Bioimaging of cells and tissues using accelerator-based sources

Size: px
Start display at page:

Download "Bioimaging of cells and tissues using accelerator-based sources"

Transcription

1 Analytical and Bioanalytical Chemistry Electronic Supplementary Material Bioimaging of cells and tissues using accelerator-based sources Cyril Petibois, Mariangela Cestelli Guidi Main features of Free Electron Lasers (FELs) implemented around the world. FLASH Wavelength range of the fundamental nm (from fall 2007: 6.5 nm) Higher harmonics 3rd 4.6 nm, 5th 2.7 nm, (7th 1.9 nm) Average pulse energy up to 100 μj Peak pulse energy 170 μj Peak power 5 GW Average power 100 mw Pulse duration fs Spectral width 0.5-1% Peak brilliance [photons/(s mrad² mm² 0.1% BW)] DUKE FEL The Duke Free Electron Laser Laboratory operates a storage ring based free electron laser light source. This ultraviolet FEL installed on a 1.2 GeV storage ring provides tunable coherent radiation from 400 nm to 193 nm. Intense gamma rays are produced by internal backscattering. Active areas of research at DFELL include FEL physics, nuclear physics, materials science, and biological and biomedical sciences. Ring Circumference m (central orbit) Operating Energy GeV (with energy ramping) Injection Energy GeV Revolution Frequency MHz Energy Acceptance ± 6% Beam Current 115 ma (in 5 bunches) Single Bunch 12 ma Horizontal Emittance 17-19E-9 m*rad Vertical Emittance < 1E-9 m*rad Bunch Length < 50 ps Coherent Emission nm

2 VANDERBILT UNIVERSITY Laser Wavelengths 2.1 to 9.8 microns Mirror Bandwidths , , , Electron beam energy 25 to 45 MeV Electron macropulse length 8.0 microseconds Electron micropulse length <1 picosecond (approximately 0.7 ps) Electron bunch separation 10.5 cm, 351 ps RF power 12 to 30 MW RF pulse length 9.0 microseconds Klystron video pulse length 14 microseconds Repetition rate, up to 30 Hz FELIX Wavelength range: µm cm-1 Spectral width % Polarization (linear) > 99 % Micropulse duration (FWHM) optical cycles Micropulse energy 1 50 µj Micropulse power MW Micropulse repetition rate 25 or 1000 MHz Macropulse duration < 10 µs Duty cycle < 10 Hz The primary application of the facility is in the studies of the vibrational dynamics of molecules, liquids, and solids, but other applications requiring an intense source in the spectral range covered, such as photo-ablation of tissue, near-field microscopy or linear spectroscopy of small-sized samples, are equally appropiate. An overview of research areas can be found here.

3 Stanford Picosecond FEL Center (US) Mid-IR (STI) Far-IR (Firefly) Wavelength 3-15 microns microns Micropulse Width ps 2-10 ps Micropulse Repetition Rate 84.6 ns 84.6 ns Macropulse Width 5 ms 5 ms Macropulse Repetition Rate 20 Hz 20 Hz Micropulse Energy 2 microjoule 1 microjoule Average Power 2 W 1 W Spectral Bandwidth Transform-Limited Transform-Limited Gaussian Gaussian Spectral Stability 0.01 % rms 0.01 % rms Amplitude Stability < 2 % rms < 2 % rms Annual Operations 2000 hours CLIO (MID IR) Spectral range Max. average power Max. peak power Laser pulse length Minimum spectral width 3 to 150 microns (for different e- energies) 1 16ns/25Hz 100 MW in 1ps 0.5 to 6 ps (adjustable) 0.2 to 2 % (wavelength dependant)

4 Jefferson Lab FEL IR Branch UV Branch Wavelength range (microns) Bunch Length (FWHM psec) Laser power / pulse (microjoulesj) Laser power (kw) > 10 > 1 Repetition Rate (cw operation, MHz) Jefferson Lab FEL Electron Beam Parameters Energy (MeV) Charge per bunch (pc) Average current (ma) 10 5 Peak Current (A) Beam Power (kw) Energy Spread (%) 0.50% 0.13% Normalized emittance (mm-mrad) <30 <11 Induced energy spread (full) 10% 5% Jefferson Lab (Broadband) THz Beamline Parameters Wavelength Range (THz) Pulse Length (ps) Power / pulse (microjoules) 2 Repetition Rate 1 Hz - 75 MHz Total Power (watts) 150 FEL-SUT (Tokio) MIR-FEL Tunable wavelength region Spectral bandwidth Micro-pulse time width Micro-pulse repetition frequency Micro-pulse energy Micro-pulse peak power Macro-pulse time width Macro-pulse energy Macro-pulse repetition rate Maximum average power 5~16 μm ~0.5 % 2 ps 2856 MHz 8~25 μj 2~5 MW 1 μs ~150 mj Max. 10 pps ~1W (for 10pps operation)

5 UCSB The primary radiation source at the UCSB Center for Terahertz Science and Technology consists of two fully operational Free-Electron Lasers, the MM-FEL and the FIR-FEL, covering the range of 2.5 mm to 63 µm (4 to 160 cm-1 or 120 GHz to 4.75 THz). MMFEL WAVELENGTH RANGE: 2.5 mm -> 338 µm (0.12 -> 0.89 THz), (4 -> 30 cm-1) POWER: 1 -> 15 KW depending on wavelength and coupler PULSE LENGTH: 1 -> 6 µs FIR-FEL WAVELENGTH RANGE: 338 -> 63 µm (0.89 -> 4.76 THz),(30 -> 160 cm-1) POWER: 1 -> 6 KW depending on wavelength and coupler PULSE LENGTH: 1 -> 20 µs PULSE REPETITION RATE: 0 -> 7.5 Hz FELBE FEL (Germany) Wavelength range 4-22 μm undulator U μm undulator U100 Pulse energy μj depending on wavelength Pulse length ps depending on wavelength Repetition rate 13 MHz 3 modes: - cw - macropulsed > 100 μs, < 25 Hz - single-pulse switched to khz/hz

6 ENEA FEL (Italy) COMPACT MM-WAVE FEL DESIGN PARAMETERS Electron Energy (MeV) 2.3 Energy spread 1% I-peak (A) 4 Und. period (cm) 2.5 I-av (A) 0.2 N (num. of periods) 8 Micropulse duration (ps) 15 Undulator par. K 1 Macropulse duration (s) 4 Waveguide hor. gap (mm) Norm. emittance (cm rad) 0.02 Waveguide vert. gap (mm) 4.32 FIR FREE ELECTRON LASER DESIGN PARAMETERS Wavelength (m) Electron Energy (MeV) Peak Electron Current I (A) Average Current on Macro-Bunch (A) 0.45 A 0.45 A Micro-Bunch Duration (FWHM) 3.7 ps 3.7 ps Macro-Bunch Duration 2-7 s 2-7 s Electron Normalized Emittance 16 mm mrad 16 mm mrad Undulator Period u (cm) Number of Periods N Undulator Parameter K Waveguide horizontal gap a (cm) 3 3 Waveguide vertical gap b (cm) Waveguide length L (cm) Power macropulse (kw) 35 35

7 S-DALINAC (IR Darmstad) Laser Properties Wavelength 3-10 µm Pulse Length ~2 ps Pulse Energy 300 nj Small Signal Gain 3-5 % Pulse Peak Power 150 kw Average Power 3 W BFEL (Beijing) Wavelength Range 5-25μm Spectrum Width 0.5-2% Macro-pulse Width 2μs Micro-pulse Width 4ps Macro-pulse Energy 2-10mJ Micro-pulse Energy 0.4-2μJ Repetition Rate 3.125Hz Energy Fluctuation <5% Wavelength Stability 0.1% Lasing Time for Users

ERL based FELs. Todd I Smith Hansen Experimental Physics Laboratories (HEPL) Stanford University Stanford, CA

ERL based FELs. Todd I Smith Hansen Experimental Physics Laboratories (HEPL) Stanford University Stanford, CA ERL based FELs Todd I Smith Hansen Experimental Physics Laboratories (HEPL) Stanford University Stanford, CA 94305-4085 Todd.Smith@Stanford.edu Electrostatic ERL-FELs University of California Santa Barbara

More information

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously FLASH at DESY The first soft X-ray FEL operating two undulator beamlines simultaneously Katja Honkavaara, DESY for the FLASH team FEL Conference 2014, Basel 25-29 August, 2014 First Lasing FLASH2 > First

More information

KU-FEL Facility. Status Report. Konstantin Torgasin PhD Student Graduate School of Energy Science Kyoto University

KU-FEL Facility. Status Report. Konstantin Torgasin PhD Student Graduate School of Energy Science Kyoto University KU-FEL Facility Status Report Konstantin Torgasin PhD Student Graduate School of Energy Science Kyoto University KU-FEL(Kyoto University FEL) A mid-infrared free electron laser (MIR-FEL) facility KU-FEL

More information

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser P. Castro for the TTF-FEL team 100 nm 1 Å FEL radiation TESLA Test Facility at DESY

More information

FLASH II. FLASH II: a second undulator line and future test bed for FEL development.

FLASH II. FLASH II: a second undulator line and future test bed for FEL development. FLASH II FLASH II: a second undulator line and future test bed for FEL development Bart.Faatz@desy.de Outline Proposal Background Parameters Layout Chalenges Timeline Cost estimate Personnel requirements

More information

High Power and Energy Femtosecond Lasers

High Power and Energy Femtosecond Lasers High Power and Energy Femtosecond Lasers PHAROS is a single-unit integrated femtosecond laser system combining millijoule pulse energies and high average powers. PHAROS features a mechanical and optical

More information

Wisconsin FEL Initiative

Wisconsin FEL Initiative Wisconsin FEL Initiative Joseph Bisognano, Mark Bissen, Robert Bosch, Michael Green, Ken Jacobs, Hartmut Hoechst, Kevin J Kleman, Robert Legg, Ruben Reininger, Ralf Wehlitz, UW-Madison/SRC William Graves,

More information

High-Power Femtosecond Lasers

High-Power Femtosecond Lasers High-Power Femtosecond Lasers PHAROS is a single-unit integrated femtosecond laser system combining millijoule pulse energies and high average power. PHAROS features a mechanical and optical design optimized

More information

improved stability (compared with

improved stability (compared with Picosecond Tunable Systems Nanosecond Lasers NT230 SERIES NT230 series lasers deliver high up to 10 mj energy pulses at 100 Hz pulse repetition rate, tunable over a broad spectral range. Integrated into

More information

Operating longitudinal mode Several Polarization ratio > 100:1. Power. Warranty. 30 <1.5 <5% Near TEM ~4.0 one year

Operating longitudinal mode Several Polarization ratio > 100:1. Power. Warranty. 30 <1.5 <5% Near TEM ~4.0 one year DL CW Blue Violet Laser, 405nm 405 nm Operating longitudinal mode Several Applications: DNA Sequencing Spectrum analysis Optical Instrument Flow Cytometry Interference Measurements Laser lighting show

More information

Designing for Femtosecond Pulses

Designing for Femtosecond Pulses Designing for Femtosecond Pulses White Paper PN 200-1100-00 Revision 1.1 July 2013 Calmar Laser, Inc www.calmarlaser.com Overview Calmar s femtosecond laser sources are passively mode-locked fiber lasers.

More information

Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics

Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics J. Michael Klopf Jefferson Lab - Free Electron Laser Division Workshop on Future Light Sources SLAC

More information

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009 Beam for LCLS Henrik Loos Workshop July 29-31, 29 1 1 Henrik Loos Overview Coherent Radiation Sources Timing THz Source Performance 2 2 Henrik Loos LCLS Layout 6 MeV 135 MeV 25 MeV 4.3 GeV 13.6 GeV σ z.83

More information

SNV/U High Performances UV Microchip Series

SNV/U High Performances UV Microchip Series SNV/U High Performances UV Microchip Series Key features 355nm and 266nm Repetition rate up to 20kHz Ultrashort pulses down to 550ps Multi-kW peak power Excellent beam quality Efficient, air-cooled Sealed

More information

FLASH: Status and upgrade

FLASH: Status and upgrade : Status and upgrade The User Facility Layout Performance and operational o a issues Upgrade Bart Faatz for the team DESY FEL 2009 Liverpool, UK August 23-28, 2009 at DESY > FEL user facility since summer

More information

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg,

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, FLASH 2 FEL seminar Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, 2016-03-22 Charge: 0.5 nc Overview 1. FLASH 2 Overview 1.Layout parameters 2. Operation FLASH2. 1.Lasing at wavelengths between

More information

FREE ELECTRON LASER RESEARCH IN CHINA

FREE ELECTRON LASER RESEARCH IN CHINA 1996 IEEE. Personal use of this material is permitted. However, permission to reprint/republish this material for advertising or promotional purposes or for creating new collective works for resale or

More information

SwissFEL Design and Status

SwissFEL Design and Status SwissFEL Design and Status Hans H. Braun Mini Workshop on Compact X ray Free electron Lasers Eastern Forum of Science and Technology Shanghai July 19, 2010 SwissFEL, the next large facility at PSI SwissFEL

More information

Power. Warranty. 30 <1.5 <3% Near TEM ~4.0 one year. 50 <1.5 <5% Near TEM ~4.0 one year

Power. Warranty. 30 <1.5 <3% Near TEM ~4.0 one year. 50 <1.5 <5% Near TEM ~4.0 one year DL CW Blue Violet Laser, 405nm 405 nm Operating longitudinal mode Several Applications: DNA Sequencing Spectrum analysis Optical Instrument Flow Cytometry Interference Measurements Laser lighting show

More information

Status, perspectives, and lessons from FLASH and European XFEL

Status, perspectives, and lessons from FLASH and European XFEL 2014 International Workshop on EUV and Soft X-ray Sources November 3-6, 2014 Dublin, Ireland Status, perspectives, and lessons from FLASH and European XFEL R. Brinkmann, E.A. Schneidmiller, J, Sekutowicz,

More information

FLASH Upgrade. Decrease wavelength and/or increase brilliance

FLASH Upgrade. Decrease wavelength and/or increase brilliance FLASH Upgrade Far-Infrared (FIR) undulator Medium and long-term issues: Decrease wavelength and/or increase brilliance Enable quasi-simultanous operation at 2 wavelengths Provide more space for users Motivation:

More information

Conceptual Design of a Table-top Terahertz Free-electron Laser

Conceptual Design of a Table-top Terahertz Free-electron Laser Journal of the Korean Physical Society, Vol. 59, No. 5, November 2011, pp. 3251 3255 Conceptual Design of a Table-top Terahertz Free-electron Laser Y. U. Jeong, S. H. Park, K. Lee, J. Mun, K. H. Jang,

More information

THz Imaging by a Wide-band Compact FEL

THz Imaging by a Wide-band Compact FEL FEL-2004, Trieste, Italy THz Imaging by a Wide-band Compact FEL 2 Sep. 2004 Young Uk Jeong, Grigori M. Kazakevitch b, Hyuk Jin Cha, Seong Hee Park, and Byung Cheol Lee Korea Atomic Energy Research Institute

More information

Atlantic. Industrial High Power Picosecond Lasers. features

Atlantic. Industrial High Power Picosecond Lasers. features Industrial High Picosecond Lasers lasers have been designed as a versatile tool for a variety of industrial material processing applications. They are compact, OEM rugged, with up to 6 W output power at

More information

arxiv:physics/ v1 [physics.acc-ph] 18 Jul 2003

arxiv:physics/ v1 [physics.acc-ph] 18 Jul 2003 DESY 03 091 ISSN 0418-9833 July 2003 arxiv:physics/0307092v1 [physics.acc-ph] 18 Jul 2003 Two-color FEL amplifier for femtosecond-resolution pump-probe experiments with GW-scale X-ray and optical pulses

More information

Short-Pulse X-ray at the Advanced Photon Source Overview

Short-Pulse X-ray at the Advanced Photon Source Overview Short-Pulse X-ray at the Advanced Photon Source Overview Vadim Sajaev and Louis Emery Accelerator Operations and Physics Group Accelerator Systems Division Mini-workshop on Methods of Data Analysis in

More information

COMMISSIONING STATUS AND FURTHER DEVELOPMENT OF THE NOVOSIBIRSK MULTITURN ERL*

COMMISSIONING STATUS AND FURTHER DEVELOPMENT OF THE NOVOSIBIRSK MULTITURN ERL* COMMISSIONING STATUS AND FURTHER DEVELOPMENT OF THE NOVOSIBIRSK MULTITURN ERL* O.A.Shevchenko #, V.S.Arbuzov, E.N.Dementyev, B.A.Dovzhenko, Ya.V.Getmanov, E.I.Gorniker, B.A.Knyazev, E.I.Kolobanov, A.A.Kondakov,

More information

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS A. Aryshev On behalf of QB group and THz collaboration 14 Outline THz project overview LUCX activity LUCX Projects Overview THz program LUCX Laser system LUCX

More information

Drive Beam Photo-injector Option for the CTF3 Nominal Phase

Drive Beam Photo-injector Option for the CTF3 Nominal Phase CTF3 Review Drive Beam Photo-injector Option for the CTF3 Nominal Phase Motivation CTF3 Drive Beam Requirements CTF3 RF gun design The Laser (I. Ross / RAL) The Photocathode Cost estimate Possible schedule

More information

PGx11 series. Transform Limited Broadly Tunable Picosecond OPA APPLICATIONS. Available models

PGx11 series. Transform Limited Broadly Tunable Picosecond OPA APPLICATIONS. Available models PGx1 PGx3 PGx11 PT2 Transform Limited Broadly Tunable Picosecond OPA optical parametric devices employ advanced design concepts in order to produce broadly tunable picosecond pulses with nearly Fourier-transform

More information

Atlantic. Industrial High Power Picosecond Lasers. features

Atlantic. Industrial High Power Picosecond Lasers. features Atlantic Industrial High Power Picosecond Lasers lasers have been designed as a versatile tool for a variety of industrial material processing applications. They are compact, OEM rugged, with up to 8 W

More information

ERLP Status. Mike Dykes

ERLP Status. Mike Dykes ERLP Status Mike Dykes Content ASTeC RF & Diagnostics Group Work of the Group 4GLS ERLP Photo-injector Accelerating Modules Summary High Power RF Engineering Andy Moss SRS Support; DIAMOND; ERLP; MICE;

More information

Atlantic. Industrial High Power Picosecond Lasers. features

Atlantic. Industrial High Power Picosecond Lasers. features Atlantic Industrial High Picosecond Lasers lasers have been designed as a versatile tool for a variety of industrial material processing applications. They are compact, OEM rugged, with up to 8 W output

More information

R&D Toward Brighter X-ray FELs

R&D Toward Brighter X-ray FELs Some R&D Toward Brighter X-ray FELs Zhirong Huang (SLAC) March 6, 2012 FLS2012 Workshop, Jefferson Lab Outline Introduction Seeding for temporal coherence Hard x-rays Soft x-rays Push for higher power

More information

Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY

Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at FLASH @ DESY N. Baboi, DESY, Hamburg for the HOM team : S. Molloy 1, N. Baboi 2, N. Eddy 3, J. Frisch 1, L. Hendrickson

More information

3 General layout of the XFEL Facility

3 General layout of the XFEL Facility 3 General layout of the XFEL Facility 3.1 Introduction The present chapter provides an overview of the whole European X-Ray Free-Electron Laser (XFEL) Facility layout, enumerating its main components and

More information

Sub-ps (and sub-micrometer) developments at ELETTRA

Sub-ps (and sub-micrometer) developments at ELETTRA Sub-ps (and sub-micrometer) developments at ELETTRA Mario Ferianis SINCROTRONE TRIESTE, Italy The ELETTRA laboratory ELETTRA is a 3 rd generation synchrotron light source in Trieste (I) since 1993 up to

More information

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation Infrared Single Shot Diagnostics for the Longitudinal Profile of the Electron Bunches at FLASH Disputation Hossein Delsim-Hashemi Tuesday 22 July 2008 7/23/2008 2/ 35 Introduction m eb c 2 3 2 γ ω = +

More information

Atlantic. series. Industrial High Power Picosecond DPSS Lasers

Atlantic. series. Industrial High Power Picosecond DPSS Lasers Atlantic series Industrial High Power Picosecond DPSS Lasers Laser description Laser micromachining is rapidly becoming the material processing technology of choice for numerous small scale, real world

More information

Circumference 187 m (bending radius = 8.66 m)

Circumference 187 m (bending radius = 8.66 m) 4. Specifications of the Accelerators Table 1. General parameters of the PF storage ring. Energy 2.5 GeV (max 3.0 GeV) Initial stored current multi-bunch 450 ma (max 500 ma at 2.5GeV) single bunch 70 ma

More information

5kW DIODE-PUMPED TEST AMPLIFIER

5kW DIODE-PUMPED TEST AMPLIFIER 5kW DIODE-PUMPED TEST AMPLIFIER SUMMARY?Gain - OK, suggest high pump efficiency?efficient extraction - OK, but more accurate data required?self-stabilisation - Yes, to a few % but not well matched to analysis

More information

LCLS-II-HE Instrumentation

LCLS-II-HE Instrumentation LCLS-II-HE Instrumentation Average Brightness (ph/s/mm 2 /mrad 2 /0.1%BW) LCLS-II-HE: Enabling New Experimental Capabilities Structural Dynamics at the Atomic Scale Expand the photon energy reach of LCLS-II

More information

ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II*

ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II* THB04 Proceedings of FEL2014, Basel, Switzerland ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II* Josef Frisch, Paul Emma, Alan Fisher, Patrick Krejcik, Henrik Loos, Timothy Maxwell, Tor Raubenheimer,

More information

Mira OPO-X. Fully Automated IR/Visible OPO for femtosecond and picosecond Ti:Sapphire Lasers. Superior Reliability & Performance. Mira OPO-X Features:

Mira OPO-X. Fully Automated IR/Visible OPO for femtosecond and picosecond Ti:Sapphire Lasers. Superior Reliability & Performance. Mira OPO-X Features: Fully Automated IR/Visible OPO for femtosecond and picosecond Ti:Sapphire Lasers Mira OPO-X is a synchronously pumped, widely tunable, optical parametric oscillator (OPO) accessory that dramatically extends

More information

taccor Optional features Overview Turn-key GHz femtosecond laser

taccor Optional features Overview Turn-key GHz femtosecond laser taccor Turn-key GHz femtosecond laser Self-locking and maintaining Stable and robust True hands off turn-key system Wavelength tunable Integrated pump laser Overview The taccor is a unique turn-key femtosecond

More information

Background. Three basic directions for timing experiments were specified by the user community at the meeting:

Background. Three basic directions for timing experiments were specified by the user community at the meeting: Preliminary report on alternate bunch schemes for the MAX IV storage rings Stacey Sorensen, Nils Mårtensson, Raimund Feifel, Christian Stråhlman, Simon Leemann Background The primary design goal of the

More information

1-Å FEL Oscillator with ERL Beams

1-Å FEL Oscillator with ERL Beams 1-Å FEL Oscillator with ERL Beams 29 th International FEL Conference August 26-31, BINP Novosibirsk, Russia Kwang-Je Kim, ANL Sven Reiche, UCLA Yuri Shvyd ko, ANL FELs for λ

More information

On-line spectrometer for FEL radiation at

On-line spectrometer for FEL radiation at On-line spectrometer for FEL radiation at FERMI@ELETTRA Fabio Frassetto 1, Luca Poletto 1, Daniele Cocco 2, Marco Zangrando 3 1 CNR/INFM Laboratory for Ultraviolet and X-Ray Optical Research & Department

More information

THE ORION PHOTOINJECTOR: STATUS and RESULTS

THE ORION PHOTOINJECTOR: STATUS and RESULTS THE ORION PHOTOINJECTOR: STATUS and RESULTS Dennis T. Palmer SLAC / ARDB ICFA Sardinia 4 July 2002 1. Introduction 2. Beam Dynamics Simulations 3. Photoinjector 1. RF Gun 2. Solenoidal Magnet 3. Diagnostics

More information

Testing with Femtosecond Pulses

Testing with Femtosecond Pulses Testing with Femtosecond Pulses White Paper PN 200-0200-00 Revision 1.3 January 2009 Calmar Laser, Inc www.calmarlaser.com Overview Calmar s femtosecond laser sources are passively mode-locked fiber lasers.

More information

Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs

Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs Alex H. Lumpkin Accelerator Operations Division Advanced Photon Source Presented at Jefferson National Accelerator Laboratory

More information

Progress in ultrafast Cr:ZnSe Lasers. Evgueni Slobodtchikov, Peter Moulton

Progress in ultrafast Cr:ZnSe Lasers. Evgueni Slobodtchikov, Peter Moulton Progress in ultrafast Cr:ZnSe Lasers Evgueni Slobodtchikov, Peter Moulton Topics Diode-pumped Cr:ZnSe femtosecond oscillator CPA Cr:ZnSe laser system with 1 GW output This work was supported by SBIR Phase

More information

H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group

H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group 7+(7(6/$;)(/352-(&7 H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group $EVWUDFW The overall layout of the X-Ray FEL to be built in international collaboration at DESY will

More information

Lasers à fibres ns et ps de forte puissance. Francois SALIN EOLITE systems

Lasers à fibres ns et ps de forte puissance. Francois SALIN EOLITE systems Lasers à fibres ns et ps de forte puissance Francois SALIN EOLITE systems Solid-State Laser Concepts rod temperature [K] 347 -- 352 342 -- 347 337 -- 342 333 -- 337 328 -- 333 324 -- 328 319 -- 324 315

More information

Calibrating the Cavity Voltage. Presentation of an idea

Calibrating the Cavity Voltage. Presentation of an idea Calibrating the Cavity Voltage. Presentation of an idea Stefan Wilke, DESY MHF-e 21st ESLS rf meeting Kraków, 15th/16th nov 2017 Accelerators at DESY. linear and circular Page 2 Accelerators at DESY. linear

More information

Nuclear Instruments and Methods in Physics Research A

Nuclear Instruments and Methods in Physics Research A Nuclear Instruments and Methods in Physics Research A 729 (2013) 19 24 Contents lists available at ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima

More information

Romania and High Power Lasers Towards Extreme Light Infrastructure in Romania

Romania and High Power Lasers Towards Extreme Light Infrastructure in Romania Romania and High Power Lasers Towards Extreme Light Infrastructure in Romania Razvan Dabu, Daniel Ursescu INFLPR, Magurele, Romania Contents GiWALAS laser facility TEWALAS laser facility CETAL project

More information

Coherent Synchrotron Radiation in the ANKA Storage Ring

Coherent Synchrotron Radiation in the ANKA Storage Ring Coherent Synchrotron Radiation in the ANKA Storage Ring Marcel Schuh On behalf of the ANKA THz-Group Laboratory for Applications of Synchrotron Radiation (LAS) / Institute of Synchrotron Radiation (ISS)

More information

Timing Issues for the BESSY Femtoslicing Source

Timing Issues for the BESSY Femtoslicing Source ICFA Workshop on Future Light Sources, Hamburg, May 15-19th, 2006 Timing Issues for the BESSY Femtoslicing Source Shaukat Khan, University of Hamburg R. Mitzner, University of Münster T. Quast, BESSY/Berlin

More information

National Science Foundation Center for Lasers and Plasmas for Advanced Manufacturing. Mool C. Gupta Applied Research Center Old Dominion University

National Science Foundation Center for Lasers and Plasmas for Advanced Manufacturing. Mool C. Gupta Applied Research Center Old Dominion University National Science Foundation Center for Lasers and Plasmas for Advanced Manufacturing Mool C. Gupta Applied Research Center Old Dominion University National Science Foundation Center - Center Mission -

More information

A novel High Average Power High Brightness Soft X-ray Source using a Thin Disk Laser System for optimized Laser Produced Plasma Generation

A novel High Average Power High Brightness Soft X-ray Source using a Thin Disk Laser System for optimized Laser Produced Plasma Generation A novel High Average Power High Brightness Soft X-ray Source using a Thin Disk Laser System for optimized Laser Produced Plasma Generation I. Mantouvalou, K. Witte, R. Jung, J. Tümmler, G. Blobel, H. Legall,

More information

Does the short pulse mode need energy recovery?

Does the short pulse mode need energy recovery? Does the short pulse mode need energy recovery? Rep. rate Beam power @ 5GeV 1nC @ 100MHz 500MW Absolutely 1nC @ 10MHz 1nC @ 1MHz 50MW 5MW Maybe 1nC @ 100kHz 0.5MW No Most applications we have heard about

More information

THE TUNABLE LASER LIGHT SOURCE C-WAVE. HÜBNER Photonics Coherence Matters.

THE TUNABLE LASER LIGHT SOURCE C-WAVE. HÜBNER Photonics Coherence Matters. THE TUNABLE LASER LIGHT SOURCE HÜBNER Photonics Coherence Matters. FLEXIBILITY WITH PRECISION is the tunable laser light source for continuous-wave (cw) emission in the visible and near-infrared wavelength

More information

High Repetition Rate Inverse Compton Scattering Source

High Repetition Rate Inverse Compton Scattering Source High Repetition Rate Inverse Compton Scattering Source W.S. Graves, F.X. Kaertner, D.E. Moncton March 2, 2010 Future Light Sources Workshop SLAC Charge from Organizers 1) Overview of the technology 2)

More information

FLASH performance after the upgrade. Josef Feldhaus

FLASH performance after the upgrade. Josef Feldhaus FLASH performance after the upgrade Josef Feldhaus European XFEL / HASYLAB Users Meeting DESY, January 27, 2011 Upgrade 2009 / 2010 > Upgrade shutdown: September 2009 February 2010 exchanged RF stations

More information

X-ray FEL Oscillator (XFEL-O) Gun Requirements and R&D Overview FLS2010: WG5: High Brightness Guns March 1, 2010

X-ray FEL Oscillator (XFEL-O) Gun Requirements and R&D Overview FLS2010: WG5: High Brightness Guns March 1, 2010 X-ray FEL Oscillator (XFEL-O) Gun Requirements and R&D Overview FLS2010: WG5: High Brightness Guns March 1, 2010 Nick Sereno (APS/ASD) - Argonne National Laboratory (ANL) / Advanced Photon source (APS)

More information

Feedback Requirements for SASE FELS. Henrik Loos, SLAC IPAC 2010, Kyoto, Japan

Feedback Requirements for SASE FELS. Henrik Loos, SLAC IPAC 2010, Kyoto, Japan Feedback Requirements for SASE FELS Henrik Loos, SLAC, Kyoto, Japan 1 1 Henrik Loos Outline Stability requirements for SASE FELs Diagnostics for beam parameters Transverse: Beam position monitors Longitudinal:

More information

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Approval: Originator: Tor Raubenheimer, Physics Support Lead Date Approved Approver: Marc Ross, Cryogenic System Manager Approver: Jose Chan,

More information

SNP High Performances IR Microchip Series

SNP High Performances IR Microchip Series SNP High Performances IR Microchip Series Key features Repetition rate up to 130kHz Ultrashort pulses down to 600ps Multi-kW peak power Excellent beam quality, M²

More information

Status of the Project

Status of the Project Status of the FERMI@Elettra Project Michele Svandrlik Elettra, Trieste, Italy IPAC 2012 New Orleans May 22 nd, 2012 OUTLINE FERMI@Elettra Overview Facility Performance Recent Progress Outlook and Conclusions

More information

Vitara. Automated, Hands-Free Ultrashort Pulse Ti:Sapphire Oscillator Family. Superior Reliability & Performance. Vitara Features:

Vitara. Automated, Hands-Free Ultrashort Pulse Ti:Sapphire Oscillator Family. Superior Reliability & Performance. Vitara Features: Automated, Hands-Free Ultrashort Pulse Ti:Sapphire Oscillator Family Vitara is the new industry standard for hands-free, integrated, ultra-broadband, flexible ultrafast lasers. Representing the culmination

More information

Electro-Optic Longitudinal Bunch Profile Measurements at FLASH: Experiment, Simulation, and Validation

Electro-Optic Longitudinal Bunch Profile Measurements at FLASH: Experiment, Simulation, and Validation Electro-Optic Longitudinal Bunch Profile Measurements at FLASH: Experiment, Simulation, and Validation Bernd Steffen, DESY FEL 2007 Novosibirsk, August 29th 2007 Electro-Optic Bunch Length Detection fs

More information

SNP High Performances IR Microchip Series

SNP High Performances IR Microchip Series SNP High Performances IR Microchip Series KEY FEATURES Repetition rate up to 130 khz Ultrashort pulses down to 600 ps Multi-kW peak power Excellent beam quality, M²

More information

FLASH II: an Overview

FLASH II: an Overview FLASH II: an Overview 1. Layout. 2. Status 1. Civil Construction 2. E-beamline 3. Photon Beamline 3. Timeplan 4. Finances 5. Personnel Situation 6. Simultaneous Operation of FLASH1 and 2 FLASH II is a

More information

Progress in High Gradient Accelerator Research at MIT

Progress in High Gradient Accelerator Research at MIT Progress in High Gradient Accelerator Research at MIT Presented by Richard Temkin MIT Physics and Plasma Science and Fusion Center May 23, 2007 MIT Accelerator Research Collaborators MIT Plasma Science

More information

Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark

Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark What is ISA? ISA operates and develops the storage ring ASTRID and related facilities ISA staff assist internal

More information

High power VCSEL array pumped Q-switched Nd:YAG lasers

High power VCSEL array pumped Q-switched Nd:YAG lasers High power array pumped Q-switched Nd:YAG lasers Yihan Xiong, Robert Van Leeuwen, Laurence S. Watkins, Jean-Francois Seurin, Guoyang Xu, Alexander Miglo, Qing Wang, and Chuni Ghosh Princeton Optronics,

More information

pulsecheck The Modular Autocorrelator

pulsecheck The Modular Autocorrelator pulsecheck The Modular Autocorrelator Pulse Measurement Perfection with the Multitalent from APE It is good to have plenty of options at hand. Suitable for the characterization of virtually any ultrafast

More information

picoemerald Tunable Two-Color ps Light Source Microscopy & Spectroscopy CARS SRS

picoemerald Tunable Two-Color ps Light Source Microscopy & Spectroscopy CARS SRS picoemerald Tunable Two-Color ps Light Source Microscopy & Spectroscopy CARS SRS 1 picoemerald Two Colors in One Box Microscopy and Spectroscopy with a Tunable Two-Color Source CARS and SRS microscopy

More information

Beam Instability Investigations at DELTA

Beam Instability Investigations at DELTA 10 th ESLS-RF Meeting, September 27-28, Dortmund Beam Instability Investigations at Thomas Weis for the group Dortmund University Synchrotron Radiation Center Content: Status of the Facility Instability

More information

Advanced Laser Personnel Safety System at Jefferson Lab

Advanced Laser Personnel Safety System at Jefferson Lab Advanced Laser Personnel Safety System at Jefferson Lab 2012 DOE Laser Safety Officer Workshop Stanford Linear Accelerator Center, Sept. 11-13 2012 Stephen Benson and Kevin Jordan, Newport News VA What

More information

Behavior of the TTF2 RF Gun with long pulses and high repetition rates

Behavior of the TTF2 RF Gun with long pulses and high repetition rates Behavior of the TTF2 RF Gun with long pulses and high repetition rates J. Baehr 1, I. Bohnet 1, J.-P. Carneiro 2, K. Floettmann 2, J. H. Han 1, M. v. Hartrott 3, M. Krasilnikov 1, O. Krebs 2, D. Lipka

More information

Electron Beam Diagnosis Using K-edge Absorp8on of Laser-Compton Photons

Electron Beam Diagnosis Using K-edge Absorp8on of Laser-Compton Photons LLNL-PRES-740689 Electron Beam Diagnosis Using K-edge Absorp8on of Laser-Compton Photons Y. Hwang 1, D. J. Gibson 2, R. A. Marsh 2, T. Tajima 1, C. P. J. Barty 1 1 University of California, Irvine 2 Lawrence

More information

Aurora II Integra OPO Integrated Nd:YAG Pumped Type II BBO OPO

Aurora II Integra OPO Integrated Nd:YAG Pumped Type II BBO OPO L i t r o n T o t a l L a s e r C a p a b i l i t y Aurora II Integra OPO Integrated Nd:YAG Pumped Type II BBO OPO The Litron Aurora II Integra is an innovative, fully motorised, type II BBO OPO and Nd:YAG

More information

Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors

Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors V.A. Dolgashev, P. Emma, M. Dal Forno, A. Novokhatski, S. Weathersby SLAC National Accelerator Laboratory FEIS 2: Femtosecond Electron

More information

TECHNICAL CHALLENGES OF THE LCLS-II CW X-RAY FEL *

TECHNICAL CHALLENGES OF THE LCLS-II CW X-RAY FEL * TECHNICAL CHALLENGES OF THE LCLS-II CW X-RAY FEL * T.O. Raubenheimer # for the LCLS-II Collaboration, SLAC, Menlo Park, CA 94025, USA Abstract The LCLS-II will be a CW X-ray FEL upgrade to the existing

More information

Beam Arrival Time Monitors. Josef Frisch, IBIC Sept. 15, 2015

Beam Arrival Time Monitors. Josef Frisch, IBIC Sept. 15, 2015 Beam Arrival Time Monitors Josef Frisch, IBIC Sept. 15, 2015 Arrival Time Monitors Timing is only meaningful relative to some reference, and in general what matters is the relative timing of two different

More information

ignis TECHNICAL DATA SHEET high specification red laser CW 660nm laser Extremely low noise Power 500mW

ignis TECHNICAL DATA SHEET high specification red laser CW 660nm laser Extremely low noise Power 500mW CW 660nm laser Extremely low noise Power 500mW TECHNICAL DATA SHEET The high specification 660nm laser Overview The at 660nm and 500mW is among the most powerful and compact red lasers available today

More information

Continuum White Light Generation. WhiteLase: High Power Ultrabroadband

Continuum White Light Generation. WhiteLase: High Power Ultrabroadband Continuum White Light Generation WhiteLase: High Power Ultrabroadband Light Sources Technology Ultrafast Pulses + Fiber Laser + Non-linear PCF = Spectral broadening from 400nm to 2500nm Ultrafast Fiber

More information

1550 nm Programmable Picosecond Laser, PM

1550 nm Programmable Picosecond Laser, PM 1550 nm Programmable Picosecond Laser, PM The Optilab is a programmable laser that produces picosecond pulses with electrical input pulses. It functions as a seed pulse generator for Master Oscillator

More information

Fiber Laser Chirped Pulse Amplifier

Fiber Laser Chirped Pulse Amplifier Fiber Laser Chirped Pulse Amplifier White Paper PN 200-0200-00 Revision 1.2 January 2009 Calmar Laser, Inc www.calmarlaser.com Overview Fiber lasers offer advantages in maintaining stable operation over

More information

Power scaling of picosecond thin disc laser for LPP and FEL EUV sources

Power scaling of picosecond thin disc laser for LPP and FEL EUV sources Power scaling of picosecond thin disc laser for LPP and FEL EUV sources A. Endo 1,2, M. Smrz 1, O. Novak 1, T. Mocek 1, K.Sakaue 2 and M.Washio 2 1) HiLASE Centre, Institute of Physics AS CR, Dolní Břežany,

More information

Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series

Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series COMMERCIAL LASERS Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series Key Features 1319 or 1064 nm outputs available Fiber-coupled output Proven nonplanar ring oscillator (NPRO) design Superior

More information

A new picosecond Laser pulse generation method.

A new picosecond Laser pulse generation method. PULSE GATING : A new picosecond Laser pulse generation method. Picosecond lasers can be found in many fields of applications from research to industry. These lasers are very common in bio-photonics, non-linear

More information

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Overview ALICE (Accelerators and Lasers In Combined Experiments)

More information

190 nm (6.5 ev) Laser-ARPES. Laser ARPES using a Tunable ps UV Source

190 nm (6.5 ev) Laser-ARPES. Laser ARPES using a Tunable ps UV Source 190 nm (6. ev) Laser-ARPES Laser ARPES using a Tunable ps UV Source 1 190 nm (6. ev) UV Source Laser ARPES/ARUPS with a High-Power UV Source Tunable deep-uv pulses from 190... 21 nm (6.....77 ev) are available

More information

The Potential for the Development of the X-Ray Free Electron Laser

The Potential for the Development of the X-Ray Free Electron Laser The Potential for the Development of the X-Ray Free Electron Laser TESLA-FEL 2004-02 E.L. Saldin, E.A. Schneidmiller, and M.V. Yurkov Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, Hamburg,

More information

TIME-PRESERVING MONOCHROMATORS FOR ULTRASHORT EXTREME-ULTRAVIOLET PULSES

TIME-PRESERVING MONOCHROMATORS FOR ULTRASHORT EXTREME-ULTRAVIOLET PULSES TIME-PRESERVING MONOCHROMATORS FOR ULTRASHORT EXTREME-ULTRAVIOLET PULSES Luca Poletto CNR - Institute of Photonics and Nanotechnologies Laboratory for UV and X-Ray Optical Research Padova, Italy e-mail:

More information

Review of the THz Coherent Light Source in Uppsala as a new Swedish Research Facility

Review of the THz Coherent Light Source in Uppsala as a new Swedish Research Facility Review of the THz Coherent Light Source in Uppsala as a new Swedish Research Facility Members of the Review Panel Prof. Jerome Hastings LCLS Directorate (SLAC), 2575 Sand Hill Rd, MS 102, Menlo Park, CA

More information

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011 Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts

More information