Ultrafast Beams and Applications UBA July, 2017 Presenter: Arsham Yeremyan

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

Maria Smedh, Centre for Cellular Imaging. Maria Smedh, Centre for Cellular Imaging

pulsecheck The Modular Autocorrelator

Administrative details:

Romania and High Power Lasers Towards Extreme Light Infrastructure in Romania

APE Autocorrelator Product Family

Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy

Drive Laser State-of-the-art: Performance, Stability and Programmable Repetition Rate The Jefferson Lab Experience

FemtoFAB. Femtosecond laser micromachining system. tel fax Konstitucijos ave. 23C LT Vilnius, Lithuania

Ultrafast instrumentation (No Alignment!)

Spectral phase shaping for high resolution CARS spectroscopy around 3000 cm 1

The All New HarmoniXX Series. Wavelength Conversion for Ultrafast Lasers

Precision Cold Ablation Material Processing using High-Power Picosecond Lasers

Fiber Laser Chirped Pulse Amplifier

Beam Shaping in High-Power Laser Systems with Using Refractive Beam Shapers

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

High Power and Energy Femtosecond Lasers

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

Pulse Shaping Application Note

A new picosecond Laser pulse generation method.

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

VELA PHOTOINJECTOR LASER. E.W. Snedden, Lasers and Diagnostics Group

TRAINING MANUAL. Multiphoton Microscopy LSM 510 META-NLO

High-Power Femtosecond Lasers

Ultrafast Lasers with Radial and Azimuthal Polarizations for Highefficiency. Applications

Femtosecond Laser Simulation Facility for SEE IC Testing

SUPPLEMENTARY INFORMATION

TIME-PRESERVING MONOCHROMATORS FOR ULTRASHORT EXTREME-ULTRAVIOLET PULSES

You won t be able to measure the incident power precisely. The readout of the power would be lower than the real incident power.

High Rep-Rate KrF Laser Development and Intense Pulse Interaction Experiments for IFE*

Designing for Femtosecond Pulses

Integrated disruptive components for 2µm fibre Lasers ISLA. 2 µm Sub-Picosecond Fiber Lasers

Bioimaging of cells and tissues using accelerator-based sources

Theoretical Approach. Why do we need ultra short technology?? INTRODUCTION:

TIGER Femtosecond and Picosecond Ti:Sapphire Lasers. Customized systems with SESAM technology*

Microprobe-enabled Terahertz sensing applications

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

LMT F14. Cut in Three Dimensions. The Rowiak Laser Microtome: 3-D Cutting and Imaging

Midaz Micro-Slab DPSS Lasers:

CHAPTER 7. Waveguide writing in optimal conditions. 7.1 Introduction

5kW DIODE-PUMPED TEST AMPLIFIER

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

combustion diagnostics

Fast Raman Spectral Imaging Using Chirped Femtosecond Lasers

Continuum White Light Generation. WhiteLase: High Power Ultrabroadband

Laser systems for science instruments

SNV/U High Performances UV Microchip Series

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

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

HEO 1080P APPLICATION NOTE

Chad A. Husko 1,, Sylvain Combrié 2, Pierre Colman 2, Jiangjun Zheng 1, Alfredo De Rossi 2, Chee Wei Wong 1,

Title: Laser marking with graded contrast micro crack inside transparent material using UV ns pulse

ULTRAFAST LASER DIAGNOSTICS

Imaging Retreat - UMASS Customized real-time confocal and 2-photon imaging

taccor Optional features Overview Turn-key GHz femtosecond laser

dnx/dt = -9.3x10-6 / C dny/dt = -13.6x10-6 / C dnz/dt = ( λ)x10-6 / C

NL300 series. Compact Flash-Lamp Pumped Q-switched Nd:YAG Lasers FEATURES APPLICATIONS NANOSECOND LASERS

Pockels Cells. Selection Guide. BBO Pockels Cells page 3.4. DQ High Repetition Rate Pockels Cell Driver for Q-Switching page 3.6

Application of EOlite Flexible Pulse Technology. Matt Rekow Yun Zhou Nicolas Falletto

Pockels Cells. Selection Guide. KD*P Pockels Cells page 3.3. DQ High Repetition Rate Pockels Cell Driver for Q-Switching page 3.6

Multiphoton Microscopy

Dr. Rüdiger Paschotta RP Photonics Consulting GmbH. Competence Area: Fiber Devices

LCLS-II-HE Instrumentation

SUPPLEMENTARY INFORMATION

STUDIES OF INTERACTION OF PARTIALLY COHERENT LASER RADIATION WITH PLASMA

Working in Visible NHMFL

PITZ Laser Systems. Light Amplification by Stimulated Emission of Radiation. Cavity. What is a Laser? General introduction: systems, layouts

Femtosecond to millisecond transient absorption spectroscopy: two lasers one experiment

3D light microscopy techniques

Practical Applications of Laser Technology for Semiconductor Electronics

Impact of the light coupling on the sensing properties of photonic crystal cavity modes Kumar Saurav* a,b, Nicolas Le Thomas a,b,

High Average Power, High Repetition Rate Side-Pumped Nd:YVO 4 Slab Laser

FR-103 WS AUTO/CROSSCORRELATOR

APPLICATION NOTE. Timing and Recombination Unit (TRU) for Time-Resolved Spectroscopy and Multiphoton Microscopy

High power UV from a thin-disk laser system

Fast, Two-Dimensional Optical Beamscanning by Wavelength Switching T. K. Chan, E. Myslivets, J. E. Ford

Development of Nano Second Pulsed Lasers Using Polarization Maintaining Fibers

Basics of confocal imaging (part I)

k λ NA Resolution of optical systems depends on the wavelength visible light λ = 500 nm Extreme ultra-violet and soft x-ray light λ = 1-50 nm

R. J. Jones Optical Sciences OPTI 511L Fall 2017

The Department of Advanced Materials Engineering. Materials and Processes in Polymeric Microelectronics

Laser Induced Damage Threshold of Optical Coatings

Micromachining of packaging materials for MEMS using lasers

J-KAREN-P Session 1, 10:00 10:

DCS laser for Thomson scattering diagnostic applications

Solea. Supercontinuum Laser. Applications

SENSOR+TEST Conference SENSOR 2009 Proceedings II

Development of near and mid-ir ultrashort pulse laser systems at Q-Peak. Evgueni Slobodtchikov Q-Peak, Inc.

Spider Pulse Characterization

Why and How? Daniel Gitler Dept. of Physiology Ben-Gurion University of the Negev. Microscopy course, Michmoret Dec 2005

Optimization of supercontinuum generation in photonic crystal fibers for pulse compression

Fabrication of Probes for High Resolution Optical Microscopy

Recent Progress on the 10PW laser Project at SIOM

Faraday Rotators and Isolators

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS

- Near Field Scanning Optical Microscopy - Electrostatic Force Microscopy - Magnetic Force Microscopy

Nanonics Systems are the Only SPMs that Allow for On-line Integration with Standard MicroRaman Geometries

:... resolution is about 1.4 μm, assumed an excitation wavelength of 633 nm and a numerical aperture of 0.65 at 633 nm.

TCSPC at Wavelengths from 900 nm to 1700 nm

G. Norris* & G. McConnell

Transcription:

Laser driven facility for irradiation experiments, two-photon microscopy and microfabrication Ultrafast Beams and Applications UBA17 04-07 July, 2017 Presenter: Arsham Yeremyan

Outline Parallel operation of AREAL linac and DELTA stations Femtosecond laser system: specs and features Beam delivery schemes, control and measurements Research fields and experimental capabilities Laser driven microscopy and microfabrication stations Fields of applications and multidisciplinary research capabilities Upcoming upgrades and extensions Applications Summary Tunable laser, THz spectroscopy, pulse-picking

Laser Driven Experimental Stations DELTA 2-photon microscope 250 fs, 50 MHz 1030 nm, 20nJ 0.4--8 ps, 1 100k Hz 1030 nm, 1.8 mj ufab 250 fs, 50 MHz 1030 nm, 25nJ Osc Ampl FHG 0.4--8 ps, 1--100 Hz 258 nm, 425uJ AREAL LASER

Laser Driven Experimental Stations Femtosecond Laser System Measurements and control IR and UV pulse profile monitoring (Spiricon) Energy/Power measurements Pulse-width variation and autocorrelator measurement

Laser Driven Experimental Stations Femtosecond Laser System Specifications and features t-pulse S-pulse FHG SHG* THG* Wavelength 1030 nm 1030 nm 258 nm 515 nm 343 nm Pulse width 250 fs 400 fs--8 ps 400 fs --8 ps 400 fs--8 ps 1 8 ps Rep. Rate 50 MHz 1-100K Hz 1-1K Hz 1-100K Hz 1 100K Hz Energy/pulse 20 nj Up to 2 mj Up to 425 uj Up to 1mJ * Conversion implemented in DELTA ufab Synchronization with Master Oscillator Remote control IR and UV pulse-to-pulse energy stability ~0.5 %

Laser Driven Experimental Stations DELTA 2-photon microscope 0.4--8 ps, 1 100k Hz 1030 nm 234 fs, 50 MHz 1030 nm ufab Osc 234 fs, 50 MHz 1030 nm Ampl FHG 0.4--8 ps, 1--100 Hz 258 nm AREAL LASER

Electron irradiation experiments on AREAL linac Experiments Dose-rate effects on DNA, radiation-induced defects in semiconductors, dielectrics, ferroelectrics, etc. Groups Yerevan State Univ Polytechnic Univ. Yerevan Phys. Inst Inst. Mol. Biology Inst. Phys. Research CANDLE Institute Fields Genetics Biology Molecular Physics Microelectronics Solid State Physics New materials

DELTA EXPERIMENTAL STATIONS Two-Photon Microscopy: Basics Advantages more sensitive than Confocal Laser Microscopy Longer wavelength penetrates deeper Higher resolution Better signal-to-noise ratio, other

DELTA EXPERIMENTAL STATIONS DELTA Two-Photon Microscope: Features Sutter Instruments Galvano-scanning system Multi-channel measurements with different filters and PMTs 3D-acquisition capability, etc. Operating Parameters Excitation: 1030 nm Fluorescence: >515 nm Energy per pulse: up to 20 nj Pulse length: 280 fs Intensity in focal plane: up to ~10 13 W/cm 2

DELTA EXPERIMENTAL STATIONS Two-Photon Microscopy Experiments Other. Interaction of lactobacteria and yeast Institute of Molecular Biology NAS RA Live brain imaging Groups CANDLE SRI Identification of dead and live soil microorganisms Yerevan State Medical University Armenian National Agrarian University/ International Association for Human and Animals Health Improvement A.I. Alikhanian National Science Laboratory (YerPhI) Institute for Physical Research NAS RA

DELTA EXPERIMENTAL STATIONS Two-Photon Microscopy Possibility of multiphoton excitation microscopy of inorganics Image scale: 200 x 200 um ZnO:Li - hydrothermal ZnO:Li solid phase growth ZnO:Er solid phase growth SHG microscopy of doped ZnO surface

DELTA EXPERIMENTAL STATIONS DELTA ufab station

DELTA EXPERIMENTAL STATIONS DELTA ufab station

DELTA EXPERIMENTAL STATIONS DELTA ufab station Operating Parameters Pulse duration: 400 fs 8 ps Repetition rate: 1 Hz 100 khz Average power: up to 8 W Pulse energy: up to 2 mj (1030 nm) and 1 mj (515 nm) Wavelengths 1030 nm, 515 nm, 343 nm Sample positioning accuracy: ±50 nm Travel range: 100 x 100 mm (XY), 25 mm (Z)

DELTA EXPERIMENTAL STATIONS Femtosecond laser processing of materials Ultrashort pulses new mechanisms of laser-matter interactions Suppression of heat diffusion to surrounding regions improvement of quality and spatial resolution for nanoscale fabrication High peak intensities nonlinear absorption Multiphoton absorption in transparent materials both surface (2D) and volume (3D) writing of micro- and nanostructures becomes feasible Processing of practically all materials: metals, semiconductors, glasses, polymers, ceramics, and biological samples

DELTA Microfabrication Femtosecond laser processing Typical Applications Direct laser writing, micromachining, laser-assisted deposition, 2D patterning Micro- and nanoelectronics Semiconductor technology, etc Bulk processing of transparent materials Microfluidics networks, waveguides, labs-on-a-chip 2-photon polymerization, ablation 3D photonic crystals, MEMS biomedical Other?!

EXPERIMENTAL STATIONS Upcoming upgrades and Extensions Ultrafast pulse picker Designed specifically for simultaneous operation of AREAL and ufab ufab To AREAL 1. Pockels cell 2. Driver 3. Polarizing beamsplitter 4. Waveplate N out of 50K pulses with switched polarization can be redirected from the train of amplifier output Sync with Master Oscillator

EXPERIMENTAL STATIONS Upcoming upgrades and Extensions Tunable femtosecond laser +Sync unit with MO cooperation with AVESTA (Russia) Ti:Sapphire, 750-950 nm, 100 fs, 80MHz Applications 2P-microscopy; extended range of fluorophores Time-resolved experiments other

EXPERIMENTAL STATIONS Upcoming upgrades and Extensions THz source + EO sampling THz spectrometer table-top, 1 to 100s nj/pulse (not a FEL); 0.5-2.3 THz 10 1 0.1 Arr ows S how th e Abs o rp tion o f Wa te r Va po r 0.01 1E -3 1E -4 0 1 2 3 4 5 6 THz Gen Basic scheme In cooperation with AVESTA (Russia) THz generation to be implemented at CANDLE

DELTA Microfabrication Current activities Fabrication of glass-based optical elements: Laser beam shaping elements fork gratings for optical vortex generation diffraction gratings 2-photon polymerization: Liquid-crystal alignment microstructures Micro-needles, cantilevers, microprobes Patterning of semiconductor and metallic surfaces: micro-contacts, nano-film patterning, photon electron beam apertures

DELTA Microfabrication Current activities Laser Beam Shaping Principle Conversion of laser irradiance distribution Gaussian Bessinc(r) or Airy disk Homogeneous (Flattop) Modulation of Gaussian with a proper phase function Far field (or f- plane of a lens)

DELTA Microfabrication Current activities Laser Beam Shaping Design and fabrication Design Parameters Wavelength Beam size Traveling (focal) distance Phase depth (0,π) binary phase function (concentric rings) are laserwritten IN/ON glass Integrated π-shaper

DELTA Microfabrication Current activities Laser Beam Shaping Results 2D Beam display 3D Beam display Applications HeNe TEM 00 p -Shaper Flattop Beam Laser fabrication technology Spatial-temporal beam shaping Features: High damage threshold Integration with a lens Efficiency >95 %

DELTA Microfabrication Current activities Optical Vortex Beams Potential Applications Optical communications Coronagraphy Micro-particle manipulation (optical tweezers) Beam shaping STED (2P-)microscopy Excitation beam quenching beam Fluorescence -allowing beam

DELTA Microfabrication Current activities Optical Vortex Beams Computer-generated Fork holograms as a source of phase singularities l=1 l=2 Features: Glass provides high damage threshold (critical with high power applications) Efficiency can be increased by fabrication of volume holograms Laser-written on glass

DELTA Microfabrication Current activities Optical Vortex Beams Results Screen l=1 CCD Optical vortex generation CGH Gaussian Beam vortex beam l=0 l=-1 CGH-Computer Generated Hologram laser-written ON/IN glass

DELTA Microfabrication Current activities Optical Vortex Beams Results Gaussian Beam CGH vorte x beam m=0 Interference pattern on CCD Readout of the topological charge m=-1 Computer Generated Fork cf.

DELTA Microfabrication Current activities More glass-based optical elements Relief diffraction gratings spiral Fiber diffraction grating Pulse shaping Applied to tilt the pump front for efficient THz generation

DELTA Microfabrication Current activities Two-photon polymerization Applications bio-medical: micro-needles for transdermal drug delivery, microelectrodes, etc. 3D photonic crystals Liquid crystal devices Micro-and nano-cantilevers, sensors MEMS (Micro- Electro-Mechanical Systems) Log pile

DELTA Microfabrication Current activities Surface patterning Matrix of holes on Mo thin film ZnO, d=600 nm Al, d=200 nm Applications micro-contacts nano-film patterning photon electron beam apertures nm 200 100 0-100 -200 200 225 250 275 300 mkm

Summary Fundamental, 2 nd, 3 rd and 4 th harmonics of femtosecond laser are used for parallel operation of 2-photon scanning microscope, microfabrication and linac stations This provides unique capability to perform a comprehensive chain of multidisciplinary experiments using ultrafast electron and photon beams Forthcoming supplements and developments are highlighted which will further extend the experimental capabilities A summary of results to demonstrate the diversity of potential applications Thank you