1
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Lin J, Zhou J, Wang Z, Li L, Li M, Xu J, Wu S, Naumov P, Gong J. Low-Temperature Flexibility of Chiral Organic Crystals with Highly Efficient Second-Harmonic Generation. Angew Chem Int Ed Engl 2025; 64:e202416856. [PMID: 39291894 DOI: 10.1002/anie.202416856] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/02/2024] [Revised: 09/17/2024] [Accepted: 09/18/2024] [Indexed: 09/19/2024]
Abstract
Flexible crystals with unique mechanical properties have presented potential for applications in optoelectronics, soft robotics and sensors. However, there have been no reports of low-temperature-resistant flexible crystals with second-order nonlinear optical properties (NLO). Here, we report flexible chiral Schiff-base crystals capable of efficient second harmonic generation (SHG). Both enantiomers and the racemic form of these crystals are mechanically flexible in two directions at both room temperature and at 77 K, although their mechanical responses differ. The enantiomers display SHG with an intensity of up to 12 times that of potassium dihydrogenphosphate (KDP) when pumped at 980 nm, and they also have high laser-induced damage thresholds (LDT). Even when bent, the crystals retain strong second harmonic generation, although with a different intensity distribution depending on the polarization, compared to when they are straight. This work describes the first instance of flexible organic single-crystalline material with NLO properties and lays the foundation for the development of mechanically flexible organic NLO materials.
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Affiliation(s)
- Jiawei Lin
- School of Chemical Engineering and Technology, State Key Laboratory of Chemical Engineering, Tianjin University, Tianjin, 300072, P. R. China
- Haihe Laboratory of Sustainable Chemical Transformations, Tianjin, 300192, P. R. China
| | - Jianmin Zhou
- School of Chemical Engineering and Technology, State Key Laboratory of Chemical Engineering, Tianjin University, Tianjin, 300072, P. R. China
- Haihe Laboratory of Sustainable Chemical Transformations, Tianjin, 300192, P. R. China
| | - Zhihua Wang
- School of Materials Science and Engineering, Smart Sensing Interdisciplinary Science Center, Frontiers Science Center for New Organic Matter, Nankai University, Tianjin, 300350, P. R. China
| | - Liang Li
- Smart Materials Lab, New York University Abu Dhabi, P.O. Box 129188, Abu Dhabi, United Arab Emirates
- Department of Sciences and Engineering, Sorbonne University Abu Dhabi, P.O. Box 38044, Abu Dhabi, United Arab Emirates
| | - Maolin Li
- School of Chemical Engineering and Technology, State Key Laboratory of Chemical Engineering, Tianjin University, Tianjin, 300072, P. R. China
- Haihe Laboratory of Sustainable Chemical Transformations, Tianjin, 300192, P. R. China
| | - Jialiang Xu
- School of Materials Science and Engineering, Smart Sensing Interdisciplinary Science Center, Frontiers Science Center for New Organic Matter, Nankai University, Tianjin, 300350, P. R. China
| | - Songgu Wu
- School of Chemical Engineering and Technology, State Key Laboratory of Chemical Engineering, Tianjin University, Tianjin, 300072, P. R. China
- Haihe Laboratory of Sustainable Chemical Transformations, Tianjin, 300192, P. R. China
| | - Panče Naumov
- Smart Materials Lab, New York University Abu Dhabi, P.O. Box 129188, Abu Dhabi, United Arab Emirates
- Center for Smart Engineering Materials, New York University Abu Dhabi, P.O. Box 129188, Abu Dhabi, United Arab Emirates
- Research Center for Environment and Materials, Macedonian Academy of Sciences and Arts Bul. Krste, Misirkov 2, MK-1000, Skopje, Macedonia
- Molecular Design Institute, Department of Chemistry, New York University, 100 Washington Square East, New York, NY 10003, USA
| | - Junbo Gong
- School of Chemical Engineering and Technology, State Key Laboratory of Chemical Engineering, Tianjin University, Tianjin, 300072, P. R. China
- Haihe Laboratory of Sustainable Chemical Transformations, Tianjin, 300192, P. R. China
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2
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Tissandier F, Jurkovičová L, Gautier J, Staněk M, Finke O, Albrecht M, Nejdl J, Hort O, Sebban S. Demonstration of a kHz-repetition-rate extreme ultraviolet laser at 41.8 nm. OPTICS LETTERS 2024; 49:6321-6324. [PMID: 39485477 DOI: 10.1364/ol.538340] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/05/2024] [Accepted: 10/15/2024] [Indexed: 11/03/2024]
Abstract
We demonstrate the operation of a plasma-based extreme ultraviolet (XUV) laser at a 1 kHz repetition rate driven by infrared pump pulses of less than 20 mJ. The 41.8 nm laser pulses were generated in a Xe plasma created by optical-field ionization by the L1 Allegra laser at ELI Beamlines. The output power of the XUV laser lies in the few microwatt range, and the energy efficiency of this pumping scheme opens the way for further scaling in repetition rate and average power.
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3
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Hutchison CM, Perrett S, van Thor JJ. XFEL Beamline Optical Instrumentation for Ultrafast Science. J Phys Chem B 2024; 128:8855-8868. [PMID: 39087627 PMCID: PMC11421085 DOI: 10.1021/acs.jpcb.4c01492] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/06/2024] [Revised: 07/15/2024] [Accepted: 07/15/2024] [Indexed: 08/02/2024]
Abstract
Free electron lasers operating in the soft and hard X-ray regime provide capabilities for ultrafast science in many areas, including X-ray spectroscopy, diffractive imaging, solution and material scattering, and X-ray crystallography. Ultrafast time-resolved applications in the picosecond, femtosecond, and attosecond regimes are often possible using single-shot experimental configurations. Aside from X-ray pump and X-ray probe measurements, all other types of ultrafast experiments require the synchronized operation of pulsed laser excitation for resonant or nonresonant pumping. This Perspective focuses on the opportunities for the optical control of structural dynamics by applying techniques from nonlinear spectroscopy to ultrafast X-ray experiments. This typically requires the synthesis of two or more optical pulses with full control of pulse and interpulse parameters. To this end, full characterization of the femtosecond optical pulses is also highly desirable. It has recently been shown that two-color and two-pulse femtosecond excitation of fluorescent protein crystals allowed a Tannor-Rice coherent control experiment, performed under characterized conditions. Pulse shaping and the ability to synthesize multicolor and multipulse conditions are highly desirable and would enable XFEL facilities to offer capabilities for structural dynamics. This Perspective will give a summary of examples of the types of experiments that could be achieved, and it will additionally summarize the laser, pulse shaping, and characterization that would be recommended as standard equipment for time-resolved XFEL beamlines, with an emphasis on ultrafast time-resolved serial femtosecond crystallography.
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Affiliation(s)
- Christopher
D. M. Hutchison
- Department
of Life Sciences, Faculty of Natural Sciences, Imperial College London, London SW7 2AZ, United
Kingdom
| | - Samuel Perrett
- Department
of Life Sciences, Faculty of Natural Sciences, Imperial College London, London SW7 2AZ, United
Kingdom
| | - Jasper J. van Thor
- Department
of Life Sciences, Faculty of Natural Sciences, Imperial College London, London SW7 2AZ, United
Kingdom
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4
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Yang Y, Liu J, Zhao C, Liang Q, Dong W, Shi J, Wang P, Kong D, Lv L, Jia L, Wang D, Huang C, Zheng S, Wang M, Liu F, Yu P, Qiao J, Ji W, Zhou J. A Universal Strategy for Synthesis of 2D Ternary Transition Metal Phosphorous Chalcogenides. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2024; 36:e2307237. [PMID: 37776266 DOI: 10.1002/adma.202307237] [Citation(s) in RCA: 5] [Impact Index Per Article: 5.0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/21/2023] [Revised: 09/26/2023] [Indexed: 10/02/2023]
Abstract
The 2D ternary transition metal phosphorous chalcogenides (TMPCs) have attracted extensive research interest due to their widely tunable band gap, rich electronic properties, inherent magnetic and ferroelectric properties. However, the synthesis of TMPCs via chemical vapor deposition (CVD) is still challenging since it is difficult to control reactions among multi-precursors. Here, a subtractive element growth mechanism is proposed to controllably synthesize the TMPCs. Based on the growth mechanism, the TMPCs including FePS3 , FePSe3 , MnPS3 , MnPSe3 , CdPS3 , CdPSe3 , In2 P3 S9 , and SnPS3 are achieved successfully and further confirmed by Raman, second-harmonic generation (SHG), and scanning transmission electron microscopy (STEM). The typical TMPCs-SnPS3 shows a strong SHG signal at 1064 nm, with an effective nonlinear susceptibility χ(2) of 8.41 × 10-11 m V-1 , which is about 8 times of that in MoS2 . And the photodetector based on CdPSe3 exhibits superior detection performances with responsivity of 582 mA W-1 , high detectivity of 3.19 × 1011 Jones, and fast rise time of 611 µs, which is better than most previously reported TMPCs-based photodetectors. These results demonstrate the high quality of TMPCs and promote the exploration of the optical properties of 2D TMPCs for their applications in optoelectronics.
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Affiliation(s)
- Yang Yang
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Jijian Liu
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Chunyu Zhao
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Qingrong Liang
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Weikang Dong
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Jia Shi
- Institute of Information Photonics Technology and School of Physics and Optoelectronics, Faculty of Science, Beijing University of Technology, Beijing, 100124, China
| | - Ping Wang
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Denan Kong
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Lu Lv
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Lin Jia
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Dainan Wang
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Chun Huang
- Advanced Research Institute of Multidisciplinary Science, Beijing Institute of Technology, Beijing, 10081, China
| | - Shoujun Zheng
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
| | - Meiling Wang
- School of Materials Science and Engineering, Taiyuan University of Technology, Taiyuan, 030002, China
| | - Fucai Liu
- School of Optoelectronic Science and Engineering, University of Electronic Science and Technology of China, Chengdu, 611731, China
| | - Peng Yu
- School of Materials Science and Engineering, Sun Yat-sen University, Guangzhou, 510275, China
| | - Jingsi Qiao
- Advanced Research Institute of Multidisciplinary Science, Beijing Institute of Technology, Beijing, 10081, China
| | - Wei Ji
- Beijing Key Laboratory of Optoelectronic Functional Materials & Micro-Nano Devices, Department of Physics, Renmin University of China, Beijing, 100872, China
| | - Jiadong Zhou
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, 10081, China
- Advanced Research Institute of Multidisciplinary Science, Beijing Institute of Technology, Beijing, 10081, China
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5
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Woodahl C, Jamnuch S, Amado A, Uzundal CB, Berger E, Manset P, Zhu Y, Li Y, Fong DD, Connell JG, Hirata Y, Kubota Y, Owada S, Tono K, Yabashi M, Te Velthuis SGE, Tepavcevic S, Matsuda I, Drisdell WS, Schwartz CP, Freeland JW, Pascal TA, Zong A, Zuerch M. Probing lithium mobility at a solid electrolyte surface. NATURE MATERIALS 2023; 22:848-852. [PMID: 37106132 PMCID: PMC10313518 DOI: 10.1038/s41563-023-01535-y] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/01/2022] [Accepted: 03/16/2023] [Indexed: 06/19/2023]
Abstract
Solid-state electrolytes overcome many challenges of present-day lithium ion batteries, such as safety hazards and dendrite formation1,2. However, detailed understanding of the involved lithium dynamics is missing due to a lack of in operando measurements with chemical and interfacial specificity. Here we investigate a prototypical solid-state electrolyte using linear and nonlinear extreme-ultraviolet spectroscopies. Leveraging the surface sensitivity of extreme-ultraviolet-second-harmonic-generation spectroscopy, we obtained a direct spectral signature of surface lithium ions, showing a distinct blueshift relative to bulk absorption spectra. First-principles simulations attributed the shift to transitions from the lithium 1 s state to hybridized Li-s/Ti-d orbitals at the surface. Our calculations further suggest a reduction in lithium interfacial mobility due to suppressed low-frequency rattling modes, which is the fundamental origin of the large interfacial resistance in this material. Our findings pave the way for new optimization strategies to develop these electrochemical devices via interfacial engineering of lithium ions.
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Affiliation(s)
- Clarisse Woodahl
- University of Florida, Gainesville, FL, USA
- Department of Chemistry, University of California, Berkeley, CA, USA
| | - Sasawat Jamnuch
- ATLAS Materials Science Laboratory, Department of Nano Engineering and Chemical Engineering, University of California, San Diego, La Jolla, CA, USA
| | - Angelique Amado
- Department of Chemistry, University of California, Berkeley, CA, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Can B Uzundal
- Department of Chemistry, University of California, Berkeley, CA, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Emma Berger
- Department of Chemistry, University of California, Berkeley, CA, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Paul Manset
- École Normale Supérieure - PSL, Paris, France
| | - Yisi Zhu
- Materials Science Division, Argonne National Laboratory, Lemont, IL, USA
| | - Yan Li
- Materials Science Division, Argonne National Laboratory, Lemont, IL, USA
| | - Dillon D Fong
- Materials Science Division, Argonne National Laboratory, Lemont, IL, USA
| | - Justin G Connell
- Materials Science Division, Argonne National Laboratory, Lemont, IL, USA
| | | | - Yuya Kubota
- RIKEN SPring-8 Center, Sayo, Hyogo, Japan
- Japan Synchrotron Radiation Research Institute, Sayo, Hyogo, Japan
| | - Shigeki Owada
- RIKEN SPring-8 Center, Sayo, Hyogo, Japan
- Japan Synchrotron Radiation Research Institute, Sayo, Hyogo, Japan
| | - Kensuke Tono
- RIKEN SPring-8 Center, Sayo, Hyogo, Japan
- Japan Synchrotron Radiation Research Institute, Sayo, Hyogo, Japan
| | - Makina Yabashi
- RIKEN SPring-8 Center, Sayo, Hyogo, Japan
- Japan Synchrotron Radiation Research Institute, Sayo, Hyogo, Japan
| | | | - Sanja Tepavcevic
- Materials Science Division, Argonne National Laboratory, Lemont, IL, USA
| | - Iwao Matsuda
- Institute for Solid State Physics, The University of Tokyo, Kashiwa, Japan
- Trans-scale Quantum Science Institute, The University of Tokyo, Tokyo, Japan
| | - Walter S Drisdell
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- Joint Center for Artificial Photosynthesis, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Craig P Schwartz
- Nevada Extreme Conditions Laboratory, University of Nevada, Las Vegas, Las Vegas, NV, USA
| | - John W Freeland
- X-ray Science Division, Argonne National Laboratory, Lemont, IL, USA
| | - Tod A Pascal
- ATLAS Materials Science Laboratory, Department of Nano Engineering and Chemical Engineering, University of California, San Diego, La Jolla, CA, USA.
- Materials Science and Engineering, University of California San Diego, La Jolla, CA, USA.
- Sustainable Power and Energy Center, University of California San Diego, La Jolla, CA, USA.
| | - Alfred Zong
- Department of Chemistry, University of California, Berkeley, CA, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Michael Zuerch
- Department of Chemistry, University of California, Berkeley, CA, USA.
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA.
- Fritz Haber Institute of the Max Planck Society, Berlin, Germany.
- Friedrich Schiller University Jena, Jena, Germany.
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6
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López S, de la Fuente E, Alonso A, Pandey AK, Guilbaud O, Oliva E. Conservation of orbital angular momentum throughout amplification of high order harmonics in Ni-like krypton and silver plasmas. OPTICS EXPRESS 2023; 31:8465-8478. [PMID: 36859961 DOI: 10.1364/oe.478099] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/28/2022] [Accepted: 01/04/2023] [Indexed: 06/18/2023]
Abstract
In this article we present modelling results of the amplification of High Order Harmonics (HOH) carrying orbital angular momentum (OAM) in plasma amplifiers created from krypton gas and silver solid targets. The resulting amplified beam is characterized in terms of intensity, phase and decomposition in helical and Laguerre-Gauss modes. Results show that the amplification process conserves OAM, although some degradation is apparent. Several structures appear in the intensity and phase profiles. These structures have been characterized with our model and related to refraction and interference with the plasma self-emission. Thus, these results not only demonstrate the capability of plasma amplifiers to deliver HOH amplified beams carrying OAM but also pave the way towards using HOH carrying OAM as a probe beam to diagnose the dynamics of hot, dense plasmas.
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7
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Tsai MS, Liang AY, Tsai CL, Lai PW, Lin MW, Chen MC. Nonlinear compression toward high-energy single-cycle pulses by cascaded focus and compression. SCIENCE ADVANCES 2022; 8:eabo1945. [PMID: 35921417 PMCID: PMC9348793 DOI: 10.1126/sciadv.abo1945] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/20/2022] [Accepted: 06/21/2022] [Indexed: 05/31/2023]
Abstract
The advancement of contemporary ultrafast science requires reliable sources to provide high-energy few-cycle light pulses. Through experiments and simulations, we demonstrate an arrangement of pulse postcompression, referred to as cascaded focus and compression (CASCADE), for generating millijoule-level, single-cycle pulses in a compact fashion. CASCADE is realized by a series of foci in matter, whereas pulse compression is provided immediately after each focus to maintain a high efficiency of spectral broadening. By implementing four stages of CASCADE in argon cells, we achieve 50-fold compression of millijoule-level pulses at 1030 nanometers from 157 to 3.1 femtoseconds, with an output pulse energy of 0.98 millijoules and a transmission efficiency of 73%. When driving high harmonic generation, these single-cycle pulses enable the creation of a carrier-envelope phase-dependent extreme ultraviolet continuum with energies extending up to 180 electron volts, providing isolated attosecond pulses at the output.
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Affiliation(s)
- Ming-Shian Tsai
- Institute of Photonics Technologies, National Tsing Hua University, Hsinchu 300044, Taiwan
| | - An-Yuan Liang
- Institute of Photonics Technologies, National Tsing Hua University, Hsinchu 300044, Taiwan
| | - Chia-Lun Tsai
- Institute of Photonics Technologies, National Tsing Hua University, Hsinchu 300044, Taiwan
| | - Po-Wei Lai
- Institute of Nuclear Engineering and Science, National Tsing Hua University, Hsinchu 300044, Taiwan
| | - Ming-Wei Lin
- Institute of Nuclear Engineering and Science, National Tsing Hua University, Hsinchu 300044, Taiwan
| | - Ming-Chang Chen
- Institute of Photonics Technologies, National Tsing Hua University, Hsinchu 300044, Taiwan
- Department of Physics, National Tsing Hua University, Hsinchu 300044, Taiwan
- Frontier Research Center on Fundamental and Applied Sciences of Matters, National Tsing Hua University, Hsinchu, Taiwan
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8
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Delmotte F, Burcklen C, Alameda J, Salmassi F, Gullikson E, Soufli R. New method for the determination of photoabsorption from transmittance measurements in the extreme ultraviolet. OPTICS EXPRESS 2022; 30:23771-23782. [PMID: 36225052 DOI: 10.1364/oe.461333] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/17/2022] [Accepted: 05/18/2022] [Indexed: 06/16/2023]
Abstract
We have developed a new method for the determination of photoabsorption at extreme ultraviolet wavelengths longer than 20 nm, where reliable refractive index values are sparse or non-existent. Our method overcomes the obstacle of multiple reflections that occur inside thin films in this spectral range, which up until now has prevented the accurate determination of photoabsorption from transmittance measurements. We have derived a mathematical expression that is independent of internal reflection amplitudes, while taking advantage of the transmittance oscillations stemming from such reflections. The method is validated on measurements of aluminum thin films. This advance will enable accurate refractive index values for many important materials for optical instrumentation, thus facilitating high-priority research on topics including coherent light sources, planetary and solar physics, and semiconductor manufacturing.
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9
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Separating Non-linear Optical Signals of a Sample from High Harmonic Radiation in a Soft X-ray Free Electron Laser. E-JOURNAL OF SURFACE SCIENCE AND NANOTECHNOLOGY 2022. [DOI: 10.1380/ejssnt.2022-002] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/20/2022]
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10
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Loetgering L, Witte S, Rothhardt J. Advances in laboratory-scale ptychography using high harmonic sources [Invited]. OPTICS EXPRESS 2022; 30:4133-4164. [PMID: 35209658 DOI: 10.1364/oe.443622] [Citation(s) in RCA: 12] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/23/2021] [Accepted: 12/22/2021] [Indexed: 06/14/2023]
Abstract
Extreme ultraviolet microscopy and wavefront sensing are key elements for next-generation ultrafast applications, such as chemically-resolved imaging, focal spot diagnostics in pump-and-probe experiments, and actinic metrology for the state-of-the-art lithography node at 13.5 nm wavelength. Ptychography offers a robust solution to the aforementioned challenges. Originally adapted by the electron and synchrotron communities, advances in the stability and brightness of high-harmonic tabletop sources have enabled the transfer of ptychography to the laboratory. This review covers the state of the art in tabletop ptychography with high harmonic generation sources. We consider hardware options such as illumination optics and detector concepts as well as algorithmic aspects in the analysis of multispectral ptychography data. Finally, we review technological application cases such as multispectral wavefront sensing, attosecond pulse characterization, and depth-resolved imaging.
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11
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12
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Berger E, Jamnuch S, Uzundal CB, Woodahl C, Padmanabhan H, Amado A, Manset P, Hirata Y, Kubota Y, Owada S, Tono K, Yabashi M, Wang C, Shi Y, Gopalan V, Schwartz CP, Drisdell WS, Matsuda I, Freeland JW, Pascal TA, Zuerch M. Extreme Ultraviolet Second Harmonic Generation Spectroscopy in a Polar Metal. NANO LETTERS 2021; 21:6095-6101. [PMID: 34264679 PMCID: PMC8323121 DOI: 10.1021/acs.nanolett.1c01502] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/20/2021] [Revised: 06/30/2021] [Indexed: 05/13/2023]
Abstract
The coexistence of ferroelectricity and metallicity seems paradoxical, since the itinerant electrons in metals should screen the long-range dipole interactions necessary for dipole ordering. The recent discovery of the polar metal LiOsO3 was therefore surprising [as discussed earlier in Y. Shi et al., Nat. Mater. 2013, 12, 1024]. It is thought that the coordination preferences of the Li play a key role in stabilizing the LiOsO3 polar metal phase, but an investigation from the combined viewpoints of core-state specificity and symmetry has yet to be done. Here, we apply the novel technique of extreme ultraviolet second harmonic generation (XUV-SHG) and find a sensitivity to the broken inversion symmetry in the polar metal phase of LiOsO3 with an enhanced feature above the Li K-edge that reflects the degree of Li atom displacement as corroborated by density functional theory calculations. These results pave the way for time-resolved probing of symmetry-breaking structural phase transitions on femtosecond time scales with element specificity.
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Affiliation(s)
- Emma Berger
- Department
of Chemistry, University of California, Berkeley, California 94720, United States
- Materials
Sciences Division, Lawrence Berkeley National
Laboratory, Berkeley, California 94720, United States
| | - Sasawat Jamnuch
- ATLAS
Materials Science Laboratory, Department of Nano Engineering and Chemical
Engineering, University of California−San
Diego, La Jolla, California 92023, United States
| | - Can B. Uzundal
- Department
of Chemistry, University of California, Berkeley, California 94720, United States
- Materials
Sciences Division, Lawrence Berkeley National
Laboratory, Berkeley, California 94720, United States
| | - Clarisse Woodahl
- University
of Florida, Gainesville, Florida 32611, United States
| | - Hari Padmanabhan
- Department
of Materials Science and Engineering, The
Pennsylvania State University, University Park, Pennsylvania 16801, United States
| | - Angelique Amado
- Department
of Chemistry, University of California, Berkeley, California 94720, United States
- Materials
Sciences Division, Lawrence Berkeley National
Laboratory, Berkeley, California 94720, United States
| | - Paul Manset
- Ecole Normale
Supérieure - PSL, Paris, France
| | - Yasuyuki Hirata
- National
Defense Academy of Japan, Yokosuka, Kanagawa 239-8686, Japan
| | - Yuya Kubota
- RIKEN
SPring-8 Center, Sayo, Hyogo 679-5148, Japan
- Japan
Synchrotron Radiation Research Institute (JASRI), Sayo, Hyogo 679-5198, Japan
| | - Shigeki Owada
- RIKEN
SPring-8 Center, Sayo, Hyogo 679-5148, Japan
- Japan
Synchrotron Radiation Research Institute (JASRI), Sayo, Hyogo 679-5198, Japan
| | - Kensuke Tono
- RIKEN
SPring-8 Center, Sayo, Hyogo 679-5148, Japan
- Japan
Synchrotron Radiation Research Institute (JASRI), Sayo, Hyogo 679-5198, Japan
| | - Makina Yabashi
- RIKEN
SPring-8 Center, Sayo, Hyogo 679-5148, Japan
- Japan
Synchrotron Radiation Research Institute (JASRI), Sayo, Hyogo 679-5198, Japan
| | - Cuixiang Wang
- Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
| | - Youguo Shi
- Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
| | - Venkatraman Gopalan
- Department
of Materials Science and Engineering, The
Pennsylvania State University, University Park, Pennsylvania 16801, United States
| | - Craig P. Schwartz
- Chemical
Sciences Division, Lawrence Berkeley National
Laboratory, Berkeley, California 94720, United States
| | - Walter S. Drisdell
- Chemical
Sciences Division, Lawrence Berkeley National
Laboratory, Berkeley, California 94720, United States
- Joint
Center for Artificial Photosynthesis, Lawrence
Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Iwao Matsuda
- Institute
for Solid State Physics, The University
of Tokyo, Kashiwa, Chiba 277-8581, Japan
- Trans-scale
Quantum Science Institute, The University
of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan
| | - John W. Freeland
- X-ray
Science Division, Argonne National Laboratory, Argonne, Illinois 60439, United States
| | - Tod A. Pascal
- ATLAS
Materials Science Laboratory, Department of Nano Engineering and Chemical
Engineering, University of California−San
Diego, La Jolla, California 92023, United States
- Materials
Science and Engineering, University of California−San
Diego, La Jolla, California 92023, United States
- Sustainable
Power and Energy Center, University of California−San
Diego, La Jolla, California 92023, United States
| | - Michael Zuerch
- Department
of Chemistry, University of California, Berkeley, California 94720, United States
- Materials
Sciences Division, Lawrence Berkeley National
Laboratory, Berkeley, California 94720, United States
- Fritz
Haber Institute of the Max Planck Society, 14195 Berlin, Germany
- Friedrich
Schiller University, 07743 Jena, Germany
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