MeV electron diffraction and microscopy

Similar documents
Jinfeng Yang. Osaka University, Japan

Single-shot Ultrafast Electron Microscopy

High gradient, high average power structure development at UCLA and Univ. Rome in X-X. band

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

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

Diagnostic Systems for High Brightness Electron Injectors

Development of Soft X-rayX using Laser Compton Scattering

Time Resolved (Pump Probe) Experiment to watch structural dynamics by using the pulsed nature of synchrotron radiation

New Electron Source for Energy Recovery Linacs

The New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun

Start-to-End Simulations

AREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts

Simulations of the IR/THz source at PITZ (SASE FEL and CTR)

SPARCLAB. Source For Plasma Accelerators and Radiation Compton with Laser And Beam

Experimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem

Pushing the limits of laser synchrotron light sources

Dark Current at Injector. Jang-Hui Han 27 November 2006 XFEL Beam Dynamics Meeting

AREAL. Test Facility for Advanced Accelerator and Radiation Sources Concepts. Part.1 Introduction. V. Tsakanov CANDLE SRI

THz Electron Gun Development. Emilio Nanni 3/30/2016

Time resolved transverse and longitudinal phase space measurements at the high brightness photo injector PITZ

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

Considerations of an Ultrafast Electron Diffraction experiment at

Toward a high quality MeV electron source from a wakefield accelerator for ultrafast electron diffraction

Recent Status of Polarized Electron Sources at Nagoya University

Linac optimisation for the New Light Source

Modeling of the secondary electron emission in rf photocathode guns

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

The VELA and CLARA Test Facilities at Daresbury Laboratory Peter McIntosh, STFC on behalf of the VELA and CLARA Development Teams

Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ

Coulomb crystal extraction from an ion trap for application to nano-beam source"

Ultrafast nanophotonics - optical control of coherent electron -

MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES

LCLS Injector Prototyping at the GTF

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

High brightness beam science

Research Laboratory for Quantum Beam Science

Weak-Beam Dark-Field Technique

The CeB6 Electron Gun for the Soft-X-ray FEL Project at SPring-8

object objective lens eyepiece lens

SCSS Prototype Accelerator -- Its outline and achieved beam performance --

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

Two-Stage Chirped-Beam SASE-FEL for High Power Femtosecond X-Ray Pulse Generation

Ultrashort electron source from laser-plasma interaction

Introduction. Thermoionic gun vs RF photo gun Magnetic compression vs Velocity bunching. Probe beam design options

SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE*

SPARCLAB. Source For Plasma Accelerators and Radiation Compton. On behalf of SPARCLAB collaboration

Set-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source

Laser-driven intense X-rays : Studies at RRCAT

Intrinsic beam emittance of laser-accelerated electrons measured by x-ray spectroscopic imaging

Oriented single crystal photocathodes: A route to high-quality electron pulses. W. Andreas Schroeder. Benjamin L. Rickman and Tuo Li

Electro optic sampling as a timing diagnostic at Pegasus lab

High Accuracy Adaptive (transverse) Laser and Electron Beam Shaping. Jared Maxson Cornell University ERL 2015, BNL

Femto-second FEL Generation with Very Low Charge at LCLS

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

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

Advanced laser technology for 3D-shaping ~ toward to the highest brightness of electron beam source ~

DESIGN AND CONSTRUCTION OF LOW ENERGY ELECTRON ACCELERATORS AT SINP MSU

AP5301/ Name the major parts of an optical microscope and state their functions.

Nanocomposite photonic crystal devices

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland

THz field strength larger than MV/cm generated in organic crystal

Scientific opportunities with ultrafast electron diffraction & microscopy

Simulations for photoinjectors C.Limborg

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

Status of linear collider designs:

Development of reliable and sophisticated photo injector system and future plan

Femto second X ray Pulse Generation by Electron Beam Slicing. F. Willeke, L.H. Yu, NSLSII, BNL, Upton, NY 11973, USA

Optical Spectroscopy of Advanced Materials

Laser-driven undulator source

Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston

Inverse Compton Scattering Sources from Soft X-rays to γ-rays

4GLS Status. Susan L Smith ASTeC Daresbury Laboratory

Emittance and Quantum Efficiency Measurements from a 1.6 cell S- Band Photocathode RF Gun with Mg Cathode *

Beam Dynamics and SASE Simulations for XFEL. Igor Zagorodnov DESY

The UCLA/LLNL Inverse Compton Scattering Experiment: PLEIADES

High quality beam generation and its application at Waseda University

Time resolved optical spectroscopy methods for organic photovoltaics. Enrico Da Como. Department of Physics, University of Bath

Trends in X-ray Synchrotron Radiation Research

Injector Experimental Progress

Opportunities and Challenges for X

Performance Metrics of Future Light Sources. Robert Hettel, SLAC ICFA FLS 2010 March 1, 2010

Transverse emittance measurements on an S-band photocathode rf electron gun * Abstract

3D- Laser pulse shaping System to Minimize Emittance for Photocathode RF gun ~ toward to the highest brightness of electron beam source ~

Beam Shaping and Permanent Magnet Quadrupole Focusing with Applications to the Plasma Wakefield Accelerator

Low Energy RHIC electron Cooling (LEReC)

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

OPTIMIZING RF LINACS AS DRIVERS FOR INVERSE COMPTON SOURCES: THE ELI-NP CASE

Update on Development of High Current Bunched Electron Beam from Magnetized DC Photogun

Investigations on the electron bunch distribution in the longitudinal phase space at a laser driven RF-electron source for the European X-FEL

Dielectric Accelerators at CLARA. G. Burt, Lancaster University On behalf of ASTeC, Lancaster U., Liverpool U., U. Manchester, and Oxford U.

Supplementary Figures

RF-Gun Experience at PITZ - Longitudinal Phase Space

Nanotechnology Nanofabrication of Functional Materials. Marin Alexe Max Planck Institute of Microstructure Physics, Halle - Germany

Dark current at the Euro-XFEL

Photoinjector design for the LCLS

LCLS-II SCRF start-to-end simulations and global optimization as of September Abstract

The MID instrument.

Second-Harmonic Generation Studies of Silicon Interfaces

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

Center for the Advancement of Natural Discoveries using Light Emission AREAL. Facility Status and Highlights. V. Tsakanov. 12 July 2016, DESY, Hamburg

Transcription:

UESDM, UCLA, Dec. 12 14, 2012 MeV electron diffraction and microscopy in Osaka University Jinfeng Yang Osaka University, Japan Collaborators: (RIKEN) Yoshie Murooka (Osaka Univ.) Y. Naruse, K. Kan, K. Tanimura, Y. Yoshida

Outline 1. Development of RF gun for UED/UEM Requirements / experimental results 2. RF gun based UED at Osaka Univ. MeV UED systems / measurements 3. RF gun based UEM at Osaka Univ. prototype of RF gun based UEM first electron image measurement 4Conclusion 4.

Photocathode th RF gun for electron diffraction/microscopy in Osaka Univ.

What requirements for UEM? Femtosecond laser fs, λ=266nm RF 2856MHz ~MW@4μs Femtosecond e- bunch ~MeV, ~pc Photocathode Cu, Mg RF cavity,~100mv/m (Usually 1.5-cell) The expected beam parameters: Bunch length: 100 fs Beam energy: 1~3 MeV Emittance: ~0.1 mm-mrad Energy spread: ~10-4 (10-5 for challenge) e- number: 10 7-8 e - s/bunch (1~10 pc) with ultralow dark current

New femtosecond RF gun Developed under the collaboration with KEK Improvements: remove two laser injection ports a new turner system new structure cavities a new insertion function of photocathode (The photocathode is removable) (The cooling system and waveguide design are same as the BNL gun-iv.) The mode separation between π mode and 0 mode is increased up to f π -f 0 = 8.5 MHz. The Q value is increased up to 14,500.

Transverse beam dynamics in RF gun Experiment studies of femtosecond e- beam in RF gun (exp. conditions: 100 fs UV laser, 30 o gun phase, 3MeV) For a copper cathode, the thermal emittance can be Reducing laser spot size to 0.1mm, ε th E kin = σ r 0. 18 mm mrad 2 m c 0 E kin = hv φ + α βe sin θ 0. 26eV 0 ε ~ 0.1mm mrad

RF gun based MeV electron diffraction at Osaka Univ. Electron energy: 1~3 MeV Time resolution: 100 fs

RF gun based MeV UED at Osaka Univ. use of electron optical lenses as like in electron microscopy RF gun 1-5MW@4μs,10Hz 2856MHz Solenoid Aperture Φ0.3mm <10-8 Pa C.Lens sample Scintillator Sample Φ3.0mm DL D.Lens PL P.Lens Φ300, 350μm Probe 3ω: Pump 2ω: 257nm,90fs, 385nm,90fs, 1kHz, 6mW 10Hz, <40mJ/cm 2 EMCCD CsI (Tl) scintillator Area: 5x5cm Probe 3ω Pump 2ω (Φ600μm, 18.2 o,p-pol ) [1-10] Diffraction 3MeV 10Hz 100 fs e- pulse 4.5x10 7 e/pulse aperture Φ0.3mm Si crystal diffraction

Picture of UED system at Osaka Univ. S.L RF gun PL DL S CL CCD 25m 2.5 use of electron optical lenses, therefore, compact.

Quality of MeV electron diffraction 7 2 Electron beam: 3 MeV, 8.9 10 e / cm / Sample: 180nm-thick single crystal Si Si<001> pulse Intensity profile of 620 pattern 620 20 shots(2s) A high-quality MeV ED was observed! Beam convergence angle: 50μrad Bragg law Maximum scattering vector : q 2d sin θ = nλ max >1.56Å -1 D tan 2α = Requirement of the e - number: 10 6-7 L Y. Murooka, et al., Appl. Phys. Lett. 98, 251903 (2011)

Power of the technique: static diffractions Single-shot measurement Si single crystal Thickness: 180nm 1 shot (0.1s) Au single crystal Thickness: 20nm 1 shot (0.1s) e-energy:3mev e-energy:3mev Y. Murooka, et al., Appl. Phys. Lett. 98, 251903 (2011) Si Au Metal (Al) Insulator (Mica) polycrystal (100nm) 440 422 331 311 220 200 111 Single crystal (~100s nm) K(Fe,Mg) 3 (AlSi 3 O 10 )(OH,F) 2 top side SiO 4 fcc SiO 4 K Fe, Mg Large scattering vector q max 600 No charging effect (Difficult at Low Voltage)

Time-resolved measurement #2 Laser heating and melting dynamics of single crystal Au 200-4 ps 3 ps 16 ps after melting

RF gun based ultrafast electron microscopy Electron beam energy: 1~3 MeV Temporal resolution: 100 fs Spatial resolution: 10 nm

Concept of RF gun based UEM 50μm spot RF gun RF aperture-2 Specimen Objective lens Solenoid 50-fs laser Intermediate lens CL-1 5μmspot CL-2 aperture-1 Projector lens Specimen 10μm spot Image screen (1024x1024 pixels)

Prototype of RF gun based MeV electron microscopy RF gun Femtosecond Laser Femtosecond electron beam Femtosecond photocathode electron gun 3m electron optical lenses image meas. Electron energy: 1~3 MeV Bunch length : 100 fs Emittance: <01mmmrad 0.1mm-mrad Energy spread: 10-4 (10-5 for challenge) Charge: 10 7 ~10 8 e - s/pulse Time resolution: 100 fs Spatial resolution: 10 nm Prototype of MeV UEM Challenge!

Prototype of RF gun based MeV electron microscopy RF gun based injector 2T objective lens Interm. & proj. lenses Femtosecond electron beam Femtosecond Laser 2010 2011 Image recording system Prototype of UEM (height: 3m, diameter: 0.7m) 2012 The prototype was constructed at the end of Oct. 2012.

Detection of MeV electron images MeV electron CsI (Tl) scintillator (Hamamatsu) Illu. Vol.(<50µm) Bright High resol. (Column Structure) Tough (for High E Xray) Large: 5x5cm Thin Polymer mirror (5µm) X, e ORCA-R 2 CCD The detection system was successfully used in UED measurement. (single-shot shot measurement with 10 5 e - s/pulse)

MeV electron diffraction in UEM MeV electron diffractions observed with 10 pulses and single-shot measurements First exp. at Nov. 9, 2012 10 pulses Electron beam (2 MeV) Specimen Objective Lens diff. plane (BFP) Projector lens Imaging plane (Selector diaphragm) Single-shot Sample: Au single crystal, ~15 nm Electron charge: ~100 fc/pulse on the scintillator

MeV electron imaging in UEM First exp. at Nov. 10, 2012 Objective Lens (Obj. Aper.) Electron beam (2 MeV) Specimen BFP Images of Au film 38 μm 83μm x50 Exposure time:2s Exposure time:60s Observed images of Au film 10μm 38nm/pixel Projector lens Interm. image plane X385 x650 x1200 Final image screen Observation #1 10μm 38nm/pixel Sample: Au single crystal, ~15 nm Electron charge: ~10 fc/pulse on the scintillator Observation #2 x650 x1200 19

Magnifications & spatial resolution RF gun Solenoid lens 5.5 μm Femtosecond electron beam CL-1 CL-2 Specimen Cu grid (1000mesh) 25μm X200 Objective lens Intermediate t lens 10μm 75 nm/pixel 5 μm 30 nm/pixel Projector lens Spatial resolution in future 300 nm 10nm 観測例 1 X650 x1700 σ~300nm σ~300nm <1nm

Next TEM: Dream TEM Weight: 140t photocathode RF gun 15cm 10m Compact High-voltage Transmission Electron Microscopy 3m 3m high-voltage TEM function (nm or sub-nm, MeV) + time-resolved function (femtosecond) Standard 3-MeV TEM at Osaka Univ. Next TEM Dream TEM!

New science and technology using UEM Electron beam (1~3MeV) Imaging Technology イメージングテクノロジー Structural observation and imaging in real space with atomic-scale spatial resolution using high-energy electron beam. Compact high-voltage electron microscopy (dream TEM) Methods MeV UEM Pump laser pulse Electron pulse(probe) Ultrafast Observation 超高速現象の観察 Observations of fundamental dynamic processes in matter occurring on femtosecond time scales over atomic spatial dimensions. Protein Structural Dynamics Visualizations of protein structural dynamics using ultrafast electron diffraction and imaging technique. New technologies and applications in medical biology. Targets Making Molecular Movie Observation of single molecule motion. Ultrafast chemical reactions. Discovery of transition states and reaction intermediates. Nano-technology Photon-induced ultrafast dynamics of novel nano-scale materials. Creation of new functional materials and devices for nanotechnology.

Conclusion Both RF gun based UED and UEM systems have been constructed at Osaka University. In UED, single-shot and time-resolved measurements have been succeeded. In UEM, the MeV electron imaging experiment was carried out. Both experiments suggest that RF gun is very useful for ultrafast MeV electron diffraction and is also expected to be used in ultrafast electron microscopy. However, great efforts and many challenges are required: reduce further the emittance (<0.1 μm) and energy spread (10-5 or less), increase the beam brightness, improve the stabilities on the charge and energy, develop a detection of very electron with MeV energy region.