischebeck Barbara Steeg Kai Tiedke Rolf Treush Engineers and Technicians: Lutz Bittner Thorsten Hans Mathias Hesse Fini Jastrow Michael Meschkat Ernst Weiner

3 Demonstration of: Saturation: from nm Tranverse coherence > 90% Diffraction patterns from double and crossed slits Variation of pulse length: fs variation via bunch compressor 1 Second harmonics spectra: wavelength 48.5 nm

4

5

6

7

8 FELIS (Free Electron Laser-Interaction with Solids) J. Krzywinski 1,2, A. Andrejczuk 1,3, U. Hahn 2, M. Kirm 4, A. Kauch 5, M. Jurek 1,2, J.B. Pelka 1, H. Reniewicz 3,W. Sobala 6, M. Sikora 7, R. Sobierajski 2,8 1 Institute of Physics, Polish Academy of Sciences, 2 HASYLAB at DESY, Germany, 3 University of Bialystok, Poland, 4 Institut Für Eksperimentalphysik der Hamburg Universität 5 Warsaw University,Poland 6 Institute of Nuclear Physics, Cracow,Poland 7 University of Mining and Metallurgy 8 Warsaw University of Technology, Cracow, Poland

9 Experimental layout VUV laser beam TOF VUV Detectors Light source CCD Camera X,Y,Z,ϕ sample manipulator Photocurrent A Evaporation cell

10 Experimental layout

11 VUV beam parameters Pulse length fs Pulse energy 1-30 uj Wavelength nm Minimum spot size 10 µm

12 Experimental results Example of ablation detected by TOF spectrometer (Si sample) H Si TOF signal [V] 0 O Time [µs]

13 Experimental results Si + ion emission threshold Normalized inte gral of MCP signal [a.u.] Beam intensity [a.u.]

14 Si =2.5mm Number of pulses max = 2.5uJ mean = 1.2uJ Npulses = Pulse energy [uj]

15 Number of pulses max = 5.1uJ mean = 1.3uJ Npulses = Pulse energy [uj] Si =1mm

16 Number of pulses max = 3.4uJ mean = 1uJ Npulses = Pulse energy [uj] =0mm Si

17 Si

18 Cluster emission from graphite surface 3C + 4C + Graphite hv = 10.1 ev fluence ~0.1 J/cm^2 5C + 7C + C + 6C + 8C + 9C + 10C + 11C + 12C + 14C + 15C +

19 Cluster emission from MgF 2 surface

20 Surface modification AFM results V. Kuestner, S. Jacobi, GKSS

21

22 C-film (10nm) / Si-substrate

23 C-film (10nm) / Si-substrate

24 C-film (10nm) / Si-substrate

25 C-film (40-nm) / Si-substrate

26 Plasma creation multiple ionisation maximum kinetic energy > 10 kev (C 5+ ) non thermal ion energy distribution

27 Number of pulses max = 5.4uJ mean = 1.6uJ Npulses = Pulse energy [uj] =0mm

28 FELIS Jan. 2002

29 plasma results Au bulk scan _/t0 /set mass/charge scale /versus/ Integ. of I0mcp-sc[V*s][] scan _/t0 /set mass/charge scale /versus/ Max of I0 peak[v][] 0.1 TOF -scan _026.dat /cond._2/t TOF -scan _037.dat /cond._2/t Voltage [V] HPF=100 V Au 3+ Au Au Au Voltage [V] HPF=200V Au 3+ Au Mass/charge [amu/e] Mass/charge [amu/e] scan _/t0 /set mass/charge scale /versus/ Max of I0 peak[v][] scan _/t0 /set mass/charge scale /versus/ Max of I0 peak[v][] TOF -scan _037.dat /cond._2/t0 TOF -scan _023.dat /cond._2/t Au 2+ HPF=200V 0.03 Au 3+ Au + Au 2+ Au Au 3+ HPF=800V 0.04 Voltage [V] Voltage [V] Mass/charge [amu/e] Mass/charge [amu/e]

30 First Results from the Clusterexperiment at the TTF-FEL Motivation Experimental Set-Up Multi-Photon Ionisation Coulomb Explosion of Clusters

31 Peter Gürtler Wiebke Laasch Tim Laarmann Joachim Schulz Anja Swiderski Klaus von Haeften Hubertus Wabnitz Thomas Möller

32 Idea of the experiment interaction of intense soft x-rays with matter which multi-photon processes are observed cross sections (surface, bulk) which ions are prepared (charge state, electronically excited states) life time of intermediate states high-order harmonic generation

33

34

35 0,4 single shot Xe ++ Xe + Xe 3+ intensity [arb. units] 0, average size of clusters N= , time of flight [ns]

36 atomic beam 0,3 intensity [arb. units] 0,2 0,1 Xe + 0, time of flight [ns]

37 ejection energy Xe + 0,3 intensity [arb. units] 0,2 0,1 4+ Xe ++ average size of clusters N=20 Xe 3+ Xe 2 + 0, time of flight [ns]

38 cluster beam 0,3 Xe ++ Xe + intensity [arb. units] 0,2 0, Xe 3+ average size of clusters N=2000 0, time of flight [ns]

39 N~30000 Dependence on the cluster size N~80 Single photon absorption in Xe atoms 0.2 intensity [arb. units] N~2-20 Xe Xe ++ emission of highly charge ions from clusters ( up to eight times charges) ions have high kinetic energy atom Xe time of flight [ns]

40 Kinetic energy of the ejected ions xenon clusters N=2000 Quadratic dependence on charge ejection energy [ev] Coulomb explosion ion charge state

41 Dependence on the power density Xenon clusters, 50 atoms Watt/cm 2 5*10 11 Watt/cm

42 Conclusions: all features of FEL SASE radiation has been demonstrated in the nm range : saturation, tunability, coherence, higher harmonics (in addition pulse length control in the fs range) two user experiments has been successfully carried out providing unique data of intense soft X-ray - matter interaction in the new domain of parameters results of the experiments are essential for planning future experiments at soft X-ray FELs

PB I FEL Gas-Monitor Detectors for FEL Online Photon Beam Diagnostics BESSY

PB I FEL Gas-Monitor Detectors for FEL Online Photon Beam Diagnostics BESSY FEL 2004 Gas-Monitor Detectors for FEL Online Photon Beam Diagnostics M. Richter S.V. Bobashev, J. Feldhaus A. Gottwald, U. Hahn A.A. Sorokin, K. Tiedtke BESSY PTB s Radiometry Laboratory at BESSY II 1

More information

CONCEPTUAL STUDY OF A SELF-SEEDING SCHEME AT FLASH2

CONCEPTUAL STUDY OF A SELF-SEEDING SCHEME AT FLASH2 CONCEPTUAL STUDY OF A SELF-SEEDING SCHEME AT FLASH2 T. Plath, L. L. Lazzarino, Universität Hamburg, Hamburg, Germany K. E. Hacker, T.U. Dortmund, Dortmund, Germany Abstract We present a conceptual study

More information

The MID instrument.

The MID instrument. The MID instrument International Workshop on the Materials Imaging and Dynamics Instrument at the European XFEL Grenoble, Oct 28/29, 2009 Thomas Tschentscher thomas.tschentscher@xfel.eu Outline 2 History

More information

Ultrafast X-Ray-Matter Interaction and Damage of Inorganic Solids October 10, 2008

Ultrafast X-Ray-Matter Interaction and Damage of Inorganic Solids October 10, 2008 Ultrafast X-Ray-Matter Interaction and Damage of Inorganic Solids October 10, 2008 Richard London rlondon@llnl.gov Workshop on Interaction of Free Electron Laser Radiation with Matter Hamburg This work

More information

Clusters in intense x-ray pulses from 100 nm to.7 nm

Clusters in intense x-ray pulses from 100 nm to.7 nm Clusters in intense x-ray pulses from 100 nm to.7 nm Linac Coherent Light Source, SLAC National Accelerator Laboratory Outline: Introduction and motivation Spectroscopy of clusters Single shot imaging

More information

FLASH/DESY, Hamburg. Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team -

FLASH/DESY, Hamburg. Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team - First Lasing below 7nm Wavelength at FLASH/DESY, Hamburg Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team - email: joerg.rossbach@desy.de FLASH: The first FEL user facility for

More information

FLASH overview. Nikola Stojanovic. PIDID collaboration meeting, Hamburg,

FLASH overview. Nikola Stojanovic. PIDID collaboration meeting, Hamburg, FLASH overview Nikola Stojanovic PIDID collaboration meeting, Hamburg, 16.12.2011 Outline Overview of the FLASH facility Examples of research at FLASH Nikola Stojanovic PIDID: FLASH overview Hamburg, December

More information

Femtosecond time-delay holography Henry Chapman Centre for Free-Electron Laser Science - DESY Lawrence Livermore National Laboratory

Femtosecond time-delay holography Henry Chapman Centre for Free-Electron Laser Science - DESY Lawrence Livermore National Laboratory Femtosecond time-delay holography Henry Chapman Centre for Free-Electron Laser Science - DESY Lawrence Livermore National Laboratory Henry.Chapman@desy.de Isaac Newton Opticks 1704 Newton was the first

More information

Damage to optics under irradiations with the intense EUV FEL pulses

Damage to optics under irradiations with the intense EUV FEL pulses Damage to optics under irradiations with the intense EUV FEL pulses Ryszard Sobierajski 1, Eric Louis 2 1 Institute of Physics PAS, 2 Universiteit Twente Damage to optics - motivation Properties of the

More information

Damage to Molecular Solids Irradiated by X-ray Laser Beam

Damage to Molecular Solids Irradiated by X-ray Laser Beam WDS'11 Proceedings of Contributed Papers, Part II, 247 251, 2011. ISBN 978-80-7378-185-9 MATFYZPRESS Damage to Molecular Solids Irradiated by X-ray Laser Beam T. Burian, V. Hájková, J. Chalupský, L. Juha,

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION doi:10.1038/nature10721 Experimental Methods The experiment was performed at the AMO scientific instrument 31 at the LCLS XFEL at the SLAC National Accelerator Laboratory. The nominal electron bunch charge

More information

Layout of the HHG seeding experiment at FLASH

Layout of the HHG seeding experiment at FLASH Layout of the HHG seeding experiment at FLASH V. Miltchev on behalf of the sflash team: A. Azima, J. Bödewadt, H. Delsim-Hashemi, M. Drescher, S. Düsterer, J. Feldhaus, R. Ischebeck, S. Khan, T. Laarmann

More information

Jitter measurement by electro-optical sampling

Jitter measurement by electro-optical sampling Jitter measurement by electro-optical sampling VUV-FEL at DESY - Armin Azima S. Duesterer, J. Feldhaus, H. Schlarb, H. Redlin, B. Steffen, DESY Hamburg K. Sengstock, Uni Hamburg Adrian Cavalieri, David

More information

LOLA: Past, present and future operation

LOLA: Past, present and future operation LOLA: Past, present and future operation FLASH Seminar 1/2/29 Christopher Gerth, DESY 8/5/29 FLASH Seminar Christopher Gerth 1 Outline Past Present Future 8/5/29 FLASH Seminar Christopher Gerth 2 Past

More information

The BESSY - FEL Collaboration

The BESSY - FEL Collaboration The BESSY - FEL Collaboration Planning the Revolution for Research with soft X-Rays Photon Energy Range : 20 ev up to 1 kev λ/λ 10-2 to 10-4 Peak Power: 1mJ in 200 fs >> 5 GW Time Structure: 200 fs (

More information

XFEL project overview

XFEL project overview EUROPEAN STRATEGY FORUM on RESEARCH INFRASTRUCTURES ESFRI workshop on Technical Challenges at the Proposed European XFEL Laboratory 30-31 October 2003 XFEL project overview Jochen R. Schneider (DESY) Scientific

More information

Linac Based Photon Sources: XFELS. Coherence Properties. J. B. Hastings. Stanford Linear Accelerator Center

Linac Based Photon Sources: XFELS. Coherence Properties. J. B. Hastings. Stanford Linear Accelerator Center Linac Based Photon Sources: XFELS Coherence Properties J. B. Hastings Stanford Linear Accelerator Center Coherent Synchrotron Radiation Coherent Synchrotron Radiation coherent power N 6 10 9 incoherent

More information

Expected properties of the radiation from VUV-FEL / femtosecond mode of operation / E.L. Saldin, E.A. Schneidmiller, M.V. Yurkov

Expected properties of the radiation from VUV-FEL / femtosecond mode of operation / E.L. Saldin, E.A. Schneidmiller, M.V. Yurkov Expected properties of the radiation from VUV-FEL / femtosecond mode of operation / E.L. Saldin, E.A. Schneidmiller, M.V. Yurkov TESLA Collaboration Meeting, September 6-8, 2004 Experience from TTF FEL,

More information

Laser heating of noble gas droplet sprays: EUV source efficiency considerations

Laser heating of noble gas droplet sprays: EUV source efficiency considerations Laser heating of noble gas droplet sprays: EUV source efficiency considerations S.J. McNaught, J. Fan, E. Parra and H.M. Milchberg Institute for Physical Science and Technology University of Maryland College

More information

AMO physics with LCLS

AMO physics with LCLS AMO physics with LCLS Phil Bucksbaum Director, Stanford PULSE Center SLAC Strong fields for x-rays LCLS experimental program Experimental capabilities End-station layout PULSE Ultrafast X-ray Summer June

More information

Short Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team

Short Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team Short Pulse, Low charge Operation of the LCLS Josef Frisch for the LCLS Commissioning Team 1 Normal LCLS Parameters First Lasing in April 10, 2009 Beam to AMO experiment August 18 2009. Expect first user

More information

Proton acceleration in thin foils with micro-structured surface

Proton acceleration in thin foils with micro-structured surface Proton acceleration in thin foils with micro-structured surface J. Pšikal*, O. Klimo*, J. Limpouch*, J. Proška, F. Novotný, J. Vyskočil Czech Technical University in Prague, Faculty of Nuclear Sciences

More information

The Free Electron Laser: Properties and Prospects 1

The Free Electron Laser: Properties and Prospects 1 The Free Electron Laser: Properties and Prospects 1 Gunnar Ingelman and Kai Siegbahn Uppsala University Abstract: Novel electron accelerator techniques can be used to create free electron lasers in a wide

More information

4 FEL Physics. Technical Synopsis

4 FEL Physics. Technical Synopsis 4 FEL Physics Technical Synopsis This chapter presents an introduction to the Free Electron Laser (FEL) physics and the general requirements on the electron beam parameters in order to support FEL lasing

More information

Laser matter interaction

Laser matter interaction Laser matter interaction PH413 Lasers & Photonics Lecture 26 Why study laser matter interaction? Fundamental physics Chemical analysis Material processing Biomedical applications Deposition of novel structures

More information

Photoelectron Spectroscopy using High Order Harmonic Generation

Photoelectron Spectroscopy using High Order Harmonic Generation Photoelectron Spectroscopy using High Order Harmonic Generation Alana Ogata Yamanouchi Lab, University of Tokyo ABSTRACT The analysis of photochemical processes has been previously limited by the short

More information

SASE FEL PULSE DURATION ANALYSIS FROM SPECTRAL CORRELATION FUNCTION

SASE FEL PULSE DURATION ANALYSIS FROM SPECTRAL CORRELATION FUNCTION SASE FEL PULSE DURATION ANALYSIS FROM SPECTRAL CORRELATION FUNCTION Shanghai, 4. August. Alberto Lutman Jacek Krzywinski, Yuantao Ding, Yiping Feng, Juhao Wu, Zhirong Huang, Marc Messerschmidt X-ray pulse

More information

Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR)

Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR) Case Study of IR/THz source for Pump-Probe Experiment at the European XFEL Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR) Introduction Outline Simulations of High-gain FEL (SASE) Simulation

More information

Excitements and Challenges for Future Light Sources Based on X-Ray FELs

Excitements and Challenges for Future Light Sources Based on X-Ray FELs Excitements and Challenges for Future Light Sources Based on X-Ray FELs 26th ADVANCED ICFA BEAM DYNAMICS WORKSHOP ON NANOMETRE-SIZE COLLIDING BEAMS Kwang-Je Kim Argonne National Laboratory and The University

More information

Upgrade of the FLASH beamlines New diagnostic and beam transport tools

Upgrade of the FLASH beamlines New diagnostic and beam transport tools Upgrade of the FLASH beamlines New diagnostic and beam transport tools Kai Tiedtke FLASH Seminar 16.3.2010 Installation in the tunnel and experimental hall -Install a focusing mirror at BL3 Experimental

More information

Lecture 1 August 29

Lecture 1 August 29 HASYLAB - Facility - Free Electron Laser (FEL) http://www-hasylab.desy.de/facility/fel/main.htm Page 1 of 1 8/23/2006 HASYLAB Facility Free Electron Laser Overview FLASH FLASH User Info Events Job Offers

More information

Gas Based Detectors for FEL Photon Diagnostics.

Gas Based Detectors for FEL Photon Diagnostics. Gas Based Detectors for FEL Photon Diagnostics. Kai Tiedtke Satellite Workshop on Photon Beam Diagnostics, 29 Jan. 2015 Outline. Intensity and Beam Position Monitor (GMD) @ FLASH Gas-Monitor-Detector for

More information

Inelastic soft x-ray scattering, fluorescence and elastic radiation

Inelastic soft x-ray scattering, fluorescence and elastic radiation Inelastic soft x-ray scattering, fluorescence and elastic radiation What happens to the emission (or fluorescence) when the energy of the exciting photons changes? The emission spectra (can) change. One

More information

Optimization of laser-produced plasma light sources for EUV lithography

Optimization of laser-produced plasma light sources for EUV lithography page 1 of 17 Optimization of laser-produced plasma light sources for EUV lithography M. S. Tillack and Y. Tao 1 University of California, San Diego Center for Energy Research 1 Currently at Cymer Inc.

More information

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source 3rd International EUVL Symposium NOVEMBER 1-4, 2004 Miyazaki, Japan Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source H. Tanaka, A. Matsumoto, K. Akinaga, A. Takahashi

More information

The European XFEL in Hamburg: Status and beamlines design

The European XFEL in Hamburg: Status and beamlines design UVX 2010 (2011) 63 67 DOI: 10.1051/uvx/2011009 C Owned by the authors, published by EDP Sciences, 2011 The European XFEL in Hamburg: Status and beamlines design J. Gaudin, H. Sinn and Th. Tschentscher

More information

Excitements and Challenges for Future Light Sources Based on X-Ray FELs

Excitements and Challenges for Future Light Sources Based on X-Ray FELs Excitements and Challenges for Future Light Sources Based on X-Ray FELs 26th ADVANCED ICFA BEAM DYNAMICS WORKSHOP ON NANOMETRE-SIZE COLLIDING BEAMS Kwang-Je Kim Argonne National Laboratory and The University

More information

X-Rays From Laser Plasmas

X-Rays From Laser Plasmas X-Rays From Laser Plasmas Generation and Applications I. C. E. TURCU CLRC Rutherford Appleton Laboratory, UK and J. B. DANCE JOHN WILEY & SONS Chichester New York Weinheim Brisbane Singapore Toronto Contents

More information

Appendix A Detector Calibration

Appendix A Detector Calibration Appix A Detector Calibration The scattering pattern from single clusters analyzed in Sect. 3.5 have been obtained with a large area detector which allows for spatially resolved measurement of the scattered

More information

X-ray Free-electron Lasers

X-ray Free-electron Lasers X-ray Free-electron Lasers Ultra-fast Dynamic Imaging of Matter II Ischia, Italy, 4/30-5/3/ 2009 Claudio Pellegrini UCLA Department of Physics and Astronomy Outline 1. Present status of X-ray free-electron

More information

Developments for the FEL user facility

Developments for the FEL user facility Developments for the FEL user facility J. Feldhaus HASYLAB at DESY, Hamburg, Germany Design and construction has started for the FEL user facility including the radiation transport to the experimental

More information

Theoretical approach to estimate radiation damage within FEL irradiated samples. Beata Ziaja

Theoretical approach to estimate radiation damage within FEL irradiated samples. Beata Ziaja Theoretical approach to estimate radiation damage within FEL irradiated samples Beata Ziaja Hasylab, DESY Hamburg and INP, Krakow Prague, 23-24 November 2006 I. Mechanisms 2 Radiation damage Contribution

More information

Laser Dissociation of Protonated PAHs

Laser Dissociation of Protonated PAHs 100 Chapter 5 Laser Dissociation of Protonated PAHs 5.1 Experiments The photodissociation experiments were performed with protonated PAHs using different laser sources. The calculations from Chapter 3

More information

Femtosecond X-Ray Experiments

Femtosecond X-Ray Experiments Femtosecond X-Ray Experiments Christian Bressler FXE Hamburg, January 25, 2017 FXE Workshop Dec 2016: Users overall very happy with implemented components 2 Scientific Instrument FXE The FXE scientific

More information

Undulator Commissioning Spectrometer for the European XFEL

Undulator Commissioning Spectrometer for the European XFEL Undulator Commissioning Spectrometer for the European XFEL FEL Beam Dynamics Group meeting DESY, Hamburg, Nov. 9 th 010 Wolfgang Freund, WP74 European XFEL wolfgang.freund@xfel.eu Contents Undulator commissioning

More information

Laser-driven undulator source

Laser-driven undulator source Laser-driven undulator source Matthias Fuchs, R. Weingartner, A.Maier, B. Zeitler, S. Becker, D. Habs and F. Grüner Ludwig-Maximilians-Universität München A.Popp, Zs. Major, J. Osterhoff, R. Hörlein, G.

More information

The MEC endstation at LCLS New opportunities for high energy density science

The MEC endstation at LCLS New opportunities for high energy density science The MEC endstation at LCLS New opportunities for high energy density science Singapore, fttp-5, April 20th, 2011 Bob Nagler BNagler@slac.stanford.edu SLAC national accelerator laboratory 1 Overview Motivation

More information

Greenfield FELs. John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL

Greenfield FELs. John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL Greenfield FELs John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL BESAC Subcommittee on BES 20-year Facility Road Map February 22-24, 2003 What is a Greenfield FEL? High-gain FELs are

More information

Atomic Photoionization Dynamics in Intense Radiation Fields

Atomic Photoionization Dynamics in Intense Radiation Fields Atomic Photoionization Dynamics in Intense Radiation Fields M. Meyer LIXAM, Centre Universitaire Paris Sud, Orsay France - Introduction - Two-Color (XUV + NIR) Experiments - intense NIR - intense XUV -

More information

Comparison of nanosecond laser ablation at 1064 and 308 nm wavelength

Comparison of nanosecond laser ablation at 1064 and 308 nm wavelength Applied Surface Science 210 (2003) 262 273 Comparison of nanosecond laser ablation at 1064 and 308 nm wavelength L. Torrisi a,b, S. Gammino b, L. Andò b, V. Nassisi c,d, D. Doria c, A. Pedone c,d,* a Dipartimento

More information

XRD endstation: condensed matter systems

XRD endstation: condensed matter systems XRD endstation: condensed matter systems Justine Schlappa SCS Instrument Beamline Scientist Hamburg, January 24, 2017 2 Outline Motivation Baseline XRD setup R&D setup Two-color operation and split&delay

More information

FLASHthe first soft x-ray free electron laser (FEL) user facility

FLASHthe first soft x-ray free electron laser (FEL) user facility FLASHthe first soft x-ray free electron laser (FEL) user facility J Feldhaus To cite this version: J Feldhaus. FLASHthe first soft x-ray free electron laser (FEL) user facility. Journal of Physics B: Atomic,

More information

AMO at FLASH. FELs provide unique opportunities and challenges for AMO physics. due to essentially three reasons:

AMO at FLASH. FELs provide unique opportunities and challenges for AMO physics. due to essentially three reasons: Experience at FLASH AMO at FLASH FELs provide unique opportunities and challenges for AMO physics due to essentially three reasons: AMO at FLASH 1. huge integrated flux dilute samples Highly charged ions

More information

Polarization control experiences in single pass seeded FELs. Carlo Spezzani on behalf of

Polarization control experiences in single pass seeded FELs. Carlo Spezzani on behalf of Polarization control experiences in single pass seeded FELs Carlo Spezzani on behalf of the FERMI team & the storage ring FEL group Outline Introduction Storage Ring FEL test facility characterization

More information

Laser-induced ablation: physics and diagnostics of ion emission

Laser-induced ablation: physics and diagnostics of ion emission NUKLEONIKA 2011;56(2):113 117 ORIGINAL PAPER Laser-induced ablation: physics and diagnostics of ion emission Lorenzo Torrisi Abstract. Pulsed lasers generating beams of different intensities may be used

More information

Innovative XUV- und X-ray-Spectroscopy to explore Warm Dense Matter

Innovative XUV- und X-ray-Spectroscopy to explore Warm Dense Matter 3rd EMMI Workshop on Plasma Physics with intense Lasers and Heavy Ion Beams Innovative XUV- und X-ray-Spectroscopy to explore Warm Dense Matter Eckhart Förster X-ray Optics Group - IOQ - Friedrich-Schiller-University

More information

NONLINEAR PROCESSES IN THE EXTREME ULTRAVIOLET REGION USING THE FEL

NONLINEAR PROCESSES IN THE EXTREME ULTRAVIOLET REGION USING THE FEL NONLINEAR PROCESSES IN THE EXTREME ULTRAVIOLET REGION USING THE FEL FERMI@ELETTRA A. Dubrouil, M. Reduzzi, C. Feng, J. Hummert, P. Finetti, O. Plekan, C. Grazioli, M. Di Fraia, V. Lyamayev,A. LaForge,

More information

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX Abstract... I Acknowledgements... III Table of Content... V List of Tables... VIII List of Figures... IX Chapter One IR-VUV Photoionization Spectroscopy 1.1 Introduction... 1 1.2 Vacuum-Ultraviolet-Ionization

More information

Radiation Safety at LCLS: The Photon Beam s Maximum Capability and Material Damage Potential

Radiation Safety at LCLS: The Photon Beam s Maximum Capability and Material Damage Potential SLAC-PUB-15708 August 2013 Radiation Safety at LCLS: The Photon Beam s Maximum Capability and Material Damage Potential J.M. Bauer *1, J.C. Liu 1, A.A. Prinz 2, and S.H. Rokni 1 1 Radiation Protection

More information

Secondary Ion Mass Spectrometry (SIMS) Thomas Sky

Secondary Ion Mass Spectrometry (SIMS) Thomas Sky 1 Secondary Ion Mass Spectrometry (SIMS) Thomas Sky Depth (µm) 2 Characterization of solar cells 0,0 1E16 1E17 1E18 1E19 1E20 0,2 0,4 0,6 0,8 1,0 1,2 P Concentration (cm -3 ) Characterization Optimization

More information

Laser and pinching discharge plasmas spectral characteristics in water window region

Laser and pinching discharge plasmas spectral characteristics in water window region Laser and pinching discharge plasmas spectral characteristics in water window region P Kolar 1, M Vrbova 1, M Nevrkla 2, P Vrba 2, 3 and A Jancarek 2 1 Czech Technical University in Prague, Faculty of

More information

Fast and Slow Ligand Exchange at the Surface of Colloidal Gold Nanoparticles

Fast and Slow Ligand Exchange at the Surface of Colloidal Gold Nanoparticles Fast and Slow Ligand Exchange at the Surface of Colloidal Gold Nanoparticles Rebecca Dinkel 1, Björn Braunschweig 1,2 * and Wolfgang Peukert 1,2 1 Institute of Particle Technology (LFG), Friedrich-Alexander

More information

4. How can fragmentation be useful in identifying compounds? Permits identification of branching not observed in soft ionization.

4. How can fragmentation be useful in identifying compounds? Permits identification of branching not observed in soft ionization. Homework 9: Chapters 20-21 Assigned 12 April; Due 17 April 2006; Quiz on 19 April 2006 Chap. 20 (Molecular Mass Spectroscopy) Chap. 21 (Surface Analysis) 1. What are the types of ion sources in molecular

More information

Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers. Zhirong Huang SLAC, Stanford University May 13, 2013

Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers. Zhirong Huang SLAC, Stanford University May 13, 2013 Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers Zhirong Huang SLAC, Stanford University May 13, 2013 Introduction GE synchrotron (1946) opened a new era of accelerator-based

More information

Commissioning of the new Injector Laser System for the Short Pulse Project at FLASH

Commissioning of the new Injector Laser System for the Short Pulse Project at FLASH Commissioning of the new Injector Laser System for the Short Pulse Project at FLASH Uni Hamburg tim.plath@desy.de 05.11.2013 Supported by BMBF under contract 05K10GU2 & FS FLASH 301 Motivation short pulses

More information

Ultrafast Structural Dynamics in Solids Klaus Sokolowski-Tinten

Ultrafast Structural Dynamics in Solids Klaus Sokolowski-Tinten Ultrafast Structural Dynamics in Solids Klaus Sokolowski-Tinten Institut für Experimentelle Physik STI Round-Table Meeting, Hamburg, 22. - 24. Juni 2004 Outline motivation: why short pulses and the XFEL

More information

Short Wavelength Regenerative Amplifier FELs (RAFELs)

Short Wavelength Regenerative Amplifier FELs (RAFELs) Short Wavelength Regenerative Amplifier FELs (RAFELs) Neil Thompson, David Dunning ASTeC, Daresbury Laboratory, Warrington UK Brian McNeil Strathclyde University, Glasgow, UK Jaap Karssenberg & Peter van

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

More information

MaRIE. MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design

MaRIE. MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design Operated by Los Alamos National Security, LLC, for the U.S. Department of Energy MaRIE (Matter-Radiation Interactions in Extremes) MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design B. Carlsten, C.

More information

Free-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center

Free-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Free-electron laser SACLA and its basic Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Light and Its Wavelength, Sizes of Material Virus Mosquito Protein Bacteria Atom

More information

Detecting high energy photons. Interactions of photons with matter Properties of detectors (with examples)

Detecting high energy photons. Interactions of photons with matter Properties of detectors (with examples) Detecting high energy photons Interactions of photons with matter Properties of detectors (with examples) Interactions of high energy photons with matter Cross section/attenution length/optical depth Photoelectric

More information

MAPPING OF ATOMIC NITROGEN IN SINGLE FILAMENTS OF A BARRIER DISCHARGE MEASURED BY TWO PHOTON FLUORESCENCE SPECTROSCOPY (TALIF)

MAPPING OF ATOMIC NITROGEN IN SINGLE FILAMENTS OF A BARRIER DISCHARGE MEASURED BY TWO PHOTON FLUORESCENCE SPECTROSCOPY (TALIF) MAPPING OF ATOMIC NITROGEN IN SINGLE FILAMENTS OF A BARRIER DISCHARGE MEASURED BY TWO PHOTON FLUORESCENCE SPECTROSCOPY (TALIF) C. LUKAS, M. SPAAN, V. SCHULZ VON DER GATHEN, H. F. DÖBELE Institut für Laser

More information

Report on the XFEL STI Round Table Workshop

Report on the XFEL STI Round Table Workshop Report on the XFEL STI Round Table Workshop June 22-24th, 2004 background workshop XFEL preparatory phase Jochen R. Schneider DESY Approaching the European XFEL Facility Steering Committee chairman: H.

More information

Studies with Ultra-Short Pulses

Studies with Ultra-Short Pulses Studies with Ultra-Short Pulses E. Hass, A. Kuhl, T. Plath, M. Rehders, J. Rönsch-Schulenburg, J. Rossbach, V. Wacker: Universität Hamburg, Institut für Experimentalphysik; N.-I. Baboi, M. Bousonville,

More information

VELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab.

VELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab. VELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab. Yuri Saveliev on behalf of VELA and CLARA teams STFC, ASTeC, Cockcroft Institute Daresbury Lab., UK Outline VELA (Versatile Electron

More information

Research with Synchrotron Radiation. Part I

Research with Synchrotron Radiation. Part I Research with Synchrotron Radiation Part I Ralf Röhlsberger Generation and properties of synchrotron radiation Radiation sources at DESY Synchrotron Radiation Sources at DESY DORIS III 38 beamlines XFEL

More information

Wir schaffen Wissen heute für morgen

Wir schaffen Wissen heute für morgen Wir schaffen Wissen heute für morgen Paul Scherrer Institut Pavle Juranić, R. Ischebeck, L. Patthey, V. Schlott, C. David, C. P. Hauri, I. Gorgisyan Single Shot Spectrometer and Pulse and Arrival Time

More information

Coherent Synchrotron Radiation and Short Bunches in Electron Storage Rings. G. Wüstefeld, BESSY, Berlin (Germany)

Coherent Synchrotron Radiation and Short Bunches in Electron Storage Rings. G. Wüstefeld, BESSY, Berlin (Germany) Coherent Synchrotron Radiation and Short Bunches in Electron Storage Rings G. Wüstefeld, BESSY, Berlin (Germany) Content content 1. Introduction 2. Low alpha optics for short bunches 3. Coherent radiation

More information

INNOVATIVE IDEAS FOR SINGLE-PASS FELS

INNOVATIVE IDEAS FOR SINGLE-PASS FELS doi:10.18429/jacow-ipac2014- Abstract INNOVATIVE IDEAS FOR SINGLE-PASS FELS Toru Hara #, RIKEN SPring-8 Center, Hyogo, Japan SASE FELs (Self-Amplified Spontaneous Emission Free-Electron Lasers) are a powerful

More information

Coherence properties of the radiation from SASE FEL

Coherence properties of the radiation from SASE FEL CERN Accelerator School: Free Electron Lasers and Energy Recovery Linacs (FELs and ERLs), 31 May 10 June, 2016 Coherence properties of the radiation from SASE FEL M.V. Yurkov DESY, Hamburg I. Start-up

More information

Introduction to Free Electron Lasers and Fourth-Generation Light Sources. 黄志戎 (Zhirong Huang, SLAC)

Introduction to Free Electron Lasers and Fourth-Generation Light Sources. 黄志戎 (Zhirong Huang, SLAC) Introduction to Free Electron Lasers and Fourth-Generation Light Sources 黄志戎 (Zhirong Huang, SLAC) FEL References K.-J. Kim and Z. Huang, FEL lecture note, available electronically upon request Charles

More information

Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site

Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site 1 Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site Sakhorn Rimjaem (on behalf of the PITZ team) Motivation Photo Injector Test Facility at

More information

Results from the Optical Replica Synthesizer at FLASH

Results from the Optical Replica Synthesizer at FLASH Results from the Optical Replica Synthesizer at FLASH Shaukat Khan, University of Hamburg FEL 2008, Gyeongju, Korea G. V. Angelova, V. Ziemann ( UU/ISV, Uppsala, Sweden) M. Larsson, P. van der Meulen,

More information

The Story of Xe 21+ at FLASH

The Story of Xe 21+ at FLASH X ray Science in the 21th Century Santa Barbara, August 2 to 6, 2010 The Story of Xe 21+ at FLASH M. Richter Physikalisch Technische Bundesanstalt (PTB) I PB Multiple Ionization of Xenon in the EUV (13.3

More information

Answers to questions on exam in laser-based combustion diagnostics on March 10, 2006

Answers to questions on exam in laser-based combustion diagnostics on March 10, 2006 Answers to questions on exam in laser-based combustion diagnostics on March 10, 2006 1. Examples of advantages and disadvantages with laser-based combustion diagnostic techniques: + Nonintrusive + High

More information

Fundamental investigation on CO 2 laser-produced Sn plasma for an EUVL source

Fundamental investigation on CO 2 laser-produced Sn plasma for an EUVL source Fundamental investigation on CO 2 laser-produced Sn plasma for an EUVL source Yezheng Tao*, Mark Tillack, Kevin Sequoia, Russel Burdt, Sam Yuspeh, and Farrokh Najmabadi University of California, San Diego

More information

Nonlinear Optics (WiSe 2015/16) Lecture 12: January 15, 2016

Nonlinear Optics (WiSe 2015/16) Lecture 12: January 15, 2016 Nonlinear Optics (WiSe 2015/16) Lecture 12: January 15, 2016 12 High Harmonic Generation 12.1 Atomic units 12.2 The three step model 12.2.1 Ionization 12.2.2 Propagation 12.2.3 Recombination 12.3 Attosecond

More information

Small Quantum Systems Scientific Instrument

Small Quantum Systems Scientific Instrument Small Quantum Systems Scientific Instrument WP-85 A. De Fanis, T. Mazza, H. Zhang, M. Meyer European XFEL GmbH TDR_2012: http://www.xfel.eu/documents/technical_documents XFEL Users Meeting 2014, January

More information

Laser Ablation for Chemical Analysis: 50 Years. Rick Russo Laser Damage Boulder, CA September 25, 2012

Laser Ablation for Chemical Analysis: 50 Years. Rick Russo Laser Damage Boulder, CA September 25, 2012 Laser Ablation for Chemical Analysis: 50 Years Rick Russo Lawrence Berkeley National Laboratory Applied Spectra, Inc 2012 Laser Damage Boulder, CA September 25, 2012 Laser Ablation for Chemical Analysis:

More information

Study of matter in extreme conditions using 4th generation FEL light sources

Study of matter in extreme conditions using 4th generation FEL light sources Study of matter in extreme conditions using 4th generation FEL light sources Sam Vinko Department of Physics Clarendon Laboratory University of Oxford Workshop on Science with Free Electron Lasers Shanghai,

More information

Synchrotron Methods in Nanomaterials Research

Synchrotron Methods in Nanomaterials Research Synchrotron Methods in Nanomaterials Research Marcel MiGLiERiNi Slovak University of Technology in Bratislava and Centre for Nanomaterials Research, Olomouc marcel.miglierini@stuba.sk www.nuc.elf.stuba.sk/bruno

More information

X-ray photoelectron spectroscopy with a laser-plasma source

X-ray photoelectron spectroscopy with a laser-plasma source Proc. SPIE Vol.3157 (1997) pp.176-183 X-ray photoelectron spectroscopy with a laser-plasma source Toshihisa TOMIE a, Hiroyuki KONDO b, Hideaki SHIMIZU a, and Peixiang Lu a a Electrotechnical Laboratory,

More information

Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI)

Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI) Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI), 2003, A dedicated proton accelerator for 1p-physics at the future GSI Demands facilities for

More information

Hiromitsu TOMIZAWA XFEL Division /SPring-8

Hiromitsu TOMIZAWA XFEL Division /SPring-8 TUPLB10 (Poster: TUPB080) Non-destructive Real-time Monitor to measure 3D- Bunch Charge Distribution with Arrival Timing to maximize 3D-overlapping for HHG-seeded EUV-FEL Hiromitsu TOMIZAWA XFEL Division

More information

EUV-Technology with Discharge EUV-Lamp"

EUV-Technology with Discharge EUV-Lamp EUV-Technology with Discharge EUV-Lamp" Rainer Lebert, Larissa Juschkin, Christian Wies, Bernhard Jägle, Manfred Meisen, Ulrich Bieberle, Willi Neff, Juri Barthel, Konstantin Walter, Klaus Bergmann, Fraunhofer

More information

Influence of gas conditions on electron temperature inside a pinch column of plasma-focus discharge

Influence of gas conditions on electron temperature inside a pinch column of plasma-focus discharge Journal of Physics: Conference Series PAPER OPEN ACCESS Influence of gas conditions on electron temperature inside a pinch column of plasma-focus discharge To cite this article: D R Zaloga et al 218 J.

More information

Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics

Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics Richard Haight IBM TJ Watson Research Center PO Box 218 Yorktown Hts., NY 10598 Collaborators Al Wagner Pete Longo Daeyoung

More information

Length of beam system = 910m. S. Reiche X var = ~50m ~ 650m / Y. Kim FEL-KY ~150m. ~60m. LaserHutch2 (access during operation)

Length of beam system = 910m. S. Reiche X var = ~50m ~ 650m / Y. Kim FEL-KY ~150m. ~60m. LaserHutch2 (access during operation) Laser Laser HHG Diagnostic ATHOS PORTHOS ARAMIS THz-Pump P A U L S C H E R R E R I N S T I T U T Length of beam system = 910m &'!( Test & Commissioning steps (A,B,C) A11 Conv. Gun & Injector A12 LINAC

More information

INVESTIGATIONS OF THE DISTRIBUTION IN VERY SHORT ELECTRON BUNCHES LONGITUDINAL CHARGE

INVESTIGATIONS OF THE DISTRIBUTION IN VERY SHORT ELECTRON BUNCHES LONGITUDINAL CHARGE INVESTIGATIONS OF THE LONGITUDINAL CHARGE DISTRIBUTION IN VERY SHORT ELECTRON BUNCHES Markus Hüning III. Physikalisches Institut RWTH Aachen IIIa and DESY Invited talk at the DIPAC 2001 Methods to obtain

More information

Trends in X-ray Synchrotron Radiation Research

Trends in X-ray Synchrotron Radiation Research Trends in X-ray Synchrotron Radiation Research Storage rings Energy Recovery Linacs (ERL) Free Electron Lasers Jochen R. Schneider DESY Development of the brilliance of X-ray sources Since the discovery

More information