Moti Fridman 1, Alessandro Farsi 2 and Alexander L. Gaeta 2 1 School of Engineering, Bar Ilan University, Ramat Gan, 52900, Israel 2 School of Applied.

Slides:



Advertisements
Similar presentations
Today • Diffraction from periodic transparencies: gratings
Advertisements

Collinear interaction of photons with orbital angular momentum Apurv Chaitanya N Photonics science Laboratory, PRL.
Observation of the relativistic cross-phase modulation in a high intensity laser plasma interaction Shouyuan Chen, Matt Rever, Ping Zhang, Wolfgang Theobald,
KAPITZA-DIRAC EFFECT Eric Weaver Phys 4P62. General Outline  Theorized in 1933 by Kapitza and Dirac  Reflection of electrons from standing light waves.
Single-Shot Tomographic Imaging of Evolving, Light Speed Object Zhengyan Li, Rafal Zgadzaj, Xiaoming Wang, Yen-Yu Chang, Michael C. Downer Department of.
Quantum Coherent Control with Non-classical Light Department of Physics of Complex Systems The Weizmann Institute of Science Rehovot, Israel Yaron Bromberg,
1 Remote Engineered Super Resolved Imaging Zeev Zalevsky Faculty of Engineering, Bar-Ilan University, Ramat-Gan, Israel.
2004 CLEO/IQEC, San Francisco, May Optical properties of the output of a high-gain, self-amplified free- electron laser Yuelin Li Advanced Photon.
On Attributes and Limitations of Linear Optics in Computing A personal view Joseph Shamir Department of Electrical Engineering Technion, Israel OSC2009.
Dimitris Papazoglou Assistant Professor, Affiliated faculty IESL-FORTH Senior member of the UNIS group PhD: 1998, Aristotle University of Thessaloniki,
Generation of short pulses
EE 230: Optical Fiber Communication Lecture 13
Frequency Bistability in a Diode Laser Using Diffraction Gratings Forrest Smith 1, Weliton Soares 2, Samuel Alves 2, Itamar Vidal 2, Marcos Oria 2 1 State.
EE 230: Optical Fiber Communication Lecture 6 From the movie Warriors of the Net Nonlinear Processes in Optical Fibers.
Propagation in the time domain PHASE MODULATION n(t) or k(t) E(t) =  (t) e i  t-kz  (t,0) e ik(t)d  (t,0)
Using Atomic Diffraction to Measure the van der Waals Coefficient for Na and Silicon Nitride J. D. Perreault 1,2, A. D. Cronin 2, H. Uys 2 1 Optical Sciences.
Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview = 4WM.
Using Atomic Diffraction to Measure the van der Waals Coefficient for Na and Silicon Nitride J. D. Perreault 1,2, A. D. Cronin 2, H. Uys 2 1 Optical Sciences.
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
First year talk Mark Zentile
Pump-Probe Spectroscopy Chelsey Dorow Physics 211a.
Space-time analogy True for all pulse/beam shapes Paraxial approximation (use of Fourier transforms) Gaussian beams (q parameters and matrices) Geometric.
FWM IN SILICON NANOWIRE & MULTICORE FIBER COUPLING
ARRAYED WAVEGUIDE GRATINGS
1/9/2007Bilkent University, Physics Department1 Supercontinuum Light Generation in Nano- and Micro-Structured Fibers Mustafa Yorulmaz Bilkent University.
Arbitrary nonparaxial accelerating beams and applications to femtosecond laser micromachining F. Courvoisier, A. Mathis, L. Froehly, M. Jacquot, R. Giust,
A 5 fs high average power OPCPA laser system for attosecond pulse production Philip Bates, Yunxin Tang, Emma Springate and Ian Ross Central Laser Facility,
Entangled photon pair generation by spontaneous parametric down conversion Atsushi Yabushita Department of Electrophysics National Chiao-Tung University.
Fourier relations in Optics Near fieldFar field FrequencyPulse duration FrequencyCoherence length Beam waist Beam divergence Focal plane of lensThe other.
Yen-Yu Chang, Li-Chung Ha, Yen-Mu Chen Chih-Hao Pai Investigator Jypyng Wang, Szu-yuan Chen, Jiunn-Yuan Lin Contributing Students Institute of Atomic and.
Wong group, Optical Nanostructures Laboratory, Columbia UniversityXiujian Li Phase Conjugation in Silicon waveguide.
Trivia Question Where is the largest laser system in the world? (a) Andrews Air Force Base (b) USS Enterprise (c) Area 51, located in ???? (d) Sandia National.
Shaping Pulses Before They are Born Avi Pe’er Physics Department and BINA center for nano-technology, Bar Ilan University FRISNO 11 Shai Yefet, Naaman.
Time lens Zhengran L.B.R Tuesday, April 23, 2013.
NONLINEAR PROPAGATION
Shortening a laser pulse at the focus of a lens Yuelin Li Accelerator Systems Division Argonne National Laboratory
Institute of Atomic and Molecular Sciences, Academia Sinica, Taiwan National Taiwan University, Taiwan National Central University, Taiwan National Chung.
R. Kupfer, B. Barmashenko and I. Bar
Quantum Optics II – Cozumel, Dec. 6-9, 2004
Pulse Shaping with MIIPS SASS 8/22/2012 David Nicholson.
QUEST - Centre for Quantum Engineering and Space-Time Research Multi-resonant spinor dynamics in a Bose-Einstein condensate Jan Peise B. Lücke, M.Scherer,
Nonlinear Optics Lab. Hanyang Univ. Chapter 6. Processes Resulting from the Intensity-Dependent Refractive Index - Optical phase conjugation - Self-focusing.
Highly efficient Raman fiber laser Collaborators: E. Bélanger M. Bernier B. Déry D. Faucher Réal Vallée.
Observation of Backwards Pulse Propagation in Erbium Doped Fiber George Gehring 1, Aaron Schweinsberg 1, Christopher Barsi 2, Natalie Kostinski 3, Robert.
Space-time analogy True for all pulse/beam shapes
Quantum Imaging MURI Kick-Off Meeting Rochester, June 9-10, Entangled state and thermal light - Foundamental and applications.
Terahertz Imaging with Compressed Sensing and Phase Retrieval Wai Lam Chan Matthew Moravec Daniel Mittleman Richard Baraniuk Department of Electrical and.
Gaussian pulses Bandwidth limited: Pulse duration FWHM Fourier transform Bandwidth duration product Chirped Gaussian Fourier Transform.
Appendix A : Fourier transform
QUANTUM OPTICS LAB IAP, UNIVERSITÄT BERN Qudit Implementations with Energy-Time Entangled Photons 1 Bänz Bessire Quantum Optics Lab – The Stefanov Group.
Observation of Quantum Beating in Rubidium at 2. 1 THz and 18
Four wave mixing in submicron waveguides
Group and phase velocity matching in THz IFEL interaction
Date of download: 10/20/2017 Copyright © ASME. All rights reserved.
Spontaneous Parametric Down Conversion
Laboratoire d’Optique Appliquée
Principle of Mode Locking
Thin film Interference
Tunable Slow Light in Cesium Vapor
Frequency vs. Time: Chirp
Stabilizing the Carrier-Envelope Phase of the Kansas Light Source
Study of linear propagation
Observational Astronomy
Interference P47 – Optics: Unit 6.
Scalar theory of diffraction
SPACE TIME Fourier transform in time Fourier transform in space.
Space-time analogy True for all pulse/beam shapes
Temporal optical differentiators (ODs) realized by using a LPG  
SPACE TIME Fourier transform in time Fourier transform in space.
Fig. 1 Experimental setup.
Presentation transcript:

Moti Fridman 1, Alessandro Farsi 2 and Alexander L. Gaeta 2 1 School of Engineering, Bar Ilan University, Ramat Gan, 52900, Israel 2 School of Applied and Engineering Physics, Cornell University, Ithaca, NY 14853, USA Multistage Accelerating Beams

Caustics Menaechmus ~ 400 BC

Accelerating beam of light G. A. Siviloglou et. al. (2007)

Accelerating beam in space Input beam Mask imposing cubic phase Accelerating beam Lens

Accelerating beam of electrons N. V. Bloch et. al. (2012)

Akhmanov, Sukhorukov, and Chirkin, Sov. Phys. - JETP, 28, 748, (1969). Kolner, IEEE J. Quantum Electron. 30, 1951 (1994). Optical processing based on time-space duality Spatial diffraction  Dispersive propagation Spatial domain Temporal domain x z z diffraction dispersive broadening

Imaging in space Imaging achieved by adding a quadratic phase to wavefront. lens quadratic phase shift in space

Temporal imaging Imaging achieved by adding a quadratic phase to the signal. quadratic phase shift in time dispersive elements

Accelerating beam in time cubic phase shift in time and a lens dispersion

Parametric mixing with a quadratic chirped pump D quadratic frequency shift Quadratic dispersion pump pulse Look for interaction that imparts quadratic phase shift. Imposing cubic phase in time

Pump Diffracting grating

Reflecting stairs

Accelerating beam in time

Multistage accelerating beam FWM Stage 1 signal idler

Multistage accelerating beam FWM Stage 1 FWM signal idler Idler #2 Stage 2

Experimental setup

Accelerating beam in time

Multistage accelerating beam in time

Conclusions Accelerating beam in time. Multistage acceleration. More complex dispersion relations. Space-time equivalent can open a rout for many more novel demonstrations.