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Süßmann F, Seiffert L, Zherebtsov S, Mondes V, Stierle J, Arbeiter M, Plenge J, Rupp P, Peltz C, Kessel A, Trushin SA, Ahn B, Kim D, Graf C, Rühl E, Kling MF, Fennel T. Field propagation-induced directionality of carrier-envelope phase-controlled photoemission from nanospheres. Nat Commun 2015; 6:7944. [PMID: 26264422 PMCID: PMC4557130 DOI: 10.1038/ncomms8944] [Citation(s) in RCA: 24] [Impact Index Per Article: 2.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/28/2015] [Accepted: 06/27/2015] [Indexed: 12/12/2022] Open
Abstract
Near-fields of non-resonantly laser-excited nanostructures enable strong localization of ultrashort light fields and have opened novel routes to fundamentally modify and control electronic strong-field processes. Harnessing spatiotemporally tunable near-fields for the steering of sub-cycle electron dynamics may enable ultrafast optoelectronic devices and unprecedented control in the generation of attosecond electron and photon pulses. Here we utilize unsupported sub-wavelength dielectric nanospheres to generate near-fields with adjustable structure and study the resulting strong-field dynamics via photoelectron imaging. We demonstrate field propagation-induced tunability of the emission direction of fast recollision electrons up to a regime, where nonlinear charge interaction effects become dominant in the acceleration process. Our analysis supports that the timing of the recollision process remains controllable with attosecond resolution by the carrier-envelope phase, indicating the possibility to expand near-field-mediated control far into the realm of high-field phenomena. The localized enhancement of laser light in optical near-fields of nanostructures enables the steering of ultrafast electronic motion. Here, the authors employ field propagation in nanospheres to obtain directional tunability and attosecond control of near-field-induced strong-field photoemission.
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Affiliation(s)
- F Süßmann
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany.,Physics Department, Ludwig-Maximilians-Universität München, D-85748 Garching, Germany
| | - L Seiffert
- Institut für Physik, Universität Rostock, D-18051 Rostock, Germany
| | - S Zherebtsov
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany.,Physics Department, Ludwig-Maximilians-Universität München, D-85748 Garching, Germany
| | - V Mondes
- Physical Chemistry, Freie Universität Berlin, Takustr. 3, D-14195 Berlin, Germany
| | - J Stierle
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany
| | - M Arbeiter
- Institut für Physik, Universität Rostock, D-18051 Rostock, Germany
| | - J Plenge
- Physical Chemistry, Freie Universität Berlin, Takustr. 3, D-14195 Berlin, Germany
| | - P Rupp
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany.,Physics Department, Ludwig-Maximilians-Universität München, D-85748 Garching, Germany
| | - C Peltz
- Institut für Physik, Universität Rostock, D-18051 Rostock, Germany
| | - A Kessel
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany
| | - S A Trushin
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany
| | - B Ahn
- Department of Physics, Center for Attosecond Science and Technology, Pohang University of Science and Technology, Pohang 790-784, South Korea.,Max Planck Center for Attosecond Science, Max Planck POSTECH/KOREA Res. Init., Pohang 790-784, South Korea
| | - D Kim
- Department of Physics, Center for Attosecond Science and Technology, Pohang University of Science and Technology, Pohang 790-784, South Korea.,Max Planck Center for Attosecond Science, Max Planck POSTECH/KOREA Res. Init., Pohang 790-784, South Korea
| | - C Graf
- Physical Chemistry, Freie Universität Berlin, Takustr. 3, D-14195 Berlin, Germany
| | - E Rühl
- Physical Chemistry, Freie Universität Berlin, Takustr. 3, D-14195 Berlin, Germany
| | - M F Kling
- Max-Planck-Institut für Quantenoptik, D-85748 Garching, Germany.,Physics Department, Ludwig-Maximilians-Universität München, D-85748 Garching, Germany.,Department of Physics, Center for Attosecond Science and Technology, Pohang University of Science and Technology, Pohang 790-784, South Korea.,J.R. Macdonald Laboratory, Physics Department, Kansas-State University, Manhattan, Kansas, USA
| | - T Fennel
- Institut für Physik, Universität Rostock, D-18051 Rostock, Germany
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Süssmann F, Zherebtsov S, Plenge J, Johnson NG, Kübel M, Sayler AM, Mondes V, Graf C, Rühl E, Paulus GG, Schmischke D, Swrschek P, Kling MF. Single-shot velocity-map imaging of attosecond light-field control at kilohertz rate. Rev Sci Instrum 2011; 82:093109. [PMID: 21974575 DOI: 10.1063/1.3639333] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/20/2023]
Abstract
High-speed, single-shot velocity-map imaging (VMI) is combined with carrier-envelope phase (CEP) tagging by a single-shot stereographic above-threshold ionization (ATI) phase-meter. The experimental setup provides a versatile tool for angle-resolved studies of the attosecond control of electrons in atoms, molecules, and nanostructures. Single-shot VMI at kHz repetition rate is realized with a highly sensitive megapixel complementary metal-oxide semiconductor camera omitting the need for additional image intensifiers. The developed camera software allows for efficient background suppression and the storage of up to 1024 events for each image in real time. The approach is demonstrated by measuring the CEP-dependence of the electron emission from ATI of Xe in strong (≈10(13) W/cm(2)) near single-cycle (4 fs) laser fields. Efficient background signal suppression with the system is illustrated for the electron emission from SiO(2) nanospheres.
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Affiliation(s)
- F Süssmann
- Max-Planck-Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, D-85748 Garching, Germany
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Abstract
The bond strength of chlorine peroxide (ClOOCl) is studied by photoionization mass spectrometry. The experimental results are obtained from the fragmentation threshold yielding ClO+, which is observed at 11.52 +/- 0.025 eV. The O-O bond strength D(o) is derived from this value in comparison to the first ionization energy of ClO, yielding D(o)298 = 72.39 +/- 2.8 kJ mol(-1). The present work provides a new and independent method to examine the equilibrium constant K(eq) for chlorine peroxide formation via dimerization of ClO in the stratosphere. This yields an approximation for the equilibrium constant in the stratospheric temperature regime between 190 and 230 K of the form K(eq) = 1.92 x 10(-27) cm3 molecules(-1) x exp(8430 K/T). This value of K(eq) is lower than current reference data and agrees well with high altitude aircraft measurements within their scattering range. Considering the error limits of the present experimental results and the resulting equilibrium constant, there is agreement with previous works, but the upper limit of current reference values appears to be too high. This result is discussed along with possible atmospheric implications.
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Affiliation(s)
- J Plenge
- Department of Chemistry, University of California at Berkeley, USA
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Meyer M, O'keeffe P, Plenge J, Flesch R, Rühl E. Radiative relaxation and fragmentation dynamics of S 2p-excited hydrogen sulfide. J Chem Phys 2006; 125:214306. [PMID: 17166020 DOI: 10.1063/1.2400234] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/14/2022] Open
Abstract
Radiative relaxation of S 2p-excited hydrogen sulfide (H(2)S) is investigated by dispersed ultraviolet and visible fluorescence spectroscopies. We observe distinct changes in the fluorescence spectra as a function of excitation energy. Excitation to Rydberg states below the S 2p ionization threshold yields intense fluorescence from neutral and ionic atomic fragments (H, S(+), and S(2+)). In addition to the atomic emission, fluorescence of the molecular fragment ion HS(+) is preferably found after excitation of the S 2p electron into the unoccupied 6a(1) and 3b(2) orbitals with sigma(*) character. This is interpreted as evidence for ultrafast dissociation of the core-excited molecule prior to electronic relaxation. The rotationally resolved fluorescence spectra of the A (3)Pi-->X (3)Sigma(-) transition are analyzed in terms of the fragmentation dynamics leading to the formation of the excited molecular fragment ion, where changes in bond angle are discussed in terms of the rotational population.
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Affiliation(s)
- M Meyer
- LURE, Centre Universitaire Paris-Sud, Bâtiment 209D, F-91898 Orsay Cedex, France
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Plenge J, Flesch R, Schürmann MC, Rühl E. Photofragmentation of Nitryl Chloride in the Ultraviolet Regime and Vacuum Ultraviolet Regime. J Phys Chem A 2001. [DOI: 10.1021/jp0044330] [Citation(s) in RCA: 11] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/03/2023]
Affiliation(s)
- J. Plenge
- Fachbereich Physik, Universität Osnabrück, Barbarastrasse 7, 49069 Osnabrück, Germany
| | - R. Flesch
- Fachbereich Physik, Universität Osnabrück, Barbarastrasse 7, 49069 Osnabrück, Germany
| | - M. C. Schürmann
- Fachbereich Physik, Universität Osnabrück, Barbarastrasse 7, 49069 Osnabrück, Germany
| | - E. Rühl
- Fachbereich Physik, Universität Osnabrück, Barbarastrasse 7, 49069 Osnabrück, Germany
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