Attomicroscopy: from Femtosecond to Attosecond Electron Microscopy
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Arxiv:1912.00017V1 [Physics.Atom-Ph] 29 Nov 2019
Theoretical Atto-nano Physics Marcelo F. Ciappina1 and Maciej Lewenstein2, 3 1Institute of Physics of the ASCR, ELI-Beamlines, Na Slovance 2, 182 21 Prague, Czech Republic 2ICFO - Institut de Ciencies Fotoniques, The Barcelona Institute of Science and Technology, Av. Carl Friedrich Gauss 3, 08860 Castelldefels (Barcelona), Spain 3ICREA - Instituci´oCatalana de Recerca i Estudis Avan¸cats,Lluis Companys 23, 08010 Barcelona, Spain (Dated: December 3, 2019) Two emerging areas of research, attosecond and nanoscale physics, have recently started to merge. Attosecond physics deals with phenomena occurring when ultrashort laser pulses, with duration on the femto- and sub-femtosecond time scales, interact with atoms, molecules or solids. The laser- induced electron dynamics occurs natively on a timescale down to a few hundred or even tens of attoseconds (1 attosecond=1 as=10−18 s), which is of the order of the optical field cycle. For com- parison, the revolution of an electron on a 1s orbital of a hydrogen atom is ∼ 152 as. On the other hand, the second topic involves the manipulation and engineering of mesoscopic systems, such as solids, metals and dielectrics, with nanometric precision. Although nano-engineering is a vast and well-established research field on its own, the combination with intense laser physics is relatively recent. We present a comprehensive theoretical overview of the tools to tackle and understand the physics that takes place when short and intense laser pulses interact with nanosystems, such as metallic and dielectric nanostructures. In particular we elucidate how the spatially inhomogeneous laser induced fields at a nanometer scale modify the laser-driven electron dynamics. -
Atomic Clocks, 14–19, 89–94 Attosecond Laser Pulses, 55–57
Index high-order harmonic generation, A 258–261 in strong laser fields, 238–243 Atomic clocks, 14–19, 89–94 in weak field regime, 274-277 Attosecond laser pulses, 55–57 metal-ligand charge-transfer, 253–254 organic chemical conversion, C 249–251 pulse shaping, 269–274 CARS microscopy with ultrashort quantum ladder climbing, 285–287 pulses, 24–25 simple shaped pulses, 235–238 Chirped-pulse amplification, 54–55 Tannor-Kosloff-Rice scheme, phase preservation in, 54–5 232–235 Chirped pulses, 271, 274–277, 235–238 via many-parameter control in liquid Coherent control, 225–266, 267–304, phase, 252–255 atoms and dimers in gas phase, Coherent transients, 274–285 228–243 bond-selective photochemistry, 248–249 D closed-loop pulse shaping, 244–246 coherent coupling, 238–243 Dielectric breakdown, 305–329 molecular electronic states, in oxide thin films, 318 238–241 phenomenological model of, 316 atomic electronic states, retrieval of dielectric constant, 322 241–243 Difference frequency generation, 123 coherent transients, 274–285 Dynamics, 146–148, 150, 167–196, control of electron motion, 255–261 187–224 control of photo-isomerization, of electronic states, 146–148 254–255 of excitonic states, 150 control of two-photon transitions, hydrogen bond dynamics, 167–196 285-287 molecular dynamics, 187–196 332 Femtosecond Laser Spectroscopy Femtosecond optical frequency combs, E 1–8, 12–21, 55–57, 87–108, 109–112, 120–128 Exciton-vibration interaction, 153–158 absolute phase control of, 55–57 dynamic intensity borrowing, attosecond pulses, 55–57 156–158 carrier-envelope offset frequency, Franck-Condon type, 159 3, 121 Herzberg-Teller type, 159–160 carrier envelope phase, 2, 121 interactions, 14–19 mid-infrared, 19-21, 120–127 F molecular spectroscopy with, 12–14 Femtochemistry, 198, 226 optical frequency standards, 14–19 Femtosecond lasers, 1–27 optical atomic clocks, 14–19, external optical cavities, 21–25 89–94 high resolution spectroscopy with, Femtosecond photon echoes. -
Attosecond Science on the East Coast
Attosecond Science on the East Coast Luca Argenti, Zenghu Chang, Michael Chini, Madhab Neupane, Mihai Vaida, and Li Fang Department of Physics & CREOL University of Central Florida The steady progress experienced by extreme non-linear optics and pulsed laser technology during the last decade of the XX century led to a transformative backthrough: the generation, in 2001, of the first attosecond extreme ultraviolet pulse. This was a revolutionary achievement, as the attosecond is the natural timescale of electronic motion in matter. The advent of attosecond pulses, therefore, opened the way to the time-resolved study of correlated electron dynamics in atoms, molecules, surfaces, and solids, to the coherent control of charge-transfer processes in chemical reactions and in nano-devices as well as, possibly, to ultrafast processing of quantum information. Attosecond research has been in a state of tumultuous growth ever since, giving rise to countless high-profile publications, the formation of a large international research community, and the appearance of new leading research hubs across the world. The University of Central Florida is one of them, establishing itself as the center of excellence for attosecond science on the US East Coast. The UCF Physics Department and CREOL host six internationally recognized leaders in attosecond science, Zenghu Chang, Michael Chini, Luca Argenti, Madhab Neupane, Mihai Vaida, and Li Fang (listed in the order they joined UCF), covering virtually all branches of this discipline, with topics ranging from theoretical photoelectron spectroscopy, to high-harmonic generation in gases and solids, the transient-absorption study of molecular core-holes decay, the time and angularly-resolved photoemission from topological insulators, heterogeneous catalysis control, and ultrafast nanoplasma physics. -
Generation of Attosecond Light Pulses from Gas and Solid State Media
hv photonics Review Generation of Attosecond Light Pulses from Gas and Solid State Media Stefanos Chatziathanasiou 1, Subhendu Kahaly 2, Emmanouil Skantzakis 1, Giuseppe Sansone 2,3,4, Rodrigo Lopez-Martens 2,5, Stefan Haessler 5, Katalin Varju 2,6, George D. Tsakiris 7, Dimitris Charalambidis 1,2 and Paraskevas Tzallas 1,2,* 1 Foundation for Research and Technology—Hellas, Institute of Electronic Structure & Laser, PO Box 1527, GR71110 Heraklion (Crete), Greece; [email protected] (S.C.); [email protected] (E.S.); [email protected] (D.C.) 2 ELI-ALPS, ELI-Hu Kft., Dugonics ter 13, 6720 Szeged, Hungary; [email protected] (S.K.); [email protected] (G.S.); [email protected] (R.L.-M.); [email protected] (K.V.) 3 Physikalisches Institut der Albert-Ludwigs-Universität, Freiburg, Stefan-Meier-Str. 19, 79104 Freiburg, Germany 4 Dipartimento di Fisica Politecnico, Piazza Leonardo da Vinci 32, 20133 Milano, Italy 5 Laboratoire d’Optique Appliquée, ENSTA-ParisTech, Ecole Polytechnique, CNRS UMR 7639, Université Paris-Saclay, 91761 Palaiseau CEDEX, France; [email protected] 6 Department of Optics and Quantum Electronics, University of Szeged, Dóm tér 9., 6720 Szeged, Hungary 7 Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany; [email protected] * Correspondence: [email protected] Received: 25 February 2017; Accepted: 27 March 2017; Published: 31 March 2017 Abstract: Real-time observation of ultrafast dynamics in the microcosm is a fundamental approach for understanding the internal evolution of physical, chemical and biological systems. Tools for tracing such dynamics are flashes of light with duration comparable to or shorter than the characteristic evolution times of the system under investigation. -
Early-Stage Dynamics of Chloride Ion–Pumping Rhodopsin Revealed by a Femtosecond X-Ray Laser
Early-stage dynamics of chloride ion–pumping rhodopsin revealed by a femtosecond X-ray laser Ji-Hye Yuna,1, Xuanxuan Lib,c,1, Jianing Yued, Jae-Hyun Parka, Zeyu Jina, Chufeng Lie, Hao Hue, Yingchen Shib,c, Suraj Pandeyf, Sergio Carbajog, Sébastien Boutetg, Mark S. Hunterg, Mengning Liangg, Raymond G. Sierrag, Thomas J. Laneg, Liang Zhoud, Uwe Weierstalle, Nadia A. Zatsepine,h, Mio Ohkii, Jeremy R. H. Tamei, Sam-Yong Parki, John C. H. Spencee, Wenkai Zhangd, Marius Schmidtf,2, Weontae Leea,2, and Haiguang Liub,d,2 aDepartment of Biochemistry, College of Life Sciences and Biotechnology, Yonsei University, Seodaemun-gu, 120-749 Seoul, South Korea; bComplex Systems Division, Beijing Computational Science Research Center, Haidian, 100193 Beijing, People’s Republic of China; cDepartment of Engineering Physics, Tsinghua University, 100086 Beijing, People’s Republic of China; dDepartment of Physics, Beijing Normal University, Haidian, 100875 Beijing, People’s Republic of China; eDepartment of Physics, Arizona State University, Tempe, AZ 85287; fPhysics Department, University of Wisconsin, Milwaukee, Milwaukee, WI 53201; gLinac Coherent Light Source, Stanford Linear Accelerator Center National Accelerator Laboratory, Menlo Park, CA 94025; hDepartment of Chemistry and Physics, Australian Research Council Centre of Excellence in Advanced Molecular Imaging, La Trobe Institute for Molecular Science, La Trobe University, Melbourne, VIC 3086, Australia; and iDrug Design Laboratory, Graduate School of Medical Life Science, Yokohama City University, 230-0045 Yokohama, Japan Edited by Nicholas K. Sauter, Lawrence Berkeley National Laboratory, Berkeley, CA, and accepted by Editorial Board Member Axel T. Brunger February 21, 2021 (received for review September 30, 2020) Chloride ion–pumping rhodopsin (ClR) in some marine bacteria uti- an acceptor aspartate (13–15). -
Comparing Femtosecond Lasers an Analysis of Commercially Available Platforms for Refractive Surgery
REFRACTIVE SURGERY FEATURE STORY Comparing Femtosecond Lasers An analysis of commercially available platforms for refractive surgery. BY JAY S. PEPOSE, MD, PHD, AND HOLGER LUBATSCHOWSKI, PHD ith the increasing popularity and expanding A BCD applications of femtosecond lasers in oph- thalmology,1,2 refractive surgery in particular, W a common question among practitioners is, how do the platforms differ? Currently commercially avail- able in the United States are the IntraLase FS (Advanced Medical Optics, Inc., Santa Ana, CA), Femto LDV (Ziemer Ophthalmic Systems Group, Port, Switzerland), Femtec (20/10 Perfect Vision AG, Heidelberg, Germany), and VisuMax femtosecond laser system (Carl Zeiss Meditec, Inc., Dublin, CA). A meaningful comparison requires some basic concepts of femtosecond laser physics and tissue interactions,3-5 important aspects of which are reviewed in this article. Figure 1. The course of a photodisruptive process is shown.Due BASIC PRINCIPLES to multiphoton absorption in the focus of the laser beam,plasma How short is ultrashort? The definition of a femtosec- develops (A).Depending on the laser parameter,the diameter ond is 10-15 seconds (ie, one millionth of a billionth of a varies between 0.5 µm to several micrometers.The expanding second). Putting that information into comprehensible plasma drives as a shock wave,which transforms after a few terms, it takes 1.2 seconds for light to travel from the microns to an acoustic transient (B).In addition to the shock moon to an earthbound observer’s retinas. In 100 fem- wave’s generation,the expanding plasma has pushed the sur- toseconds, light traverses 30 µm—around one-third the rounding medium away from its center,which results in a cavita- thickness of a human hair. -
Terahertz-Time Domain Spectrometer with 90 Db Peak Dynamic Range
J Infrared Milli Terahz Waves DOI 10.1007/s10762-014-0085-9 Terahertz-time domain spectrometer with 90 dB peak dynamic range N. Vieweg & F. Rettich & A. Deninger & H. Roehle & R. Dietz & T. Göbel & M. Schell Received: 24 January 2014 /Accepted: 12 June 2014 # The Author(s) 2014. This article is published with open access at Springerlink.com Abstract Many time-domain terahertz applications require systems with high bandwidth, high signal-to-noise ratio and fast measurement speed. In this paper we present a terahertz time-domain spectrometer based on 1550 nm fiber laser technology and InGaAs photocon- ductive switches. The delay stage offers both a high scanning speed of up to 60 traces / s and a flexible adjustment of the measurement range from 15 ps – 200 ps. Owing to a precise reconstruction of the time axis, the system achieves a high dynamic range: a single pulse trace of 50 ps is acquired in only 44 ms, and transformed into a spectrum with a peak dynamic range of 60 dB. With 1000 averages, the dynamic range increases to 90 dB and the measurement time still remains well below one minute. We demonstrate the suitability of the system for spectroscopic measurements and terahertz imaging. Keywords terahertz time domain spectroscopy. femtosecond fiber laser. InGaAs photoconductive switches . terahertz imaging 1 Introduction Terahertz waves feature unique properties: like microwaves, terahertz radiation passes through a plethora of non-conducting materials, including paper, cardboard, plastics, wood, ceramics and glass-fiber composites [1]. In contrast to microwaves, terahertz waves have a smaller wavelength and thus offer sub-millimeter spatial resolution. -
14. Measuring Ultrashort Laser Pulses I: Autocorrelation the Dilemma the Goal: Measuring the Intensity and Phase Vs
14. Measuring Ultrashort Laser Pulses I: Autocorrelation The dilemma The goal: measuring the intensity and phase vs. time (or frequency) Why? The Spectrometer and Michelson Interferometer 1D Phase Retrieval Autocorrelation 1D Phase Retrieval E(t) Single-shot autocorrelation E(t–) The Autocorrelation and Spectrum Ambiguities Third-order Autocorrelation Interferometric Autocorrelation 1 The Dilemma In order to measure an event in time, you need a shorter one. To study this event, you need a strobe light pulse that’s shorter. Photograph taken by Harold Edgerton, MIT But then, to measure the strobe light pulse, you need a detector whose response time is even shorter. And so on… So, now, how do you measure the shortest event? 2 Ultrashort laser pulses are the shortest technological events ever created by humans. It’s routine to generate pulses shorter than 10-13 seconds in duration, and researchers have generated pulses only a few fs (10-15 s) long. Such a pulse is to one second as 5 cents is to the US national debt. Such pulses have many applications in physics, chemistry, biology, and engineering. You can measure any event—as long as you’ve got a pulse that’s shorter. So how do you measure the pulse itself? You must use the pulse to measure itself. But that isn’t good enough. It’s only as short as the pulse. It’s not shorter. Techniques based on using the pulse to measure itself are subtle. 3 Why measure an ultrashort laser pulse? To determine the temporal resolution of an experiment using it. To determine whether it can be made even shorter. -
Attosecond Streaking Spectroscopy of Atoms and Solids
U. Thumm et al., in: Fundamentals of photonics and physics, D. L. Andrew (ed.), Chapter 13 (Wiley, New York 2015) Chapter x Attosecond Physics: Attosecond Streaking Spectroscopy of Atoms and Solids Uwe Thumm1, Qing Liao1, Elisabeth M. Bothschafter2,3, Frederik Süßmann2, Matthias F. Kling2,3, and Reinhard Kienberger2,4 1 J.R. Macdonald Laboratory, Physics Department, Kansas-State University, Manhattan, KS66506, USA 2 Max-Planck Institut für Quantenoptik, 85748 Garching, Germany 3 Physik Department, Ludwig-Maximilians-Universität, 85748 Garching, Germany 4 Physik Department, Technische Universität München, 85748 Garching, Germany 1. Introduction Irradiation of atoms and surfaces with ultrashort pulses of electromagnetic radiation leads to photoelectron emission if the incident light pulse has a short enough wavelength or has sufficient intensity (or both)1,2. For pulse intensities sufficiently low to prevent multiphoton absorption, photoemission occurs provided that the photon energy is larger than the photoelectron’s binding energy prior to photoabsorption, ħ휔 > 퐼푃. Photoelectron emission from metal surfaces was first analyzed by Albert Einstein in terms of light quanta, which we now call photons, and is commonly known as the photoelectric effect3. Even though the photoelectric effect can be elegantly interpreted within the corpuscular description of light, it can be equally well described if the incident radiation is represented as a classical electromagnetic wave4,5. With the emergence of lasers able to generate very intense light, it was soon shown that at sufficiently high intensities (routinely provided by modern laser systems) the condition ħω < 퐼푃 no longer precludes photoemission. Instead, the absorption of two or more photons can lead to photoemission, where 6 a single photon would fail to provide the ionization energy Ip . -
The Effect of Long Timescale Gas Dynamics on Femtosecond Filamentation
The effect of long timescale gas dynamics on femtosecond filamentation Y.-H. Cheng, J. K. Wahlstrand, N. Jhajj, and H. M. Milchberg* Institute for Research in Electronics and Applied Physics, University of Maryland, College Park, Maryland 20742, USA *[email protected] Abstract: Femtosecond laser pulses filamenting in various gases are shown to generate long- lived quasi-stationary cylindrical depressions or ‘holes’ in the gas density. For our experimental conditions, these holes range up to several hundred microns in diameter with gas density depressions up to ~20%. The holes decay by thermal diffusion on millisecond timescales. We show that high repetition rate filamentation and supercontinuum generation can be strongly affected by these holes, which should also affect all other experiments employing intense high repetition rate laser pulses interacting with gases. ©2013 Optical Society of America OCIS codes: (190.5530) Pulse propagation and temporal solitons; (350.6830) Thermal lensing; (320.6629) Supercontinuum generation; (260.5950) Self-focusing. References and Links 1. A. Couairon and A. Mysyrowicz, “Femtosecond filamentation in transparent media,” Phys. Rep. 441(2-4), 47– 189 (2007). 2. P. B. Corkum, C. Rolland, and T. Srinivasan-Rao, “Supercontinuum generation in gases,” Phys. Rev. Lett. 57(18), 2268–2271 (1986). S. A. Trushin, K. Kosma, W. Fuss, and W. E. Schmid, “Sub-10-fs supercontinuum radiation generated by filamentation of few-cycle 800 nm pulses in argon,” Opt. Lett. 32(16), 2432–2434 (2007). 3. N. Zhavoronkov, “Efficient spectral conversion and temporal compression of femtosecond pulses in SF6.,” Opt. Lett. 36(4), 529–531 (2011). 4. C. P. Hauri, R. B. -
Femtosecond Pulse Generation
Femto-UP 2020-21 School Femtosecond Pulse Generation Adeline Bonvalet Laboratoire d’Optique et Biosciences CNRS, INSERM, Ecole Polytechnique, Institut Polytechnique de Paris, 91128, Palaiseau, France 1 Definitions Electric field of a 10-fs 800-nm pulse nano 10-9 sec pico 10-12 femto 10-15 2,7 fs atto 10-18 10 fs time 2 Many properties Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Ultrashorti Duration Spectral Properties i (Frequency Comb) time 3 Time-resolved spectroscopy Electric field of a 10-fs 800-nm pulse Ultrashorti Duration Time-resolved spectroscopy Direct observation of ultrafast motions time Ahmed Zewail, Nobel Prize in chemistry 1999, femtochemistry 4 Imaging Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Nonlinear microscopy time 5 Material processing Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Laser matter interaction Drilling, cutting, etching,… time Areas of applications : aeronautics, electronics, medical,6 optics… Light matter interaction Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Ability to reach extreme conditions (amplified system) Applications : Sources of intense particles beams, X-rays, high energy density science, laboratory astroprophysics … time 7 Metrology Electric field of a 10-fs 800-nm pulse Spectral Properties i (Frequency Comb) Nobel Prize 2005 "for their contributions to the development of laser-based time precision spectroscopy, including the optical frequency comb technique." 8 Outline -
Attosecond Time-Resolved Photoelectron Holography
ARTICLE DOI: 10.1038/s41467-018-05185-6 OPEN Attosecond time-resolved photoelectron holography G. Porat1,2, G. Alon2, S. Rozen2, O. Pedatzur2, M. Krüger 2, D. Azoury2, A. Natan 3, G. Orenstein2, B.D. Bruner2, M.J.J. Vrakking4 & N. Dudovich2 Ultrafast strong-field physics provides insight into quantum phenomena that evolve on an attosecond time scale, the most fundamental of which is quantum tunneling. The tunneling 1234567890():,; process initiates a range of strong field phenomena such as high harmonic generation (HHG), laser-induced electron diffraction, double ionization and photoelectron holography—all evolving during a fraction of the optical cycle. Here we apply attosecond photoelectron holography as a method to resolve the temporal properties of the tunneling process. Adding a weak second harmonic (SH) field to a strong fundamental laser field enables us to recon- struct the ionization times of photoelectrons that play a role in the formation of a photo- electron hologram with attosecond precision. We decouple the contributions of the two arms of the hologram and resolve the subtle differences in their ionization times, separated by only a few tens of attoseconds. 1 JILA, National Institute of Standards and Technology and University of Colorado-Boulder, Boulder, CO 80309-0440, USA. 2 Department of Physics of Complex Systems, Weizmann Institute of Science, Rehovot 76100, Israel. 3 Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA. 4 Max-Born-Institut, Max Born Strasse 2A, Berlin 12489, Germany. These authors contributed equally: G. Porat, G. Alon. Correspondence and requests for materials should be addressed to N.D.