Workshop on High-Field THz Science High Power THz Generation and THz Field Enhancement in Nanostructures Fabian Brunner 1, Salvatore Bagiante 2, Florian.

Slides:

Advertisements

Similar presentations

Λ1λ1 λ2λ2 2λ22λ2 λ1λ1 λ2λ2 2λ22λ2 Enhancement of Second-Harmonic Generation through Plasmon Resonances in Silver Nanorods Nicholas Wang 1, Patrick McAvoy.

Advertisements

"NANO-ACOUSTICS AND TERAHERTZ ACOUSTICS"

The Sum Over States model, although exact, requires a detailed knowledge of many parameters which are not generally available. Experience has shown that.

Transient Four-Wave Mixing Spectroscopy on PbS Quantum Dots Kevin Blondino (Florida State University) Advisors: Dr. Denis Karaiskaj, USF (faculty) Jason.

OUTLINE Introduction „Tera-to-Nano“: Our Novel Near-Field Antenna 80 GHz CW Frequency Domain Measurements Picosecond Pulse Time Domain Measurements 2D.

Positronium Rydberg excitation in AEGIS Physics with many positrons International Fermi School July 2009 – Varenna, Italy The experimental work on.

Janez Žabkar Advisers: dr. Marko Zgonik dr. Marko Marinček

Generation of short pulses

Materials in Extreme THz Fields Valery Dolgashev Hermann Duerr Shambhu Ghimire Hirohito Ogasawara Haidan Wen Aaron Lindenberg.

Third harmonic imaging of plasmonic nanoantennas

First THz Measurements at FACET Ziran Wu, Alan Fisher, Henrik Loos FACET 2011 Users Meeting

2. High-order harmonic generation in gases Attosecond pulse generation 1. Introduction to nonlinear optics.

Introduction to Nonlinear Optics

ARC 11/02/10 Recent Advances in Surface Plasmon Resonance: From Biosensor to Space/astronomical Interest Hololab and CSL S. Habraken, C. Lenaerts, and.

Ultrabroadband terahertz generation using DAST single crystal

Neutron Generation and Detection Lee Robertson Instrument & Source Division Oak Ridge National Laboratory 17 th National School on Neutron and X-ray Scattering.

Chapter 8. Second-Harmonic Generation and Parametric Oscillation

30. Nov I.Will, G. Klemz, Max Born Institute: Optical sampling system Optical sampling system for detailed measurement of the longitudinal pulse.

1Ruđer Bošković Institute, Zagreb, Croatia

Physical Phenomena for TeraHertz Electronic Devices

Solid-state Compact Blue-green Lasers: Research and Development; Practical Implementation and Applications in Science and Technology Stepan Essaian Spectralus.

Picosecond needs for phonon dynamics in nanoscience / energy science Yuelin Li, X-ray Science Division, Argonne National Laboratory.

1 ST workshop 2005 Numerical modeling and experimental study of ICR heating in the spherical tokamak Globus-M O.N.Shcherbinin, F.V.Chernyshev, V.V.Dyachenko,

High efficiency generation and detection of terahertz pulses using laser pulses at tele- communication wavelengths A.Schneider et al. OPTICS EXPRESS 5376/Vol.14,No.12(2006)

Christopher Devulder, Slava V. Rotkin 1 Christopher Devulder, Slava V. Rotkin 1 1 Department of Physics, Lehigh University, Bethlehem, PA INTRODUCTION.

Spectroscopic Line Shapes Of Broad Band Sum Frequency Generation Himali Jayathilake Igor Stiopkin, Champika Weeraman, Achani Yatawara and Alexander Benderskii.

Nuclear Magnetic Resonance Spectroscopy Dr. Sheppard Chemistry 2412L.

T. Smoleński 1, M. Goryca 1,2, T. Kazimierczuk 1, J. A. Gaj 1, P. Płochocka 2, M. Potemski 2,P. Wojnar 3, P. Kossacki 1,2 1. Institute of Experimental.

FYRIRLESTRAMARAÞON HR 2011 | RU LECTURE MARATHON 2011 Ágúst Valfells Science and Engineering SIZE MATTERS –ELECTRON BEAMS AT THE MICROSCALE.

Applications of Quantum Physics

1 Components of Optical Instruments Lecture Silicon Diode Transducers A semiconductor material like silicon can be doped by an element of group.

Photo-induced ferromagnetism in bulk-Cd 0.95 Mn 0.05 Te via exciton Y. Hashimoto, H. Mino, T. Yamamuro, D. Kanbara, A T. Matsusue, B S. Takeyama Graduate.

Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Controlling light with light.

Sarah Newton University of Oregon Applied Physics.

Compton/Linac based Polarized Positrons Source V. Yakimenko BNL IWLC2010, Geneva, October 18-22, 2010.

Design Considerations for a High-Efficiency High-Gain Free-Electron Laser for Power Beaming C. Muller and G. Travish UCLA Department of Physics & Astronomy,

Transverse Profiling of an Intense FEL X-Ray Beam Using a Probe Electron Beam Patrick Krejcik SLAC National Accelerator Laboratory.

Itoh Lab. M1 Masataka YASUDA

Advanced semiconductor detectors of neutrons

Terahertz Applications by THz Time Domain Spectroscopy

A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.

Surface Plasmon Resonance

SEM- Schematic Overview. Electron Detection Tungsten Filament Electron Source.

Enhancing the Macroscopic Yield of Narrow-Band High-Order Harmonic Generation by Fano Resonances Muhammed Sayrac Phys-689 Texas A&M University 4/30/2015.

High frequency hopping conductivity in semiconductors. Acoustical methods of research. I.L.Drichko Ioffe Physicotechnical Institute RAS Физико-технический.

Nonlinear Optical Response of Nanocavities in Thin Metal Films Yehiam Prior Department of Chemical Physics Weizmann Institute of Science With Adi Salomon.

NIRT: Semiconductor nanostructures and photonic crystal microcavities for quantum information processing at terahertz frequencies M. S. Sherwin and P.

Switching with Ultrafast Magnetic Field Pulses Ioan Tudosa.

Metal-insulator-metal metamaterial absorbers consisting of proximity-coupled resonators with the control of the fundamental and the second-order frequencies.

Pushing the space charge limit in the CERN LHC injectors H. Bartosik for the CERN space charge team with contributions from S. Gilardoni, A. Huschauer,

Controlled fabrication and optical properties of one-dimensional SiGe nanostructures Zilong Wu, Hui Lei, Zhenyang Zhong Introduction Controlled Si and.

Lez. 6 - Fisica At. Mol. Spec Carlo Altucci Consorzio Nazionale Interuniversitario di Struttura della Materia – CNISM Dipartimento di Scienze.

Conclusion QDs embedded in micropillars are fabricated by MOCVD and FIB post milling processes with the final quality factor about Coupling of single.

Measurement of 400 MeV Proton Beam Intensity and Transmission Through Collimator of HPRF Cavity at Fermilab MuCool Test Area M. R. Jana 1, M. Chung 1,

Introduction to Laser Spectroscopic Techniques for Condensed Matter.

Transverse Coherent Transition Radiation (TCTR) Experiment First Ideas for a Measurement Setup Max-Planck-Institute for Physics Munich Olaf Reimann, Scott.

All-Dielectric Metamaterials: A Platform for Strong Light-Matter Interactions Jianfa Zhang* （College of Optoelectronic Science and Engineering, National.

Coherent THz radiation source driven by pre-bunched electron beam

Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.

Ultra broadband plasmonic absorbers for terahertz waves

The 2nd European Advanced Accelerator Concepts Workshop

Spectral methods for measurement of longitudinal beam profile

Tunable Electron Bunch Train Generation at Tsinghua University

Performance of the prototype THz-driven electron gun for the AXSIS project. Grygorii Vashchenko R. Assmann, U. Dorda, M. Fakhari, A. Fallahi, K. Galaydych,

Muhammed Sayrac Phys-689 Modern Atomic Physics Spring-2016

Optical and Terahertz Spectroscopy of CdSe/ZnS Quantum Dots

Terahertz Spectroscopy of CdSe Quantum Dots

Soft X-ray Absorption and Coherence Analysis

Compact linear accelerator FLUTE: status update

Pump and probe technique

Presentation transcript:

Workshop on High-Field THz Science High Power THz Generation and THz Field Enhancement in Nanostructures Fabian Brunner 1, Salvatore Bagiante 2, Florian Enderli 1, Justyna Fabianska 1, and Thomas Feurer 1 1 Institute of Applied Physics, University of Bern, Switzerland 2 Laboratory for Micro- and Nanotechnology, Paul Scherrer Institut, Switzerland

Outline > Introduction: Applications of strong electric and magnetic fields at THz frequencies > Generation of intense THz pulses in nonlinear optical crystals > THz field enhancement in metallic nanostructures > THz SHG in lithium niobate crystals > Conclusions Outline2

Applications of strong electric and magnetic fields at THz frequencies > Nonlinear optics at THz frequencies (bulk semiconductors, quantum dots, …) > Direct excitation of transverse optical phonons or anti- ferromagnetic spin waves > Acceleration of charged particles and measurements of electron bunch profiles (THz streak camera) > Single shot imaging > … Introduction3

Efficient THz generation in NLO crystals: Requirements for the crystals > A large tensor element of the nonlinear optical susceptibility > Low linear and nonlinear optical absorption > Low THz absorption > Phase-matching: —collinear: (organic nonlinear optical crystals: DAST, OH1,…) —Cherenkov-type: (LiNbO 3 ) THz generation in nonlinear optical crystals4

High power THz time-domain spectroscopy 5

Comparison of laser-based methods for THz pulse generation 6

Peak electric field vs. pulse energy Assumptions: > Single cycle pulse > Focusing with F# = 1 7

Non-resonant enhancement: array of slits 8 Gold slit array on silicon Typical field enhancement of a slit

Ideal periodicity of slit array > most effective harvesting of incident field 9 > Nonlinear signal: trade-off between volume of high field strength and high field enhancement

Resonant enhancement: Split ring resonators nm

Second harmonic generation in LiNbO 3 Simulated spectra of transmitted pulses 11 Fabrication of the sample

Conclusions > Combination of high power THz source with local field enhancement enables new experiments > Fabrication of gold nano-structures on silicon > New fabrication process for gold nano-slits filled with lithium niobate > Simulation of SHG spectra and optimization of geometry parameters for the highest conversion efficiency 12