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.

Slides:



Advertisements
Similar presentations
Diode UV Output Fiber M1 Nd:Van Q.S. M2Lens SHGTHG UV Filter Diode UV Output M1 Nd:Van Q.S. M2Lens SHGTHG Extracavity Intracavity Techniques for UV Tripling.
Advertisements

Description of a pulse train
Direct Frequency Comb Spectroscopy for the Study of Molecular Dynamics in the Infrared Fingerprint Region Adam J. Fleisher, Bryce Bjork, Kevin C. Cossel,
In Search of the “Absolute” Optical Phase
Components of ultrafast laser system
Quantum Coherent Control with Non-classical Light Department of Physics of Complex Systems The Weizmann Institute of Science Rehovot, Israel Yaron Bromberg,
Laser physics simulation program Lionel Canioni University Bordeaux I France.
Self-Guided Operation of Green-Pumped Singly Resonant
Tunable Laser Spectroscopy Referenced with Dual Frequency Combs International Symposium on Molecular Spectroscopy 2010 Fabrizio Giorgetta, Ian Coddington,
Results The optical frequencies of the D 1 and D 2 components were measured using a single FLFC component. Typical spectra are shown in the Figure below.
Space-time positioning at the quantum limit with optical frequency combs Workshop OHP September 2013 Valérian THIEL, Pu JIAN, Jonathan ROSLUND, Roman SCHMEISSNER,
Samansa Maneshi, Jalani Kanem, Chao Zhuang, Matthew Partlow Aephraim Steinberg Department of Physics, Center for Quantum Information and Quantum Control,
Generation of short pulses Jörgen Larsson, Fysiska Instutionen Lunds Tekniska Högskola.
Dylan Yost, Arman Cingoz, Tom Allison and Jun Ye JILA, University of Colorado Boulder Collaboration with Axel Ruehl, Ingmar Hartl and Martin Fermann IMRA.
Characterization and optimization of entangled states produced by a self-phase-locked OPO J. Laurat, G. Keller, J.A.O. Huguenin T. Coudreau, N. Treps,
Narrow transitions induced by broad band pulses  |g> |f> Loss of spectral resolution.
Ultrafast Spectroscopy
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
1 09:05-09:55 am, Wednesday, September 22, 2010 CHEM 8152: Analytical Spectroscopy Smith 1111, University of Minnesota Resonant cavities Gain Threshold.
All-Fiber Optical Parametric Oscillator (FOPO) Chengao Wang.
Angus Henderson, Paul Hoffman and Ryan Stafford
Time-Bandwidth Products getting the average power of ultrafast DPSS lasers from hundreds of mW to tens of Watts by Dr. Thomas Ruchti CERN, April 2006 SESAM.
Ultrafast Experiments Hangwen Guo Solid State II Department of Physics & Astronomy, The University of Tennessee.
High power ultrafast fiber amplifiers Yoann Zaouter, E. Cormier CELIA, UMR 5107 CNRS - Université de Bordeaux 1, France Stephane Gueguen, C. Hönninger,
Masters Course: Experimental Techniques Detection of molecular species (with lasers) Techniques Direct absorption techniques Cavity Ring Down Cavity Enhanced.
NOISE IN OPTICAL SYSTEMS F. X. Kärtner High-Frequency and Quantum Electronics Laboratory University of Karlsruhe.
High Harmonic Generation in Gases Muhammed Sayrac Texas A&M University.
Spectroscopy with comb-referenced diode lasers
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
Tunable Mid-IR Frequency Comb for Molecular Spectroscopy
Interaction of radiation with atoms and ions (I) Absorption- Stimulated emission E1E1 E2E2 W 12 =W 21 Spontaneous emission More definitionsCross section.
Intra-cavity Pulse Shaping of Mode-locked Oscillators Shai Yefet, Naaman Amer and Avi Pe’er Department of physics and BINA Center of nano-technology, Bar-Ilan.
Sub-Doppler Spectroscopy of Molecular Ions in the Mid-IR James N. Hodges, Kyle N. Crabtree, & Benjamin J. McCall WI06 – June 20, 2012 University of Illinois.
Lasers and RF-Timing Franz X. Kaertner
__–––– Sensitivity Scaling of Dual Frequency Combs Ian Coddington, Esther Baumann, Fabrizio Giorgetta, William Swann, Nate Newbury NIST, Boulder, CO
Lineshape and Sensitivity of Spectroscopic Signals of N 2 + in a Positive Column Collected Using NICE-OHVMS Michael Porambo, Andrew Mills, Brian Siller,
Fourier-transform coherent anti-Stokes Raman scattering microscopy Jennifer P. Ogilvie et al. Opt. Lett. 31, 480 (2006) Kazuya MORI MIYASAKA Lab.
Lineshape and Sensitivity of Spectroscopic Signals of N 2 + in a Positive Column Collected Using NICE-OHVMS Michael Porambo, Andrew Mills, Brian Siller,
Femtosecond Laser Spectroscopy of C 60 Nieuwegein, The Netherlands August 21, 2001 Eleanor Campbell, Göteborg University & Chalmers, Sweden R.D. Levine,
Pulse Shaping with MIIPS SASS 8/22/2012 David Nicholson.
Measuring the Wave-Function of Broadband Bi-Photons
Development of high-power and stable laser for gravitational wave detection Mio Laboratory Kohei Takeno.
We have experimentally observed a similar qualitative behavior by measuring the ratio between the CW and ML intra-cavity powers as a function of Z for.
Kerr-lens Mode Locking Without Nonlinear Astigmatism Shai Yefet, Valery Jouravsky and Avi Pe’er Physics Department and the Institute of Nanotechnology.
Development of a System for High Resolution Spectroscopy with an Optical Frequency Comb Dept. of Applied Physics, Fukuoka Univ., JST PRESTO, M. MISONO,
Operated by Los Alamos National Security, LLC for NNSA Dynamics of modulated beams Operated by Los Alamos National Security, LLC, for the U.S. Department.
Highly efficient Raman fiber laser Collaborators: E. Bélanger M. Bernier B. Déry D. Faucher Réal Vallée.
Workshop for advanced THz and Compton X-ray generation
Tze-Wei Liu Y-C Hsu & Wang-Yau Cheng
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
Multimode quantum optics Nicolas Treps Claude Fabre Gaëlle Keller Vincent Delaubert Benoît Chalopin Giuseppe Patera Virginia d’Auria Jean-François Morizur.
“Finding” a Pulse Shape
Space-time analogy True for all pulse/beam shapes
INDIRECT TERAHERTZ SPECTROSCOPY OF MOLECULAR IONS USING HIGHLY ACCURATE AND PRECISE MID-IR SPECTROSCOPY Andrew A. Mills, Kyle B. Ford, Holger Kreckel,
Freezing phase scheme for complete-field characterization and coherent control of femtosecond optical pulses Jung Y. Huang, Ci L. Pan, and J. I. Chyi An.
J. Corlett. June 16, 2006 A Future Light Source for LBNL Facility Vision and R&D plan John Corlett ALS Scientific Advisory Committee Meeting June 16, 2006.
Sub-Doppler Spectroscopy of H 3 + James N. Hodges, Adam J. Perry, Brian M. Siller, Benjamin J. McCall.
QUANTUM OPTICS LAB IAP, UNIVERSITÄT BERN Qudit Implementations with Energy-Time Entangled Photons 1 Bänz Bessire Quantum Optics Lab – The Stefanov Group.
Four wave mixing in submicron waveguides
Present myself and the group Present our current research on: “title”
Fiber Laser Preamplifier
Sistem Telekomunikasi, Sukiswo, ST, MT Sukiswo
A. Bramati M. Romanelli E. Giacobino
Optical Feedback in a Curved-Facet Self-Pulsing Semiconductor Laser
Two-Photon Absorption Spectroscopy of Rubidium
Principle of Mode Locking
Stabilizing the Carrier-Envelope Phase of the Kansas Light Source
And their applications
LCLS Injector Laser System Paul R. Bolton, SLAC April 24, 2002
Wave front and energy front
Presentation transcript:

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 Amer ₪ - ISF, Kahn Foundation

Outline Why pulse shaping Standard techniques ◦ Mode locked oscillator cavity ◦ Extra-cavity shaping Intra cavity shaping – why not ? Gain shaping concept Results Conclusions

Pulse Shaping In Optics Control a pulse shape in time / spectrum Coherent quantum control Precision spectroscopy using frequency comb PRL 98, (2007) Label free Fluorescence microscopy with Stimulated Raman Science 322, (2008). Frequency domain picture Pump Dump τ vib t rep PumpDump Time domain picture

Standard Mode Locked Cavity (Ti:S) OC HR gain medium Pump 532 nm Mode competition (Gain, Loss, Dispersion) No knob on spectrum

Kerr Lens Mode Locked Cavities 1 st stability limit - Telescope 2 nd stability limit

Pulse Shaping (Extra-Cavity) Phase modulation: Simple, lossless Amplitude modulation: Lossy ! SLM

Intra Cavity Pulse Shaper ? OC HR gain medium Pump 532 nm In cavity phase = frequency shift No phase shaping ! Amplitude shaping = loss shaping Mode competition ! Two Colors – Impossible !

Two-Colors so far ? Active locking of independent lasers Opt. Lett. 27, 312 (2002) Passive Locking – shared Kerr medium Opt. Lett. 29, 629 (2004) OPO – signal and idler Synchronously pumped OPOs Time lens technique - Active modulation of a CW laser Optics Express 18, (2010)

Gain Shaping Spatial shaper OC HR 1st gain medium 2nd gain medium Beam splitter Pump 532 nm Spatial shape of pump = Spectral shape of gain

Results I Power (a.u.) Wavelength (nm)

Results II

Conclusions Multi lobed spectra in mode locked oscillators are important for many applications No easy solution so far – Synchronization of independent sources Gain shaping allows for arbitrary control of the oscillation spectrum.