Hirohito Ogasawara, Dennis Nordlund, Anders Nilsson

Size: px
Start display at page:

Download "Hirohito Ogasawara, Dennis Nordlund, Anders Nilsson"

Transcription

1 Pump-probe Ultrafast Surface Chemistry (PES, XES) station for Real Time Electronic Structure Mapping of Catalytic Reactions: Instrumentation Hirohito Ogasawara, Dennis Nordlund, Anders Nilsson Stanford Synchrotron Radiation Lightsource (SSRL) & Stanford Institute for Materials & Energy Science (SIMES) SSRL LCLS?

2 Catalytic reactions on surfaces are used for Conversion of chemicals N 2 + H 2 NH 3 NH 3 + O 2 HNO 3 CO + H 2 O CO 2 + H 2 R-CO-R, R-CHO RCHOH CO, HC, NO x N 2, H 2 O, CO 2 etc Clean fuel H 2 O, electricity H 2, O 2 H + + O 2 H 2 O, electricity etc On the surface catalyst, reactions occur efficiently and selectively.

3 Catalsyt surface provides a mechanism to lower the activation energy activation barrier Gibbs free energy reactant H + + O 2 product H O 2

4 Catalsyt surface provides a mechanism to lower the activation energy Gibbs free energy reactant H + + O 2 Pt catalyst product O, electricity H 2

5 Catalsyt surface provides a mechanism to lower the activation energy Gibbs free energy reactant H + + O 2 Pt catalyst product O, electricity H 2 Catalyst can perform the reaction faster or at lower temperatures Catalyst can perform the reaction selectively

6 Catalyt surface provides a mechanism to lower the activation energy Gibbs free energy reactant H + + O 2 bad catalyst Harmful to the fuel cell assembly H 2 O 2 H 2 product O, electricity Catalyst can perform the reaction efficiently Catalyst can perform the reaction selectively

7 SXR: Observe the surface reaction mechanism in the time domain Understand the origin of catalytic efficiency and selectivity dissociation adsorption hydrogenation desorption Laser temperature jump Photodissociation X-ray emission (XES) Photoemission (PES)

8 Plan under the SXR consortium FY2009 Customize the XES/PES endstation at BL 13-2 new sample holder, new manipulator, remote operation, DAQ, valve position sensors, pump interlocks Test this complete setup at SSRL BL13-2 FY2010 Ready for first experiments. After first experiments: Design a complete new instrument, dedicated for SXR in-situ study, THz pump etc 2011 Static study at SSRL Ultrafast study at LCLS

9 PES/XES station at BL13-2 X-ray emission spectrometer XES beam photoemission spectrometer Requirements: Power 1 x 208V, 30A, 3-phase or 3 x 115V, 30A, 2-phase Ducting for pump exhaust Pressurized air line Nitrogen line PES

10 PES/XES station at BL13-2 X-ray emission spectrometer This part is mainly used at LCLS XES beam photoemission spectrometer Requirements: Power 1 x 208V, 30A, 3-phase or 3 x 115V, 30A, 2-phase Ducting for pump exhaust Pressurized air line Nitrogen line PES

11 PES/XES station for SXR Sample manipulator XES elliptically shaped grating LCLS DAQ digital camera beam beam PES VG-Scienta R3000 LCLS DAQ digital camera Side view Lens acceptance: +/- 15 degrees Energy window(single-shot): 24 ev, 12% of E pass Top view

12 PES and XES performance molecular oxygen heat atomic oxygen O1s XPS taken during Temperature ramp time per spectrum = 7 sec at SSRL BL13-2 Analyzer: Scienta SES-100 (+ digital camera, ~50fps) Photon Flux: ~10 11 photons/sec Lens acceptance: +/- 6 degrees New analyzer was installed in Sep 2008 Lens acceptance: +/- 15 degrees Energy window(single-shot): 24 ev Plan to install 120fps digital camera VG-Scienta R3000

13 PES and XES performance C, N and O Kedges Illumination selector Revolver place for 3 gratings Elliptical grating: L=10 cm Ni coating: less grazing incidenc Sample X,Y stage Grating Selector rotation+lock Under commission at BL13 2 MCP + digital camera Incidence angle

14 PES/XES station for SXR Sample manipulator Preparation level beam Spectroscopy level 10 mm Side view

15 PES/XES station for SXR When the sample is at the preparation level.. Gas doser Users can operate the Ne sputter gun, the EB heating system (up to 1100 K) and the gas doser to prepare sample. Preparation levelsputter gun Users can operate the gas line system to adjust the pressure.

16 PES/XES station for SXR When the sample is at the spectroscopy level.. If FEL beam is used in the hatch 2, users may not enter the hatch 2. The gas doser can be operated remotely. A filament for radiative heating can be controlled remotely. XES power supply can be turn on and off remotely. Spectroscopy level PES power supply can be controlled remotely. beam Gas doser Pulsed gas beam is delivered. Pulse width: ~300 microseconds, Repetition rate ~250 Hz

17 PES/XES station for SXR Beam position monitor? Beam dump TV cameras The position of reflected soft x-ray beam may be monitored. Side view Top view (PES) Top view (XES)

18 - Grazing incidence e 1 deg. reflectivity [%] X-ray interaction with matter calculator deg. 80 Ni 60 5 deg. Cu Photon Energy [ev] e- e- 5 deg. Advantage: large foot print on the sample: 2 mm x 10 micron less power density reflectivity [%] X-ray interaction with matter calculator deg. 40 Ni Cu Photon Energy [ev] angle of incidence <0.5 degree gives, reflectivity: >90% attenuation length: ~5 atomic layers, less photoionization of bulk atoms

19 Scan the sample to avoid X-ray irradiation induced damages Each FEL pulse hits a fresh spot SSRL BL13-2 Without scanning, the sample is seriously damaged! LCLS One shot seriously damages the sample. SSRL LCLS Scanning is necessary: 10 micron/sec SSRL Scanning is necessary: 10 micron/shot =1 mm/sec. LCLS Sample scan bea m

20 PES and XES count rate: SSRL and LCLS SSRL BL13-2: PES: a few sec accumulation (~10 11 photons/sec) XES: ~1000 sec accumulation (~10 12 photons/sec) LCLS SXR: same amount of photons/pulse PES: one-shot XES: ~10 sec accumulation

21 First experiments Ultrafast temperature jump Hot Oxygen Atom Hot Nitrogen Atom NIR laser: 780nm, short pulse width, small spot size: 10micron hot atom Photodissociation Dissociation of O 2 Dissociation of NO UV laser: 260nm, short pulse width, small spot size: 10 micron * *

22 Pump-probe Ultrafast Surface Chemistry Station: Understand the origin of catalytic efficiency and selectivity Main Point of Contact for the Project: Anders Nillsson Point of Contact for the Instrumentation: Dennis Nordlund Hirohito Ogasawara SSRL LCLS reactant(ads) product(ads)? intermediates(ads) intermediates(ads) reactant(ads) product(ads) Time [fs]

Pump-Probe Surface Chemistry at LCLS

Pump-Probe Surface Chemistry at LCLS Pump-Probe Surface Chemistry at LCLS Anders Nilsson Stanford Synchrotron Radiation Laboratory Alan Luntz, Palo Alto, previous IBM Alec Wodtke, University of California, Santa Barbara Tony Heinz, Columbia

More information

X-Ray Emission Spectrometer Design with Single-Shot. Pump-Probe and Resonant Excitation Capabilities. Katherine Spoth

X-Ray Emission Spectrometer Design with Single-Shot. Pump-Probe and Resonant Excitation Capabilities. Katherine Spoth X-Ray Emission Spectrometer Design with Single-Shot Pump-Probe and Resonant Excitation Capabilities Katherine Spoth Office of Science, Science Undergraduate Laboratory Internship (SULI) State University

More information

Ultrafast Single-Shot X-Ray Emission Spectrometer Design. Katherine Spoth

Ultrafast Single-Shot X-Ray Emission Spectrometer Design. Katherine Spoth Ultrafast Single-Shot X-Ray Emission Spectrometer Design Katherine Spoth O ce of Science, Science Undergraduate Laboratory Internship (SULI) State University of New York at Bu alo SLAC National Accelerator

More information

Probing Matter: Diffraction, Spectroscopy and Photoemission

Probing 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 information

NanoEngineering of Hybrid Carbon Nanotube Metal Composite Materials for Hydrogen Storage Anders Nilsson

NanoEngineering of Hybrid Carbon Nanotube Metal Composite Materials for Hydrogen Storage Anders Nilsson NanoEngineering of Hybrid Carbon Nanotube Metal Composite Materials for Hydrogen Storage Anders Nilsson Stanford Synchrotron Radiation Laboratory (SSRL) and Stockholm University Coworkers and Ackowledgement

More information

Hydrogenation of Single Walled Carbon Nanotubes

Hydrogenation of Single Walled Carbon Nanotubes Hydrogenation of Single Walled Carbon Nanotubes Anders Nilsson Stanford Synchrotron Radiation Laboratory (SSRL) and Stockholm University Coworkers and Ackowledgement A. Nikitin 1), H. Ogasawara 1), D.

More information

A facility for Femtosecond Soft X-Ray Imaging on the Nanoscale

A 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 information

Supporting Information s for

Supporting Information s for Supporting Information s for # Self-assembling of DNA-templated Au Nanoparticles into Nanowires and their enhanced SERS and Catalytic Applications Subrata Kundu* and M. Jayachandran Electrochemical Materials

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

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

Photoemission Spectroscopy

Photoemission Spectroscopy FY13 Experimental Physics - Auger Electron Spectroscopy Photoemission Spectroscopy Supervisor: Per Morgen SDU, Institute of Physics Campusvej 55 DK - 5250 Odense S Ulrik Robenhagen,

More information

Workshop 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 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 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

X-Ray Spectro-Microscopy Joachim Stöhr Stanford Synchrotron Radiation Laboratory

X-Ray Spectro-Microscopy Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Ray Spectro-Microscopy Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Rays have come a long way Application to Magnetic Systems 1 µm 1895 1993 2003 http://www-ssrl.slac.stanford.edu/stohr/index.htm

More information

X-TOD Update. Facility Advisory Committee Photon Breakout Session. October 30, 2007

X-TOD Update. Facility Advisory Committee Photon Breakout Session. October 30, 2007 XTOD Update Facility Advisory Committee Photon Breakout Session LCLS Layout Linac Undulator Hall FEE (Front-End-Enclosure) Diagnostics SOMS HOMS X-Ray Tunnel FEH (Far Experimental Hall) NEH (Near Experimental

More information

The first two years of TES spectrometer at SSRL

The first two years of TES spectrometer at SSRL The first two years of TES spectrometer at SSRL Developing the TES spectrometer for cutting-edge science Sang Jun Lee SLAC National Accelerator Laboratory SSRL Acknowledgement SLAC/Stanford Mike Baker

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

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

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

SLS Symposium on X-Ray Instrumentation

SLS Symposium on X-Ray Instrumentation SLS Symposium on X-Ray Instrumentation Tuesday, December 7, 2010 10:00 to 12:15, WBGB/019 10:00 The optics layout of the PEARL beamline P. Oberta, U. Flechsig and M. Muntwiler 10:30 Instrumentation for

More information

Lecture 5. X-ray Photoemission Spectroscopy (XPS)

Lecture 5. X-ray Photoemission Spectroscopy (XPS) Lecture 5 X-ray Photoemission Spectroscopy (XPS) 5. Photoemission Spectroscopy (XPS) 5. Principles 5.2 Interpretation 5.3 Instrumentation 5.4 XPS vs UV Photoelectron Spectroscopy (UPS) 5.5 Auger Electron

More information

Technical description of photoelectron spectrometer Escalab 250Xi

Technical description of photoelectron spectrometer Escalab 250Xi Technical description of photoelectron spectrometer Escalab 250Xi Resource center Physical Methods of Surface Investigations 2014 Table of contents Common description 3 Analytical chamber 8 Preparation

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

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

Surface Chemistry and Reaction Dynamics of Electron Beam Induced Deposition Processes

Surface Chemistry and Reaction Dynamics of Electron Beam Induced Deposition Processes Surface Chemistry and Reaction Dynamics of Electron Beam Induced Deposition Processes e -? 2 nd FEBIP Workshop Thun, Switzerland 2008 Howard Fairbrother Johns Hopkins University Baltimore, MD, USA Outline

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

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

Results on a-c tubes subjected to synchrotron irradiation

Results on a-c tubes subjected to synchrotron irradiation Results on a-c tubes subjected to synchrotron irradiation V. Baglin, P. Chiggiato, P. Costa-Pinto, B. Henrist (CERN, Geneva) V. Anashin, D. Dorokhov. A. Semenov, A. Krasnov, D. Shwartz, A. Senchenko (,

More information

SOFT X-RAY MATERIAL INSTRUMENT (SXR)

SOFT X-RAY MATERIAL INSTRUMENT (SXR) SOFT X--RAY MATERIAL INSTRUMENT ((SXR)) SUMMARY OF THE TECHNICAL DESIGN DRAFT 3-3-09 This document is derived from the SXR Technical Design Report, July 2008, prepared for the LCLS by the SXR consortium.

More information

A Review of X-Ray Free Electron Laser Oscillator

A Review of X-Ray Free Electron Laser Oscillator A Review of X-Ray Free Electron Laser Oscillator ERL 2011 Kwang-Je Kim Argonne National Laboratory October 16-21, 2011 KEK Tsukuba Japan FEL Works for Hard X-rays! Self Amplified Spontaneous Emission (SASE)

More information

Generation and characterization of ultra-short electron and x-ray x pulses

Generation and characterization of ultra-short electron and x-ray x pulses Generation and characterization of ultra-short electron and x-ray x pulses Zhirong Huang (SLAC) Compact XFEL workshop July 19-20, 2010, Shanghai, China Ultra-bright Promise of XFELs Ultra-fast LCLS Methods

More information

An Adventure in Marrying Laser Arts and Accelerator Technologies

An Adventure in Marrying Laser Arts and Accelerator Technologies An Adventure in Marrying Laser Arts and Accelerator Technologies Dao Xiang Beam Physics Dept, SLAC, Stanford University Feb-28-2012 An example sample Probe (electron) Pump (laser) Typical pump-probe experiment

More information

Breakout Session Deliverables

Breakout Session Deliverables Workshop Charge Identify most important science drivers (transformational, grand challenge level) that can uniquely be addressed using capabilities of LCLS-II (high rep rate

More information

TPD-MS. Photocatalytic Studies Using Temperature Programmed Desorption Mass Spectrometry (TPD-MS) APPLICATION NOTE NOTE

TPD-MS. Photocatalytic Studies Using Temperature Programmed Desorption Mass Spectrometry (TPD-MS) APPLICATION NOTE NOTE TPD-MS APPLICATION NOTE NOTE Photocatalytic Studies Using Temperature Programmed Desorption Mass Spectrometry (TPD-MS) Thermal analysis consists of many techniques for the exploration of the physical properties

More information

Making Functional Surfaces and Thin Films: Where are the Atoms?

Making Functional Surfaces and Thin Films: Where are the Atoms? Making Functional Surfaces and Thin Films: Where are the Atoms? K. Ludwig, A. DeMasi, J. Davis and G. Erdem Department of Physics Materials Science and Engineering Program Why x-rays? λ ~10-10 m ~ distance

More information

X-Ray Spectroscopy at LCLS

X-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 information

Cover Page. The handle holds various files of this Leiden University dissertation.

Cover Page. The handle   holds various files of this Leiden University dissertation. Cover Page The handle http://hdl.handle.net/1887/44295 holds various files of this Leiden University dissertation. Author: Badan, C. Title: Surface-structure dependence of water-related adsorbates on platinum

More information

X-Ray Photoelectron Spectroscopy (XPS)

X-Ray Photoelectron Spectroscopy (XPS) X-Ray Photoelectron Spectroscopy (XPS) Louis Scudiero http://www.wsu.edu/~scudiero; 5-2669 Fulmer 261A Electron Spectroscopy for Chemical Analysis (ESCA) The basic principle of the photoelectric effect

More information

Performance 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 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 information

Modern Methods in Heterogeneous Catalysis Research

Modern Methods in Heterogeneous Catalysis Research Modern Methods in Heterogeneous Catalysis Research Axel Knop-Gericke, January 09, 2004 In situ X-ray photoelectron spectroscopy (XPS) In situ near edge X-ray absorption fine structure (NEXAFS) in the soft

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

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

Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems

Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems Wei-Sheng Lee Stanford Institute of Material and Energy Science (SIMES) SLAC & Stanford University Collaborators

More information

New advances in folded pathlength technology for Process Tunable Diode Laser Absorption Spectrometers (TDLAS)

New advances in folded pathlength technology for Process Tunable Diode Laser Absorption Spectrometers (TDLAS) New advances in folded pathlength technology for Process Tunable Diode Laser Absorption Spectrometers (TDLAS) Jean-Nicolas Adami, PhD Head of Strategic Product Group Gas Analytics Mettler-Toledo GmbH,

More information

Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL

Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL R. Kuroda, H. Ogawa, N. Sei, H. Toyokawa, K. Yagi-Watanabe, M. Yasumoto, M. Koike, K. Yamada, T. Yanagida*, T. Nakajyo*, F. Sakai*

More information

Supporting Information

Supporting Information Supporting Information Three-dimensional frameworks of cubic (NH 4 ) 5 Ga 4 SbS 10, (NH 4 ) 4 Ga 4 SbS 9 (OH) H 2 O, and (NH 4 ) 3 Ga 4 SbS 9 (OH 2 ) 2H 2 O. Joshua L. Mertz, Nan Ding, and Mercouri G.

More information

A DIVISION OF ULVAC-PHI

A DIVISION OF ULVAC-PHI A DIVISION OF ULVAC-PHI X-ray photoelectron spectroscopy (XPS/ESCA) is the most widely used surface analysis technique and has many well established industrial and research applications. XPS provides

More information

MODERN TECHNIQUES OF SURFACE SCIENCE

MODERN TECHNIQUES OF SURFACE SCIENCE MODERN TECHNIQUES OF SURFACE SCIENCE Second edition D. P. WOODRUFF & T. A. DELCHAR Department ofphysics, University of Warwick CAMBRIDGE UNIVERSITY PRESS Contents Preface to first edition Preface to second

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

Check the LCLS Project website to verify 2 of 6 that this is the correct version prior to use.

Check the LCLS Project website to verify 2 of 6 that this is the correct version prior to use. 1. Introduction The XTOD Offset Systems are designed to spatially separate the useful FEL radiation from high-energy spontaneous radiation and Bremsstrahlung γ-rays. These unwanted radiations are generated

More information

RF Gun Photo-Emission Model for Metal Cathodes Including Time Dependent Emission

RF Gun Photo-Emission Model for Metal Cathodes Including Time Dependent Emission RF Gun Photo-Emission Model for Metal Cathodes Including Time Dependent Emission SLAC-PUB-117 February 6 (A) J. F. SCHMERGE, J. E. CLENDENIN, D. H. DOWELL, AND S. M. GIERMAN SLAC, Stanford University,

More information

1 EX/P4-8. Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device

1 EX/P4-8. Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device 1 EX/P4-8 Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device T. Hino 1,2), T. Hirata 1), N. Ashikawa 2), S. Masuzaki 2), Y. Yamauchi

More information

Progress Report on the LCLS XFEL at SLAC

Progress Report on the LCLS XFEL at SLAC Progress Report on the LCLS XFEL at SLAC L F DiMauro 1, J Arthur 2, N Berrah 3, J Bozek 2, J N Galayda 2 and J Hastings 2 1 The Ohio State University, Department of Physics, Columbus, OH 43210 USA 2 Stanford

More information

Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging

Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging U. Manju, M. Sreemony and A. K. Chakraborty In this note we present the new multipurpose photoelectron spectroscopy facility

More information

Spectroscopy with Free Electron Lasers. David Bernstein SASS Talk January 28 th, 2009

Spectroscopy with Free Electron Lasers. David Bernstein SASS Talk January 28 th, 2009 Spectroscopy with Free Electron Lasers David Bernstein SASS Talk January 28 th, 2009 Overview Who am I?! What is FLASH?! The promise of Free Electron Lasers (FELs) The Trouble with Spectroscopy Sample

More information

Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis

Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis Dmitry Zemlyanov Birck Nanotechnology Center, Purdue University Outline Introduction

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

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

Development of Soft X-rayX using Laser Compton Scattering

Development of Soft X-rayX using Laser Compton Scattering 26 th Advanced ICFA Beam Dynamics Workshop on Nanometre-Size Colliding Beams September 2-6, 2002 at Lausanne Development of Soft X-rayX Source using Laser Compton Scattering R. Kuroda*, S. Kashiwagi*,

More information

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7 Advanced Lab Course X-Ray Photoelectron Spectroscopy M210 As of: 2015-04-01 Aim: Chemical analysis of surfaces. Content 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT 3 3.1 Qualitative analysis 6 3.2 Chemical

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

Characterization of Secondary Emission Materials for Micro-Channel Plates. S. Jokela, I. Veryovkin, A. Zinovev

Characterization of Secondary Emission Materials for Micro-Channel Plates. S. Jokela, I. Veryovkin, A. Zinovev Characterization of Secondary Emission Materials for Micro-Channel Plates S. Jokela, I. Veryovkin, A. Zinovev Secondary Electron Yield Testing Technique We have incorporated XPS, UPS, Ar-ion sputtering,

More information

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960 Introduction to X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS), also known as Electron Spectroscopy for Chemical Analysis (ESCA) is a widely used technique to investigate

More information

Thermo Scientific K-Alpha + XPS Spectrometer. Fast, powerful and accessible chemical analysis for surface and thin film characterization

Thermo Scientific K-Alpha + XPS Spectrometer. Fast, powerful and accessible chemical analysis for surface and thin film characterization Thermo Scientific K-Alpha + XPS Spectrometer Fast, powerful and accessible chemical analysis for surface and thin film characterization X-ray Photoelectron Spectroscopy Quantitative, chemical identification

More information

Supporting Information. Effect of Backbone Chemistry on the Structure of Polyurea Films Deposited by Molecular Layer Deposition

Supporting Information. Effect of Backbone Chemistry on the Structure of Polyurea Films Deposited by Molecular Layer Deposition Supporting Information Effect of Backbone Chemistry on the Structure of Polyurea Films Deposited by Molecular Layer Deposition David S. Bergsman, Richard G. Closser, Christopher J. Tassone, Bruce M. Clemens

More information

Lecture 22 Ion Beam Techniques

Lecture 22 Ion Beam Techniques Lecture 22 Ion Beam Techniques Schroder: Chapter 11.3 1/44 Announcements Homework 6/6: Will be online on later today. Due Wednesday June 6th at 10:00am. I will return it at the final exam (14 th June).

More information

Size-selected Metal Cluster Deposition on Oxide Surfaces: Impact Dynamics and Supported Cluster Chemistry

Size-selected Metal Cluster Deposition on Oxide Surfaces: Impact Dynamics and Supported Cluster Chemistry Size-selected Metal Cluster Deposition on Oxide Surfaces: Impact Dynamics and Supported Cluster Chemistry Sungsik Lee, Masato Aizawa, Chaoyang Fan, Tianpin Wu, and Scott L. Anderson Support: AFOSR, DOE

More information

Set-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 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 information

UV Source Series. UVS 10/35 gas discharge, UVS 300 duoplasmatron. Key Features

UV Source Series. UVS 10/35 gas discharge, UVS 300 duoplasmatron. Key Features UV Source Series UVS 10/35 gas discharge, UVS 300 duoplasmatron and UVLS microwave source for UPS and arpes Key Features Ultimate intensity and stability UV sources Ease of operation Variable excitation

More information

SPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS

SPPS: 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 information

Electron Spectroscopy

Electron Spectroscopy Electron Spectroscopy Photoelectron spectroscopy is based upon a single photon in/electron out process. The energy of a photon is given by the Einstein relation : E = h ν where h - Planck constant ( 6.62

More information

Methods of surface analysis

Methods of surface analysis Methods of surface analysis Nanomaterials characterisation I RNDr. Věra Vodičková, PhD. Surface of solid matter: last monoatomic layer + absorbed monolayer physical properties are effected (crystal lattice

More information

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS Name of contact person: Surender Kumar Sharma Name of other contributors: R.

More information

Stanford Synchrotron Radiation Lightsource SSRL

Stanford Synchrotron Radiation Lightsource SSRL Stanford Synchrotron Radiation Lightsource SSRL x Chi-Chang Kao BL1-4 BL1-5 BL2-1 BL2-2 BL2-3 BL4-1 BL4-2 BL4-3 BL5-4 BL6-2(3) BL7-1 BL7-2 BL7-3 BL8-1 BL8-2 BL9-1 BL9-2 BL9-3 BL10-1 BL10-2(2) BL11-1 BL11-2

More information

Applications of Micro-Area Analysis Used by JPS-9200 X-ray Photoelectron Spectrometer

Applications of Micro-Area Analysis Used by JPS-9200 X-ray Photoelectron Spectrometer Applications of Micro-Area Analysis Used by JPS-9200 X-ray Photoelectron Spectrometer Yoshitoki Iijima Application & Research Center, JEOL Ltd. Introduction Recently, with advances in the development of

More information

LIBSlab ANALYZERS ANALYZERS

LIBSlab ANALYZERS ANALYZERS ANALYZERS ANALYZERS Chemical multi-elemental analysis with LIBS in modular benchtop design LIBSlab LIBSpector compact sample chamber for the LIBS analysis of solid, liquid and gaseous samples. Sample chamber

More information

Catalysis CAPABILITIES

Catalysis   CAPABILITIES Catalysis www.extrel.com CAPABILITIES Contents Extrel instruments have been recognized for their exceptional performance by the world s leading researchers for more than 50 years. Reliability and flexibility

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

The Use of Synchrotron Radiation in Modern Research

The 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 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

Abstract. PEGASUS Toroidal Experiment University of Wisconsin-Madison

Abstract. PEGASUS Toroidal Experiment University of Wisconsin-Madison Abstract Measurement capabilities for the Pegasus ST are increasing to support the scientific studies of plasma behavior at very-low A. Global parameters are obtained from equilibrium reconstructions constrained

More information

Spectroscopy of Nanostructures. Angle-resolved Photoemission (ARPES, UPS)

Spectroscopy 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 information

Undulator radiation from electrons randomly distributed in a bunch

Undulator radiation from electrons randomly distributed in a bunch Undulator radiation from electrons randomly distributed in a bunch Normally z el >> N u 1 Chaotic light Spectral property is the same as that of a single electron /=1/N u Temporal phase space area z ~(/

More information

X-Ray Diagnostics Commissioning at the LCLS

X-Ray Diagnostics Commissioning at the LCLS X-Ray Diagnostics Commissioning at the LCLS - Selected Studies - J. Welch, SLAC National Accelerator Laboratory Aug. 3-27, 2010 Commissioning Studies Microbunching Instability Laser Heater tune-up Gas

More information

Supplementary Materials

Supplementary Materials Atomic layer-deposited tunnel oxide stabilizes silicon photoanodes for water oxidation Yi Wei Chen 1, Jonathan D. Prange 2, Simon Dühnen 2, Yohan Park 1, Marika Gunji 1, Christopher E. D. Chidsey 2, and

More information

The Second Half Year 2017 PAL-XFEL Call for Proposals

The 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 information

High quality beam generation and its application at Waseda University

High quality beam generation and its application at Waseda University High quality beam generation and its application at Waseda University Shigeru Kashiwagi, Yoshimasa Hama, Hiroki Ishikawa, Ryunosuke Kuroda, Takashi Oshima, Masakazu Washio, Akira Yada Advanced Rsearch

More information

XPS/UPS and EFM. Brent Gila. XPS/UPS Ryan Davies EFM Andy Gerger

XPS/UPS and EFM. Brent Gila. XPS/UPS Ryan Davies EFM Andy Gerger XPS/UPS and EFM Brent Gila XPS/UPS Ryan Davies EFM Andy Gerger XPS/ESCA X-ray photoelectron spectroscopy (XPS) also called Electron Spectroscopy for Chemical Analysis (ESCA) is a chemical surface analysis

More information

X-ray Photoelectron Spectroscopy (XPS)

X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS) As part of the course Characterization of Catalysts and Surfaces Prof. Dr. Markus Ammann Paul Scherrer Institut markus.ammann@psi.ch Resource for further reading:

More information

Photoemission Electron Microscopy (PEEM)

Photoemission Electron Microscopy (PEEM) PHOTOEMISSION ELECTRON MICROSCOPY Pat Photongkam Research Facility Division Synchrotron Light Research Institute (Public Organization) Synchrotron Light Research Institute (Public Organization) 111 University

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

Construction of an extreme ultraviolet polarimeter based on highorder harmonic generation

Construction of an extreme ultraviolet polarimeter based on highorder harmonic generation Construction of an extreme ultraviolet polarimeter based on highorder harmonic generation N. Brimhall *, J. C. Painter, M. Turner, S. V. Voronov, R. S. Turley, M. Ware, and J. Peatross Department of Physics

More information

ATHENA / AD-1. First production and detection of cold antihydrogen atoms. ATHENA Collaboration. Rolf Landua CERN

ATHENA / AD-1. First production and detection of cold antihydrogen atoms. ATHENA Collaboration. Rolf Landua CERN ATHENA / AD-1 First production and detection of cold antihydrogen atoms ATHENA Collaboration Rolf Landua CERN 1 LONG TERM PHYSICS GOALS Antihydrogen = Hydrogen? CPT Gravity But... 2 FIRST GOAL PRODUCTION

More information

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu X-ray Photoelectron Spectroscopy Introduction Qualitative analysis Quantitative analysis Charging compensation Small area analysis and XPS imaging

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

PHYS 4400, Principles and Varieties of Solar Energy Instructor: Randy J. Ellingson The University of Toledo

PHYS 4400, Principles and Varieties of Solar Energy Instructor: Randy J. Ellingson The University of Toledo Light and Photons PHYS 4400, Principles and Varieties of Solar Energy Instructor: Randy J. Ellingson The University of Toledo January 16, 2014 Light What is light? Electromagnetic wave direction of the

More information

Table 1: Residence time (τ) in seconds for adsorbed molecules

Table 1: Residence time (τ) in seconds for adsorbed molecules 1 Surfaces We got our first hint of the importance of surface processes in the mass spectrum of a high vacuum environment. The spectrum was dominated by water and carbon monoxide, species that represent

More information

Richard 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 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 information

X-ray Fluorescence Imaging Following Synchrotron Beam Excitation

X-ray Fluorescence Imaging Following Synchrotron Beam Excitation Conference on Applied Digital Imaging Techniques for Understanding the Palimpsest X-ray Fluorescence Imaging Following Synchrotron Beam Excitation Uwe Bergmann Stanford Synchrotron Radiation Laboratory

More information

Review of the doctoral dissertation of Ismail Saber titled: Spectral investigation of extreme ultraviolet induced plasmas

Review of the doctoral dissertation of Ismail Saber titled: Spectral investigation of extreme ultraviolet induced plasmas Prof. dr hab. inż. Tadeusz Pisarczyk Institute of Plasma Physics and Laser Microfusion. 23 Hery St., 01-489 Warsaw. Warsaw, November 21, 2018r. Introduction: Review of the doctoral dissertation of Ismail

More information