Single-Shot Tomographic Imaging of Evolving, Light Speed Object Zhengyan Li, Rafal Zgadzaj, Xiaoming Wang, Yen-Yu Chang, Michael C. Downer Department of.

Slides:



Advertisements
Similar presentations
CO 2 laser system M. Polyanskiy, I. Pogorelsky, M. Babzien, and V. Yakimenko.
Advertisements

The scaling of LWFA in the ultra-relativistic blowout regime: Generation of Gev to TeV monoenergetic electron beams W.Lu, M.Tzoufras, F.S.Tsung, C. Joshi,
Collinear interaction of photons with orbital angular momentum Apurv Chaitanya N Photonics science Laboratory, PRL.
Particle acceleration in plasma By Prof. C. S. Liu Department of Physics, University of Maryland in collaboration with V. K. Tripathi, S. H. Chen, Y. Kuramitsu,
Observation of the relativistic cross-phase modulation in a high intensity laser plasma interaction Shouyuan Chen, Matt Rever, Ping Zhang, Wolfgang Theobald,
Contour plots of electron density 2D PIC in units of  [n |e|] cr wake wave breaking accelerating field laser pulse Blue:electron density green: laser.
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,
Bunch Length Measurements in the E167 Experiment Ian Blumenfeld E167 Collaboration SLAC/UCLA/USC.
J.K. Wahlstrand, Y.-H. Chen a, Y.-H. Cheng, J. Palastro, S. Varma b, and H.M. Milchberg Dept. of Physics Dept. of Electrical and Computer Engineering Institute.
S. Varma, Y.-H. Chen, and H. M. Milchberg Institute for Research in Electronics and Applied Physics Dept. of Electrical and Computer Engineering Dept.
Ariadna study : Space-based femtosecond laser filamentation Vytautas Jukna, Arnaud Couairon, Carles Milián Centre de Physique théorique, CNRS École.
Ariadna study : Space-based femtosecond laser filamentation Vytautas Jukna, Arnaud Couairon, Carles Milián Centre de Physique théorique, CNRS École.
Enhancement of electron injection using two auxiliary interfering-pulses in LWFA Yan Yin ( 银燕 ) Department of Physics National University of Defense Technology.
Generation of short pulses
PWFA WG > 25 participants. 5 presentations: A. Krasnykh, A Proposal for Study of Structure and Dynamics of Energy/Matter Based on Production of γ-Ray.
2. High-order harmonic generation in gases Attosecond pulse generation 1. Introduction to nonlinear optics.
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)
Diagnostics for Benchmarking Experiments L. Van Woerkom The Ohio State University University of California, San Diego Center for Energy Research 3rd MEETING.
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
Imaging Diagnostics at the H-1 National Plasma Fusion Research Facility Left: The coherence tomography system Above: Plasma emission reconstructions compared.
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,
Ultrafast Dynamics in Solid Plasmas Using Solid Plasmas Using Doppler Spectrometry and Giant magnetic Pulses Ultrafast Dynamics in Solid Plasmas Using.
Single-shot visualization of EVOLVING, light-speed index structures by multi- object phase contrast imaging Zhengyan Li, Rafal Zgadzaj, Xiaoming Wang,
High Harmonic Generation in Gases Muhammed Sayrac Texas A&M University.
Palaiseau - FRANCE Spatio-Temporal Chirped Pulse Amplification for Avoiding Spectral Modifications in Ultra-Short Petawatt Lasers C. Radier1,2, F. Giambruno1,3,
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
Ultrafast particle and photon sources driven by intense laser ‐ plasma interaction Jyhpyng Wang Institute of Atomic and Molecular Sciences, Academia Sinica.
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.
Femto-second Measurements of Semiconductor Laser Diodes David Baxter
Interaction of laser pulses with atoms and molecules and spectroscopic applications.
Argonne National Laboratory is managed by The University of Chicago for the U.S. Department of Energy Distortion of single-shot EO sampling techniques.
Shortening a laser pulse at the focus of a lens Yuelin Li Accelerator Systems Division Argonne National Laboratory
Application of Plasma Waveguides to Advanced High Energy Accelerators H.M. Milchberg +* and T.M. Antonsen, Jr. #* * Institute for Physical Science and.
Institute of Atomic and Molecular Sciences, Academia Sinica, Taiwan National Taiwan University, Taiwan National Central University, Taiwan National Chung.
Nonlinear Optics in Plasmas. What is relativistic self-guiding? Ponderomotive self-channeling resulting from expulsion of electrons on axis Relativistic.
R. Kupfer, B. Barmashenko and I. Bar
LASER-PLASMA ACCELERATORS: PRODUCTION OF HIGH-CURRENT ULTRA-SHORT e - -BEAMS, BEAM CONTROL AND RADIATION GENERATION I.Yu. Kostyukov, E.N. Nerush (IAP RAS,
Relativistic nonlinear optics in laser-plasma interaction Institute of Atomic and Molecular Sciences Academia Sinica, Taiwan National Central University,
W.Lu, M.Tzoufras, F.S.Tsung, C.Joshi, W.B.Mori
SIMULATIONS FOR THE ELUCIDATION OF ELECTRON BEAM PROPERTIES IN LASER-WAKEFIELD ACCELERATION EXPERIMENTS VIA BETATRON AND SYNCHROTRON-LIKE RADIATION P.
Multiple-Cone Formation during the Femtosecond-Laser Pulse Propagation in Silica Kenichi Ishikawa *, Hiroshi Kumagai, and Katsumi Midorikawa Laser Technology.
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.
Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.
Transverse Gradient Undulator and its applications to Plasma-Accelerator Based FELs Zhirong Huang (SLAC) Introduction TGU concept, theory, technology Soft.
Measurements of High-Field THz Induced Photocurrents in Semiconductors Michael Wiczer University of Illinois – Urbana-Champaign Mentor: Prof. Aaron Lindenberg.
Accelerator Laboratory of Tsinghua University Generation, measurement and applications of high brightness electron beam Dao Xiang Apr-17, /37.
Single-shot, Sub-picosecond, EO bunch measurements at FELIX Steven Jamison, Giel Berden, Allan MacLeod Allan Gillespie, Jingling Shen, Dino Jaroszynski,
Prospects for generating high brightness and low energy spread electron beams through self-injection schemes Xinlu Xu*, Fei Li, Peicheng Yu, Wei Lu, Warren.
(Frequency-resolved optical-gating)
Muhammad Firmansyah Kasim University of Oxford, UK PhD Supervisors: Professor Peter Norreys & Professor Philip Burrows University of Oxford, UK AWAKE Collaboration.
Ionization Injection E. Öz Max Planck Institute Für Physik.
10fs laser pulse propagation in air Conclusion The properties of femtosecond laser pulse propagation over a long distance (up to 100m) were studied for.
V.N. Litvinenko (SBU) C. Joshi, W. Mori (UCLA)
The 2nd European Advanced Accelerator Concepts Workshop
SUPA, Department of Physics, University of Strathclyde,
Single-shot visualization of EVOLVING, light-speed index structures by multi-object phase contrast imaging Zhengyan Li, Rafal Zgadzaj, Xiaoming Wang, Chih-Hao.
Laboratoire d’Optique Appliquée
Tunable Electron Bunch Train Generation at Tsinghua University
FCC ee Instrumentation
All-Optical Injection
SPLASH FALL ALEXANDRE GAUTHIER
Principle of Mode Locking
Peking University: Jinqing Yu, Ronghao Hu, Haiyang Lu & Xueqing Yan
Diagnosis of a High Harmonic Beam Using
High-power laser pulse propagation in silica
Plasma acceleration and betatron oscillations
High energy 6.2 fs pulses Shambhu Ghimire, Bing Shan, and Zenghu Chang
Presentation transcript:

Single-Shot Tomographic Imaging of Evolving, Light Speed Object Zhengyan Li, Rafal Zgadzaj, Xiaoming Wang, Yen-Yu Chang, Michael C. Downer Department of Physics and Institute of Fusion Studies The University of Texas at Austin, Austin, TX Advanced Accelerator Concepts, Austin, TX, June 15, 2012

Evolution of index structures is common in different medium and different applications… Simulation of evolving wakes for e - self-injection in LWFA S. Kalmykov, et al., PRL 103, (2009) Simulation of evolving electron driving and witness beam in electron-driven plasma accelerators I. Blumenfeld, et al., Nature 445, (2007) Single-shot visualization in laboratory of evolving refractive index structures! Simulation of evolving pulse intensity during nonlinear propagation in fused silica A. Couairon, et al., Phys. Rev. B 71, (2005)

Single-shot Frequency-Domain Holography (FDH) took snapshots of quasi-static laser wakefields… N. Matlis et al., “Snapshots of laser wakefields,” Nature Physics 2, (2006) Phase accumulated in the collinear probe averages the z-dependence of the wakefields, i.e. index structure η(r, ζ, z). Thus FDH can only take snapshots of quasi-static objects.

As a generalization FDH, Frequency-Domain Streak Camera (FDSC) is a time sequence of the object’s tomographic projections… Z. Li, et al., “Frequency-domain streak camera for ultrafast imaging of evolving, light-speed objects,” Opt. Lett. 35, (2010) FDSC is a time sequence of the object’s projections along projection angle ϕ

Frequency-domain tomography (FDT) incorporate multiple probes to get FDSC covering projection angles from -70 to 70 degree in a single shot…

Compact probe array generation are based on nonlinear optical effects for tomographic application… Large n 2 glass HZF4 for cascaded FWM BBO Go to another HZF4 for chirp Incident beam pair 800 nm cascade FWM: 8 in total polarization 400 nm probes through SHG & SFG: 15 in total Frequency domain streak cameras (FDSC) coded in selected 5 probes  No movable parts for tomographic angle scanning  Self-synchronized by imaging the “sandwich” to interaction region  Up to 15 probes generated with comparable energy  Minimized phase mismatch in BBO by using correct polarization  Compact and inexpensive

Angular or temporal multiplexing of probes enables cost-efficient data collection with a single spectrometer in a single shot… FDH raw data2D Fourier transform RefProbe 1 RefProbe 1 Probe 2 RefProbe 1 Probe 2 Probe 3

Single-shot tomographic movies reveal dynamics of nonlinear pulse propagation, i.e. self-focusing, laser filamentation, plasma generation…

Simulation of femtosecond pulse nonlinear propagation is consistent with measured movie, including effects of diffraction, dispersion, self-focusing, plasma effect, and multi-photon processes… 400 nJ 500 nJ 600 nJ 700 nJ

What interesting physics can we learn from movies for glass experiments? It is not only a prototype experiment for future application in plasma based wake field accelerators, but also important to understanding femtosecond filamentation. White-light LIDAR J. Kasparian et al., Science 301,61-64 (2003) Lightening control Nature Photonics 3, (2009) Triggering rain in air P. Rohwetter et al., Nature Photonics 4, (2010) What is the mechanism of filamentation? Established theory: the balance between positive nonlinear refractive index n 2 I and negative index by plasma New theory: negative contribution of high order nonlinearity (e.g. n 4, n 8 ) leads to saturation of nonlinear refractive index V. S. P. Bejot, et al., PRL 104, (2010) P. Bejot, et al., PRL 106, (2011) C. Bree, et al., PRL 106, (2011) A. Couairona, et al., Phys. Rep. 441, (2007) P. Polynkin, et al., PRL 106, (2011) J. M. Brown, et al., Opt. Lett. 37, (2012)

Different mechanisms yield different behaviors of refractive index profiles… Established theoryNew theory For peak plasma density, i.e. steady state Movie frame at z = 2.5 mm for 700 nJ pump In simulation, plasma effect starts to balance nonlinear Kerr effect at z = 2.5 mm, with laser peak intensity of 26 TW, and plasma density of ~10 18 cm -3 Our “movie” supported the established theory about plasma effect for glass in our parameter regime.

Single-shot tomographic technique, i.e. frequency-domain tomography (FDT), yields a movie of wake-field evolution or electron bunch interactions for both high and low density LWFA/PWFA… Index structure evolution in laser- filamentation in glass medium A broadening of probe band- width to ~100 nm for temporal resolution of ~10 fs For high density LWFA, modified FDT system with broader bandwidth can make a movie of wake-field “bubble” evolution For low density LWFA/PWFA, small oblique angle probing reveals temporal profile evolution For Texas Petawatt, temporal profile of wake field and its elongation and contraction would be visualized, which is critical for electron injection.

Summary Frequency-domain tomography (FDT) applies multiple probes at different angles in a single shot, yielding a movie of evolving index structures. FDT is compact and inexpensive by generating multi-probe array through standard nonlinear optical effects, and by detecting probes through angular/temporal multiplexing methods. The application of FDT to laser-dielectrics interactions reveals the mechanism of femtosecond filamentation. FDT will be applied to wake field diagnosis in future. This work is supported by U.S. Department of Energy (DoE) grants DE-FG02-07ER54945 and DE-FG02-96ER and National Science Foundation (NSF) grant PHY