Time-Resolved X-Ray. with One Trillion Photons. XDL Workshop tickle and probe, Cornell University, June 21, 2011
|
|
- Cameron Richards
- 5 years ago
- Views:
Transcription
1 Time-Resolved X-Ray Spectroscopies and Scattering with One Trillion Photons Christian Bressler XDL Workshop tickle and probe, Cornell University, June 21, 2011
2 Dynamic Studies in Photochemistry Ru(bpy) 3 (aq) 1. Intramolecular Charge Transfer Absorption / a.u. 0,5 0,4 03 0,3 0,2 0,1 0, X-Ray XRay Probe Energy / ev 2. Towards Solvation Dynamics Absorption / a.u. 1,0 0,5 0,0 I - I 0 Nascent I 0 (aq) X-Ray Probe Energy (ev) 3. Light-Induced Spin Crossover Fe(bpy) 3 (aq)
3 What are the fundamental timescales? Chemistry and Biochemistry Photosynthesis Vision Molecular Vibrations Protein Folding Strings, Particle Molecular l Rotations ti Cosmology Collisions Electron dynamics harpo yacto zepto atto femto pico nano micro milli Time /seconds
4 Now for the low-lying fruit (K edges) RIXS, X-Ray Raman Valence XES K XES Transm ansmission XAFS Fluorescence XAFS , Aqueous Sample Concentation / mm Incident Photons for S/N = 10
5 Towards Solvation Dynamics -Distinguishg IVR from guest-host interactions -Example: NO/Rg matrix
6 Rydberg NO in rare gas matrices: bubble formation
7 Ultrafast Processes in the Condensed n d Phase (of any kind) Speed of Sound: >10 Å/ps ca Solvent Molecules l involved X-Ray Absorption Spectroscopy X Ray Absorption Spectroscopy Singles Out Reaction Center...
8 Electron Detachment Reactions (via XAFS) 2s 5p Absorption / a.u. 1,0 0,5 0,0 I - I X-Ray Probe Energy (ev) Pham et al., JACS (2007) Nascent I atoms in solution I. Tavernelli (EPFL)
9 EXAFS and XANES of nascent iodine radicals static 300 fs 50 ps 50 ps 300 fs 50 ps V.-T. Pham et al. Chem. Phys. (2010) V.-T. Pham, PhD thesis (2010) V.-T. Pham et al. Submitted (2011) I - I 0
10 Now to something completely different. LS HS 10 C. Consani et al. Angew Chem (2009)
11 Towards Transient Structures via TR-XAFS A / a.u. 0 3 A x 1 1 HS LS 50 ps X-Ray Probe Energy / ev 665 ps (k) x k 2 0 Photoelectron Wavevector k / Å t < t = 50 ps Exp. (Ground State) Fit R Fe-N = 0.2 ±0.008 Å M. Benfatto (INFN Rome) B k 2 (k) x k 70 ps 0 W. Gawelda et al. 11 Phys. Rev. Lett. (2007) Exp. (Transient) Fit Photoelectron Wavevector k / Å -1 W. Gawelda et al. J. Chem. Phys. (2009)
12 ps and fs XANES (Synchrotron) A / a.u u. x 10 3 A HS LS 50 ps 300 fs X-Ray Probe Energy / ev C. Bressler et al., Science (2009)
13 Identifying intermediate states... R Fe-N N =0.2 Å Time Delay / fs 250 fs (instrument response): 140(30) fs hard x-ray pulse 115(10) fs laser pulse <100(30) fs time zero drifts photons/pulse (2 khz, 2 ev BW)
14 Combined optical and x-ray results?? b) 20 fs 1 MLCT 3 MLCT 120 fs <130 fs Energy 1 A 1 (LS) R (Fe-N) 5 T (HS) ps Need now a Spin-Sensitive Sensitive Tool!!
15 Spin sensitivity e 3p 2p IP 1s Courtesy: Pieter Glatzel (ESRF)
16 1s XES of a spin transition molecule exchange (J) 3d n p 1s2p 1s3p 1sVB 1s Fe II 3d 6 S = 0 2 T,p h G. Vankó et al., J. Phys. Chem. B 110 (2006) 11647
17 Towards ultrafast X-ray Emission Spectroscopy ph/pulse (100 ps) ph/pulse (200 fs) 10-3 ph/pulse (100 ps XES) a) b) D1 D2 X L S D3 c) T = 960 ns Ge(440) Laser 0.5 ms G. Vankó et al., Angew. Chem. Int. Ed. (2010)
18 Direct spin probing: first TR-XES (ps) Femtosecond Time Resolution Ideally suited for single wavelength XFEL experiments MHz repetition rates!!!! G. Vanko et al., Angew. Chem. Int. Ed., (2010)
19 MHz Laser Installation at ESRF Ready to Pump-Probe at MHz rep-rates!! 19
20 ID26 X-ray Emission/Absorption Spectroscopy MHz
21 21 ID26/ESRF (March 2011)
22 22 APS, sector 7 (March 2011)
23 Picosecond K alpha XES at APS 1 khz pp studies at SLS (Angew. Chem. 2010) 0.13 MHz at APS 23
24 back to the future: Entering the femtosecond time scale (again) Linac coherent light source (LCLS) Credits: D. Fritz, M. Cammarata (SLAC)
25 XPP Commissioning (LCLS, Oct 2010) (Cammarata)
26 One single File (10 min scan) at LCLS
27 Oct 2010: XPP commissioning XANES / a.u. Tra ansient 0,1 0,0 SLS ( t = 50 ps) SLS ( t = 300 fs) f ) XPP ( t = fs) X-Ray Probe Energy / ev
28 Real-Time Traces sorption X-Ra ay Trans sient Ab 0,003 0,002 0,001 0,000 Science 2009 Fit curve 2009 XPP , Laser-X-RayTimeDelay/fs
29 Transient Spectra around Time Zero 0,036 0,06 Trans sient XANES 0,034 0,032 XANES 0,04 0, Laser X-Ray Time Delay / fs 0,00 Po opulation 1,0 0,9 0,8 0,1 1,3 MLCT 1 GS 5 HS Spin Flip? Tra ansient XAN NES 0,0025 0, , Time / fs X-Ray Probe Energy / ev
30 Looking into the raw data
31 Summary of combined optical/xas studies?? e g t 2g 120 fs a) Energy 1,3 MLCT 1 T 2 1 T 1 3 T 2 1,3 T :<60 fs 5 E 3 T 1 1 A 1 5 T 2 R (Fe-N) Need to include XES (spin) and even XRD (solvent) experiments at APS/ESRF to prepare for LCLS
32 Next Step: Exploit Complementary Structural Tools (LCLS project 2011): Towards understanding chemical reactivity e - XES: occupied DOS (spin) XAS: empty DOS (orbitals) XRD: geometric structures Collaboration: 1) Ru(II) Ru(III) (XAS, XES, optical) 2) IVR + e-transport (XRD, optical) 3) Co(III) Co(II) (XAS, XES, optical) 4) Co(II) LS HS (XAS, XES) M. Nielsen (Copenhagen) V. Sundström dtö (Lund) G. Vanko (Budapest) P. Glatzel (ESRF) A. Meents (Petra3) R. Abela (SwissFEL)
33 Conclusions Towards Solvation Dynamics Absorption / a.u. 1,0 0,5 0,0 I - I 0 Nascent I 0 (aq) X-Ray Probe Energy (ev) - We can follow the sequence of events from 300 fs onwards Even the (few) ps time scale we do not fully understand Theoretical input important - We need to know how things evolve between fs New experiments are planned (theory required) Light-Induced Spin Crossover Fe(bpy) 3 (aq) - We do not understand this correlated SCO behavior! but we are already looking into the elementary steps!!!
34 Acknowledgments 34 University of Copenhagen - Martin Meedom Nielsen - Kristoffer Haldrup Lund University - Villy Sundström - Sophie Canton - Jens Uhlig - Grigory Smolentsev SwissFEL - Rafael labela Argonne National Lab (APS) - Steven Southworth - Anne-Marie March (MHz laser) - Gilles Doumy - Elliot Kanter - Dipanwita Ray - Robert Dunford - Linda Young KFKI Budapest - György Vankó ESRF European XFEL Facility - Pieter Glatzel - Wojciech Gawelda - Erik Gallo - Andreas Galler LCLS (SLAC) K. Gaffney, L. X. Chen, H. Ihee - David Fritz, Marco Cammarata (XPP Oct 2010)
Tracking chemical reactions using combined time-resolved x- ray spectroscopies and scattering
Tracking chemical reactions using combined time-resolved x- ray spectroscopies and scattering Workshop on MXAN code for XANES analysis IP PAS, Warsaw, Poland April 8, 2014 Alexander Britz and Tadesse Assefa
More informationFemtosecond 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 informationXFEL User Meeting, Hamburg, Jan 28, 2015
Femtosecond X-Ray Experiments at the European XFEL Christian Bressler, Femtosecond X-ray Experiments (FXE) Instrument European XFEL XFEL User Meeting, Hamburg, Jan 28, 2015 Experiment Hall Integration
More informationTime Resolved (Pump Probe) Experiment to watch structural dynamics by using the pulsed nature of synchrotron radiation
SESAME-JSPS School November 14-16, 2011 Amman, Jordan Time Resolved (Pump Probe) Experiment to watch structural dynamics by using the pulsed nature of synchrotron radiation Shin-ichi Adachi (Photon Factory,
More informationX-Ray Spectroscopy at LCLS
LCLS proposal preparation workshop for experiments at XPP, June 21, 2008, SLAC, Menlo Park, CA ħω ħω e - X-Ray Spectroscopy at LCLS Uwe Bergmann SSRL Stanford Linear Accelerator Center bergmann@slac.stanford.edu
More informationUltrafast nanoscience with ELI ALPS
Ultrafast nanoscience with ELI ALPS Péter Dombi Wigner Research Centre for Physics, Budapest & Max Planck Institute of Quantum Optics, Garching Overview ultrafast (femtosecond/attosecond) dynamicsin metal
More informationCore Level Spectroscopies
Core Level Spectroscopies Spectroscopies involving core levels are element-sensitive, and that makes them very useful for understanding chemical bonding, as well as for the study of complex materials.
More informationDIFFRACTION UNDER LASER IRRADIATION. ANF RECIPROCS C. Mariette
DIFFRACTION UNDER LASER IRRADIATION ANF RECIPROCS- 2018 C. Mariette Okhoshi et al., Nat. Chem.(2010) Calculated DOS of photo-switchable Ti 3 O 5 Photochromism Conductivity Insulating Metal This also
More informationX-ray Transient Absorption (XTA) Spectroscopy: A Decade and Beyond
Ultrafast Science with Tickel and Probe, June 20-21, 2011, XDL2011 Workshop 3, CHESS, Cornell University, Ithaca, New York X-ray Transient Absorption (XTA) Spectroscopy: A Decade and Beyond Lin X. Chen
More informationToward Fourier-limited X-ray Science
XDL2011 RPCC, Cornell Univ. June 20-21, 2011 GRC X-ray Science 2009 Colby College August 2-7, 2009 Toward Fourier-limited X-ray Science Photon Factory, KEK & PREST, JST Shin-ichi Adachi outline Time-domain
More informationUltrafast X-ray Spectroscopy of Solvated Transition-metal Complexes and Oxide Materials
Ultrafast X-ray Spectroscopy of Solvated Transition-metal Complexes and Oxide Materials Robert Schoenlein Materials Sciences Division Chemical Sciences Division - UXSL Matteo Rini ils Huse F. Reboani &
More informationTime-resolved Diffuse Scattering: phonon spectoscopy with ultrafast x rays
Time-resolved Diffuse Scattering: phonon spectoscopy with ultrafast x rays David A. Reis PULSE Institute, Departments of Photon Science and Applied Physics, Stanford University SLAC National Accelerator
More informationUnsolved problems in biology
Unsolved problems in biology What can advanced x-ray spectroscopy contribute? James Penner-Hahn Biophysics Research Division and Department of Chemistry The University of Michigan Metalloproteins 30-50%
More informationAttosecond Science. Jon Marangos, Director Extreme Light Consortium, Imperial College London
Attosecond Science Jon Marangos, Director Extreme Light Consortium, Imperial College London Electron Orbit in Bohr Model T orbit 150 as for H ground state Electron Motion In most matter electrons are in
More informationOpportunities and Challenges for X
Opportunities and Challenges for X -ray Free Electron Lasers for X-ray Ultrafast Science J. Hastings Stanford Linear Accelerator Center June 22, 2004 European XFEL Laboratory How Short is short? defined
More informationProbing Matter: Diffraction, Spectroscopy and Photoemission
Probing Matter: Diffraction, Spectroscopy and Photoemission Anders Nilsson Stanford Synchrotron Radiation Laboratory Why X-rays? VUV? What can we hope to learn? 1 Photon Interaction Incident photon interacts
More informationOptical Spectroscopy of Advanced Materials
Phys 590B Condensed Matter Physics: Experimental Methods Optical Spectroscopy of Advanced Materials Basic optics, nonlinear and ultrafast optics Jigang Wang Department of Physics, Iowa State University
More informationPhoton Interaction. Spectroscopy
Photon Interaction Incident photon interacts with electrons Core and Valence Cross Sections Photon is Adsorbed Elastic Scattered Inelastic Scattered Electron is Emitted Excitated Dexcitated Stöhr, NEXAPS
More informationSpectroscopy of Nanostructures. Angle-resolved Photoemission (ARPES, UPS)
Spectroscopy of Nanostructures Angle-resolved Photoemission (ARPES, UPS) Measures all quantum numbers of an electron in a solid. E, k x,y, z, point group, spin E kin, ϑ,ϕ, hν, polarization, spin Electron
More informationPerformance Metrics of Future Light Sources. Robert Hettel, SLAC ICFA FLS 2010 March 1, 2010
Performance Metrics of Future Light Sources Robert Hettel, SLAC ICFA FLS 2010 March 1, 2010 http://www-ssrl.slac.stanford.edu/aboutssrl/documents/future-x-rays-09.pdf special acknowledgment to John Corlett,
More informationUltrafast XAFS Studies on the Photoabsorption Processe
Ultrafast XAFS Studies on the Photoabsorption Processe Kiyotaka Asakura 1, Yohei Uemura 2 and Toshihiko Yokoyama 3, 1 Institute for Catalyst, Hokkaido University, 2Utrecht University 3Institute for Molecular
More informationThe Lund Attosecond Science Centre in the MEDEA network PER THE MEDEA KICK-OFF MEETING, BERLIN, JANUARY 2015
The Lund Attosecond Science Centre in the MEDEA network PER JOHNSSON @ THE MEDEA KICK-OFF MEETING, BERLIN, JANUARY 2015 Lund University Founded in 1666 47 700 students (individuals) 7 500 employees - 840
More informationReceived: January 19, 2015 Revised: February 24, 2015 Published: February 25, 2015
This is an open access article published under a Creative Commons Attribution (CC-BY) License, which permits unrestricted use, distribution and reproduction in any medium, provided the author and source
More informationCOOPERATIVE ELASTIC SWITCHING IN VOLUME-CHANGING MAGNETIC MATERIALS TRIGGERED BY FEMTOSECOND MOLECULAR PHOTOSWITCHING.
COOPERATIVE ELASTIC SWITCHING IN VOLUME-CHANGING MAGNETIC MATERIALS TRIGGERED BY FEMTOSECOND MOLECULAR PHOTOSWITCHING. E. Collet, R. Bertoni, H. Cailleau, M. Buron, M. Lorenc, M. Cammarata S. Zerdane,
More informationX-ray Photon Correlation Spectroscopy (XPCS) at Synchrotron and FEL sources
X-ray Photon Correlation Spectroscopy (XPCS) at Synchrotron and FEL sources Christian Gutt Department of Physics, University ofsiegen, Germany gutt@physik.uni-siegen.de Outline How to measure dynamics
More informationI. Transient Absorption Spectroscopy
I. Transient Absorption Spectroscopy Setup The femtosecond laser setup used to record the transient absorption (TA) data was based on a Spitfire Pro XP amplifier seeded by a Mai Tai (both from Spectra-Physics).
More informationHigh Energy Upgrade: LCLS-II-HE High Repetition Rate Soft X-rays Hard X-rays
High Energy Upgrade: LCLS-II-HE High Repetition Rate Soft X-rays Hard X-rays Electronic & nuclear coupling Emergent properties Materials heterogeneity lattice spin charge orbital LCLS-II-HE provides: Ultrafast
More informationX-ray Absorption Spectroscopy. Kishan K. Sinha Department of Physics and Astronomy University of Nebraska-Lincoln
X-ray Absorption Spectroscopy Kishan K. Sinha Department of Physics and Astronomy University of Nebraska-Lincoln Interaction of X-rays with matter Incident X-ray beam Fluorescent X-rays (XRF) Scattered
More informationSfb 658 Colloquium 11 May Part II. Introduction to Two-Photon-Photoemission (2PPE) Spectroscopy. Martin Wolf
Sfb 658 Colloquium 11 May 2006 Part II Introduction to Two-Photon-Photoemission (2PPE) Spectroscopy Martin Wolf Motivation: Electron transfer across interfaces key step for interfacial and surface dynamics
More informationFemtosecond X ray Absorption Spectroscopy at a Hard X ray Free Electron Laser: Application to Spin Crossover Dynamics
pubs.acs.org/jpca Femtosecond X ray Absorption Spectroscopy at a Hard X ray Free Electron Laser: Application to Spin Crossover Dynamics Henrik T. Lemke, Christian Bressler, Lin X. Chen, David M. Fritz,
More informationPart 1: What is XAFS? What does it tell us? The EXAFS equation. Part 2: Basic steps in the analysis Quick overview of typical analysis
Introduction to XAFS Part 1: What is XAFS? What does it tell us? The EXAFS equation Part 2: Basic steps in the analysis Quick overview of typical analysis Tomorrow Measurement methods and examples The
More informationBrazilian Synchrotron Radiation and Laser/X-rays experiments
Brazilian Synchrotron Radiation and Laser/X-rays experiments Frederico Alves Lima Centro Nacional de Pesquisa em Energia e Materiais - CNPEM Laboratório Nacional de Luz Síncrotron - LNLS International
More informationElectronic Structure and Oxidation State Changes in the Mn 4 Ca Cluster of
SLAC-PUB-15218 Electronic Structure and Oxidation State Changes in the Mn 4 Ca Cluster of Photosystem II Junko Yano, 1 Yulia Pushkar, 1 Johannes Messinger, 2 Uwe Bergmann, 3 Pieter Glatzel, 4 Vittal K.
More informationUltrafast surface carrier dynamics in topological insulators: Bi 2 Te 3. Marino Marsi
Ultrafast surface carrier dynamics in topological insulators: Bi 2 Te 3 Marino Marsi Laboratoire de Physique des Solides CNRS UMR 8502 - Université Paris-Sud IMPACT, Orsay, September 2012 Outline Topological
More informationUltrafast Radiation Chemistry and the Development of Laser Based Electron Sources*
Ultrafast Radiation Chemistry and the Development of Laser Based Electron Sources* Robert A. Crowell Chemistry Division Argonne National Laboratory International Conference on Transient Chemical Structures
More informationUltrafast XPCS. Gerhard Grübel
. Ultrafast XPCS Gerhard Grübel W.Roseker, S. Lee, F. Lehmkühler, I. Steinke, H. Schulte-Schrepping, M. Walther, G.B. Stephenson, P. Fuoss, M. Sikorski, and A. Robert DESY Deutsches Elektronen Synchrotron,
More informationWP-3: HHG and ultrafast electron imaging
WORKPACKAGE WP-3: HHG and ultrafast electron imaging Coordinators: P. Salières (CEA), A. Assion (FEMTO, Spectra Physics Vienna) Period: Start Month 4 End Month 48 Leading Participants (Orange in the picture):
More informationPERSpECTIVES. The ultrafast X- ray spectroscopic revolution in chemical dynamics
Corrected: Publisher Correction PERSpECTIVES The ultrafast X- ray spectroscopic revolution in chemical dynamics Peter M. Kraus, Michael Zürch, Scott K. Cushing, Daniel M. Neumark Stephen R. Leone Abstract
More informationTime-resolved photoelectron spectroscopy: An ultrafast clock to study electron dynamics at surfaces, interfaces and condensed matter
Time-resolved photoelectron spectroscopy: An ultrafast clock to study electron dynamics at surfaces, interfaces and condensed matter Benjamin Stadtmüller Department of Physics and Research Center OPTIMAS,
More informationAdvanced Photon-In Photon-Out Hard X-ray Spectroscopy
FLS 2010, ICFA Beam Dynamics Workshop, SLAC, Menlo Park, CA, March 2, 2010 ħω ħω e - Advanced Photon-In Photon-Out Hard X-ray Spectroscopy Uwe Bergmann Linac Coherent Light Source SLAC National Accelerator
More informationHierarchical Dynamics of Soft Matters & Prospects of Japanese Future Light Sources
XDL Workshop 6 @ Cornell Univ. Hierarchical Dynamics of Soft Matters & Prospects of Japanese Future Light Sources Yuya Shinohara Department of Advanced Materials Science, Graduate School of Frontier Sciences,
More informationMolecular Dynamics Studied by Picosecond X-ray Diffraction
Paris 17-3-25 Molecular Dynamics Studied by Picosecond X-ray Diffraction Experiments: Theory: Maciej Lorenc, Qingyu Kong, Manuela Lo Russo, Marco Cammarata, Michael Wulff Savo Bratos, Rodolphe Vuilleumier,
More informationPhoto-magnetic transitions: Spin crossover molecules
Photo-magnetic transitions: Spin crossover molecules Amandine Bellec amandine.bellec@univ-paris-diderot.fr Laboratoire Matériaux et Phénomènes Quantiques (Université Paris Diderot/CNRS) Sept 2018 Amandine
More informationRadboud Universeit Nijmegen
Magnetism and Light Theo Rasing Radboud Universeit Nijmegen Challenges Magnetism and on the Opportunities timescale of fth the exchange interaction ti Theo Rasing Radboud University Nijmegen JFe-Fe=1.4x10-19
More informationUltrafast laser-plasma sources for 50-fs hard x-ray pulse generation and laser pump x-ray probe measurements of solvated transition metal complexes
Ultrafast laser-plasma sources for 50-fs hard x-ray pulse generation and laser pump x-ray probe measurements of solvated transition metal complexes ERL Workshop, Cornell University June 2006 C. Rose-Petruck
More informationAdditional information on J. Chem. Phys. W. Gawelda, V.-T. Pham, R. M. van der Veen, D. Grolimund, R. Abela et al.
Structural analysis of ultrafast extended x-ray absorption fine structure with subpicometer spatial resolution: Application to spin crossover complexes W. Gawelda, V.-T. Pham, R. M. van der Veen, D. Grolimund,
More informationResearch 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 informationThe 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 informationElectron Dynamiχ MPRG Fritz-Haber-Institut der Max-Planck-Gesellschaft
Electron Dynamiχ MPRG Fritz-Haber-Institut der Max-Planck-Gesellschaft How exciting! 2016 Berlin, 3-6 August laura.foglia@elettra.eu 1 Current research challenges V Light Harvesting Light Emission Energy
More informationThe 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 informationPolarization 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 informationSHIELDING CALCULATIONS FOR THE HARD X-RAY GENERATED BY LCLS MEC LASER SYSTEM R. QIU, J. C. LIU, S. H. ROKNI AND A. A. PRINZ
SLAC-PUB-14159 SHIELDING CALCULATIONS FOR THE HARD X-RAY GENERATED BY LCLS MEC LASER SYSTEM R. QIU, J. C. LIU, S. H. ROKNI AND A. A. PRINZ SLAC National Accelerator Laboratory: 2575 Sand Hill Road, Menlo
More informationNew Electron Source for Energy Recovery Linacs
New Electron Source for Energy Recovery Linacs Ivan Bazarov 20m Cornell s photoinjector: world s brightest electron source 1 Outline Uses of high brightness electron beams Physics of brightness High brightness
More informationX-ray Spectroscopy Theory Lectures
TIMES Lecture Series SIMES-SLAC-Stanford Winter, 2017 X-ray Spectroscopy Theory Lectures J. J. Rehr I. Introduction to the Theory of X-ray spectra II. Real-space Green's function Theory and FEFF III. Inelastic
More informationWorkshop Overview & Charge, Science Examples, Instrumentation R&D. Bill Schlotter Feb. 9, 2015
Workshop Overview & Charge, Science Examples, Instrumentation R&D Bill Schlotter Feb. 9, 2015 Outline Workshop Charge Workshop Format Breakout activities Scientific Opportunity Example From workshops to
More informationSPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS
LCLS Technical Advisory Committee December 10-11, 2001. SPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS Patrick Krejcik LCLS Technical Advisory Committee Report 1: July 14-15, 1999 The
More informationOut-of-equilibrium electron dynamics in photoexcited topological insulators studied by TR-ARPES
Cliquez et modifiez le titre Out-of-equilibrium electron dynamics in photoexcited topological insulators studied by TR-ARPES Laboratoire de Physique des Solides Orsay, France June 15, 2016 Workshop Condensed
More informationScientific opportunities with ultrafast electron diffraction & microscopy
Scientific opportunities with ultrafast electron diffraction & microscopy Jim Cao Frontier of ultrafast science MeV UED Transition pathways Rate and time scale Elementary steps Probe dynamics on the atomic
More informationHigh-Resolution Molybdenum K-edge X-ray Absorption Spectroscopy analyzed with Time-Dependent Density Functional Theory: Supplementary Information
High-Resolution Molybdenum K-edge X-ray Absorption Spectroscopy analyzed with Time-Dependent Density Functional Theory: Supplementary Information Frederico A. Lima, a Ragnar Björnsson, a Thomas Weyhermüller,
More informationSpectroscopies for Unoccupied States = Electrons
Spectroscopies for Unoccupied States = Electrons Photoemission 1 Hole Inverse Photoemission 1 Electron Tunneling Spectroscopy 1 Electron/Hole Emission 1 Hole Absorption Will be discussed with core levels
More informationA facility for Femtosecond Soft X-Ray Imaging on the Nanoscale
A facility for Femtosecond Soft X-Ray Imaging on the Nanoscale Jan Lüning Outline Scientific motivation: Random magnetization processes Technique: Lensless imaging by Fourier Transform holography Feasibility:
More informationRichard Miles and Arthur Dogariu. Mechanical and Aerospace Engineering Princeton University, Princeton, NJ 08540, USA
Richard Miles and Arthur Dogariu Mechanical and Aerospace Engineering Princeton University, Princeton, NJ 08540, USA Workshop on Oxygen Plasma Kinetics Sept 20, 2016 Financial support: ONR and MetroLaser
More informationTitle: Ultrafast photocurrent measurement of the escape time of electrons and holes from
Title: Ultrafast photocurrent measurement of the escape time of electrons and holes from carbon nanotube PN junction photodiodes Authors: Nathaniel. M. Gabor 1,*, Zhaohui Zhong 2, Ken Bosnick 3, Paul L.
More informationSPPS: New Science on the way to LCLS
SPPS: New Science on the way to LCLS Aaron Lindenberg SLAC/SSRL FEL2004 9/02/04 UC Berkeley DESY Roger W. Falcone Jochen Schneider Aaron Lindenberg Thomas Tschentscher Donnacha Lowney Horst Schulte-Schrepping
More informationSonder et impacter les matériaux aux échelles de temps ultra-rapides
Sonder et impacter les matériaux aux échelles de temps ultra-rapides GDR Meeticc Latresne 28_31 mars 2017 Eric Collet Institut de Physique de Rennes, F-35000 Rennes, France. eric.collet@univ-rennes1.fr
More informationX-Ray Emission Spectroscopy
X-Ray Emission Spectroscopy Axel Knop-Gericke knop@fhi-berlin.mpg.de Core Level Spectroscopy Anders Nilsson. Journal of Electron Spectroscopy and Related Phenomena 126 (2002) 3-42 Creation of core holes
More informationMike Towrie Central Laser Facility Rutherford Appleton Laboratory. Diamond DIAMOND. Tony Parker, Pavel Matousek
Ultrafast deactivation of the electronic excited states of DNA bases and polynucleotides following 267 nm laser excitation explored using picosecond time-resolved infrared spectroscopy 1 Mike Towrie (m.towrie@rl.ac.uk)
More informationICPEAC XXX, Carins, Australia. Nonlinear resonant Auger spectroscopy in CO using an x-ray pump-control scheme 2017/07/31
ICPEAC XXX, Carins, Australia Nonlinear resonant Auger spectroscopy in CO using an x-ray pump-control scheme Song-Bin Zhang Shaanxi Normal University, Xi an, China 2017/07/31 Acknowledgements Victor Kimberg
More informationOrganometallic alkane and noble-gas complexes in conventional and supercritical fluids*
Pure Appl. Chem., Vol. 73, No. 3, pp. 443 447, 2001. 2001 IUPAC Organometallic alkane and noble-gas complexes in conventional and supercritical fluids* Gavin I. Childs, David C. Grills, Xue Z. Sun, and
More informationTheoretical Photochemistry WiSe 2016/17
Theoretical Photochemistry WiSe 2016/17 Lecture 8 Irene Burghardt burghardt@chemie.uni-frankfurt.de) http://www.theochem.uni-frankfurt.de/teaching/ Theoretical Photochemistry 1 Topics 1. Photophysical
More informationPump-Probe EXAFS or Probing Structural and Electronic Excitations with X-rays
Pump-Probe EXAFS or Probing Structural and Electronic Excitations with X-rays Klaus Attenkofer (ANL) Michael Goerlich Guvenc Akgul Stefan Groissmeier Guy Jennings Chuck Kurtz Xiaoyi Zhang Lin X. Chen (ANL)
More informationUltrafast X-ray Studies of Complex Materials: Science Challenges and Opportunities
Ultrafast X-ray Studies of Complex Materials: Science Challenges and Opportunities Lawrence Berkeley National Laboratory Robert Schoenlein Materials Sciences Division - Chemical Sciences Division Ultrafast
More information"Molecular Photochemistry - how to study mechanisms of photochemical reactions?"
"Molecular Photochemistry - how to study mechanisms of photochemical reactions?" Bronislaw Marciniak Faculty of Chemistry, Adam Mickiewicz University, Poznan, Poland 2014/2015 - lecture 4 Contents 1. Introduction
More informationNanotechnology and Solar Energy. Solar Electricity Photovoltaics. Fuel from the Sun Photosynthesis Biofuels Split Water Fuel Cells
Nanotechnology and Solar Energy Solar Electricity Photovoltaics Fuel from the Sun Photosynthesis Biofuels Split Water Fuel Cells Solar cell A photon from the Sun generates an electron-hole pair in a semiconductor.
More informationSet-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source
Set-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source C. Blome, K. Sokolowski-Tinten *, C. Dietrich, A. Tarasevitch, D. von der Linde Inst. for Laser- and
More informationUltrafast electron transfer studied by picosecond pulse radiolysis, new redox reactions. Mehran Mostafavi, April 2017, Vienna, Austria H 2 O * H 2 O
Ultrafast electron transfer studied by picosecond pulse radiolysis, new redox reactions Mehran Mostafavi, April 2017, Vienna, Austria e hyd H 3 O + H 2 O * H 2 O H 2 O H 2 O + S e 1 Mostafavi, AIEA, April
More informationFLASH 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 informationThe Initial Process of Photoinduced Phase Transition in an Organic Electron-Lattice Correlated System using 10-fs Pulse
The Initial Process of Photoinduced Phase Transition in an Organic Electron-Lattice Correlated System using 1-fs Pulse S. Koshihara, K. Onda, Y. Matsubara, T. Ishikawa, Y. Okimoto, T. Hiramatsu, G. Saito,
More informationPart II Course Content. Outline Lecture 9. Frequency Correlations & Lineshapes. Nonlinear Spectroscopic Methods
Part II Course Content Outline Lecture 9 Optical Bloch equations Nonlinear polarizations in matter: the perturbative expansion approach. Ultrafast Fourier-transform spectroscopy: two and more dimensions.
More informationattosecond laser pulse
Kenichi Ishikawa ( ) http://ishiken.free.fr/english/lecture.html ishiken@atto.t.u-tokyo.ac.jp Advanced Plasma and Laser Science E attosecond laser pulse 1 attosecond pulse train (APT) isolated attosecond
More informationSLAC National Accelerator Laboratory. Persis S. Drell Director August 30, 2010
SLAC National Accelerator Laboratory Persis S. Drell Director August 30, 2010 SLAC Mission Explore the ultimate structure and dynamics of matter in the domains of energy, space and time at the smallest
More informationImplementation and evaluation of data analysis strategies for time-resolved optical spectroscopy
Supporting information Implementation and evaluation of data analysis strategies for time-resolved optical spectroscopy Chavdar Slavov, Helvi Hartmann, Josef Wachtveitl Institute of Physical and Theoretical
More informationXRD 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 informationOverview: Attosecond optical technology based on recollision and gating
Overview: Attosecond optical technology based on recollision and gating Zenghu Chang Kansas State University Team members Kansas State University Zenghu Chang (Dept. of Phys.) Lew Cocke (Dept. of Phys.)
More informationBrightness 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 informationQuantum Condensed Matter Physics Lecture 9
Quantum Condensed Matter Physics Lecture 9 David Ritchie QCMP Lent/Easter 2018 http://www.sp.phy.cam.ac.uk/drp2/home 9.1 Quantum Condensed Matter Physics 1. Classical and Semi-classical models for electrons
More informationFEL WG: Summary. SLAC National Accelerator Lab. Kwang-Je Kim (Part I, Mo-Tu) Joe Bisognano (Part II, Th) Future Light Source WS 2010: FEL WG
FEL WG: Summary Kwang-Je Kim (Part I, Mo-Tu) Joe Bisognano (Part II, Th) Future Light Source WS 2010: FEL WG March 1-5, 2010 SLAC National Accelerator Lab Menlo Park, CA The submitted manuscript has been
More informationUltrafast Electron-Electron Dynamics in Graphene Daniele Brida
Ultrafast Electron-Electron Dynamics in Graphene Ultrafast Spectroscopy Light-matter interaction on timescale of fundamental physical processes: electron scattering, phonon emission, energy transfer D.
More informationThe Second Half Year 2017 PAL-XFEL Call for Proposals
The Second Half Year 2017 PAL-XFEL Call for Proposals Summary Information for Submitting Proposals We encourage scientists from all over the world to submit applications for beam time proposal to utilize
More informationIntroduction to X-ray Absorption Near Edge Spectroscopy (XANES) Ritimukta Sarangi SSRL, SLAC Stanford University June 28, 2010
Introduction to X-ray Absorption Near Edge Spectroscopy (XANES) Ritimukta Sarangi SSRL, SLAC Stanford University June 28, 2010 Basics of X-ray Absorption Spectroscopy (XAS) An edge results when a core
More informationDetermination of the hyperfine parameters of iron in aluminous (Mg,Fe)SiO 3 perovskite
Determination of the hyperfine parameters of iron in aluminous (Mg,Fe)SiO 3 perovskite Jennifer M. Jackson Seismological Laboratory, Geological & Planetary Sciences California Institute of Technology VLab
More informationTechnology, Techniques and Applications. Ric Allott Business Development Manager
Technology, Techniques and Applications Ric Allott Business Development Manager 1 Central Laser Facility ASTRA GEMINI VULCAN ARTEMIS ULTRA OCTOPUS High power, ultrashort pulse dual beams of 15 J, 30 fs
More informationSmall 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 informationTime-resolved x-ray absorption spectroscopy: Watching atoms dance
Time-resolved x-ray absorption spectroscopy: Watching atoms dance Chris J. Milne 1, Van-Thai Pham 1, Wojciech Gawelda 3, Renske M. van der Veen 1,2, Amal El Nahhas 1, Steven L. Johnson 2, Paul Beaud 2,
More informationInitial Hydrogen-Bonding Dynamics of. Photoexcited Coumarin in Solution with. Femtosecond Stimulated Raman Spectroscopy
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2015 Electronic Supplementary Information (ESI) for: Initial Hydrogen-Bonding
More informationSupporting information for the manuscript. Excited state structural evolution during charge-transfer reactions in Betaine-30
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2015 Supporting information for the manuscript Excited state structural evolution during
More informationSurvey on Laser Spectroscopic Techniques for Condensed Matter
Survey on Laser Spectroscopic Techniques for Condensed Matter Coherent Radiation Sources for Small Laboratories CW: Tunability: IR Visible Linewidth: 1 Hz Power: μw 10W Pulsed: Tunabality: THz Soft X-ray
More informationThe Use of Synchrotron Radiation in Modern Research
The Use of Synchrotron Radiation in Modern Research Physics Chemistry Structural Biology Materials Science Geochemical and Environmental Science Atoms, molecules, liquids, solids. Electronic and geometric
More informationCoherent Nonlinear Spectroscopy: From Femtosecond Dynamics to Control
Coherent Nonlinear Spectroscopy: From Femtosecond Dynamics to Control Annu.rev.phys.chem., 52, 639 Marcos dantus ⅠIntroduction 1. History of breaking time resolution limit mid 1950 ; microsecond time resolution.
More informationLaser-driven X-ray sources: realization and future trends
Laser-driven X-ray sources: realization and future trends Patrick Audebert, Julien Gautier, Fabien Quéré, Rodrigo Lopez-Martens, Le Thi Thu Thuy, Philippe Martin, Hamed Merdji, Pascal Monot, Eduardo Oliva,
More information