1
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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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2
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Li H, MacArthur J, Littleton S, Dunne M, Huang Z, Zhu D. Femtosecond-Terawatt Hard X-Ray Pulse Generation with Chirped Pulse Amplification on a Free Electron Laser. PHYSICAL REVIEW LETTERS 2022; 129:213901. [PMID: 36461971 DOI: 10.1103/physrevlett.129.213901] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/11/2022] [Accepted: 10/21/2022] [Indexed: 06/17/2023]
Abstract
Advances of high intensity lasers have opened up the field of strong field physics and led to a broad range of technological applications. Recent x-ray laser sources and optics development makes it possible to obtain extremely high intensity and brightness at x-ray wavelengths. In this Letter, we present a system design that implements chirped pulse amplification for hard x-ray free electron lasers. Numerical modeling with realistic experimental parameters shows that near-transform-limit single-femtosecond hard x-ray laser pulses with peak power exceeding 1 TW and brightness exceeding 4×10^{35} s^{-1} mm^{-2} mrad^{-2}0.1% bandwdith^{-1} can be consistently generated. Realization of such beam qualities is essential for establishing systematic and quantitative understanding of strong field x-ray physics and nonlinear x-ray optics phenomena.
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Affiliation(s)
- Haoyuan Li
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - James MacArthur
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - Sean Littleton
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - Mike Dunne
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - Zhirong Huang
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - Diling Zhu
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
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3
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Recovery Process from the Reversed Magnetization Simulated with a Square Lattice. E-JOURNAL OF SURFACE SCIENCE AND NANOTECHNOLOGY 2022. [DOI: 10.1380/ejssnt.2022-039] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/20/2022]
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4
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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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5
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Uzundal CB, Jamnuch S, Berger E, Woodahl C, Manset P, Hirata Y, Sumi T, Amado A, Akai H, Kubota Y, Owada S, Tono K, Yabashi M, Freeland JW, Schwartz CP, Drisdell WS, Matsuda I, Pascal TA, Zong A, Zuerch M. Polarization-Resolved Extreme-Ultraviolet Second-Harmonic Generation from LiNbO_{3}. PHYSICAL REVIEW LETTERS 2021; 127:237402. [PMID: 34936786 DOI: 10.1103/physrevlett.127.237402] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/02/2021] [Revised: 08/21/2021] [Accepted: 10/15/2021] [Indexed: 06/14/2023]
Abstract
Second harmonic generation (SHG) spectroscopy ubiquitously enables the investigation of surface chemistry, interfacial chemistry, as well as symmetry properties in solids. Polarization-resolved SHG spectroscopy in the visible to infrared regime is regularly used to investigate electronic and magnetic order through their angular anisotropies within the crystal structure. However, the increasing complexity of novel materials and emerging phenomena hampers the interpretation of experiments solely based on the investigation of hybridized valence states. Here, polarization-resolved SHG in the extreme ultraviolet (XUV-SHG) is demonstrated for the first time, enabling element-resolved angular anisotropy investigations. In noncentrosymmetric LiNbO_{3}, elemental contributions by lithium and niobium are clearly distinguished by energy dependent XUV-SHG measurements. This element-resolved and symmetry-sensitive experiment suggests that the displacement of Li ions in LiNbO_{3}, which is known to lead to ferroelectricity, is accompanied by distortions to the Nb ion environment that breaks the inversion symmetry of the NbO_{6} octahedron as well. Our simulations show that the measured second harmonic spectrum is consistent with Li ion displacements from the centrosymmetric position while the Nb─O bonds are elongated and contracted by displacements of the O atoms. In addition, the polarization-resolved measurement of XUV-SHG shows excellent agreement with numerical predictions based on dipole-induced SHG commonly used in the optical wavelengths. Our result constitutes the first verification of the dipole-based SHG model in the XUV regime. The findings of this work pave the way for future angle and time-resolved XUV-SHG studies with elemental specificity in condensed matter systems.
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Affiliation(s)
- Can B Uzundal
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - Sasawat Jamnuch
- ATLAS Materials Science Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, California, 92023, USA
| | - Emma Berger
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - Clarisse Woodahl
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- University of Florida, Gainesville, Florida 32611, USA
| | - Paul Manset
- Ecole Normale Superieure de Paris, Paris, France
| | - Yasuyuki Hirata
- National Defense Academy of Japan, Yokosuka, Kanagawa 239-8686, Japan
| | - Toshihide Sumi
- Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
| | - Angelique Amado
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - Hisazumi Akai
- Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
| | - Yuya Kubota
- RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
- Japan Synchrotron Radiation Research Institute, (JASRI), 1-1-1 Kouto, Sayo, Hyogo 679-5198, Japan
| | - Shigeki Owada
- RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
- Japan Synchrotron Radiation Research Institute, (JASRI), 1-1-1 Kouto, Sayo, Hyogo 679-5198, Japan
| | - Kensuke Tono
- RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
- Japan Synchrotron Radiation Research Institute, (JASRI), 1-1-1 Kouto, Sayo, Hyogo 679-5198, Japan
| | - Makina Yabashi
- RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
- Japan Synchrotron Radiation Research Institute, (JASRI), 1-1-1 Kouto, Sayo, Hyogo 679-5198, Japan
| | - John W Freeland
- Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA
| | - Craig P Schwartz
- Nevada Extreme Conditions Laboratory, University of Nevada, Las Vegas, Las Vegas, Nevada 89154, USA
| | - Walter S Drisdell
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Joint Center for Artificial Photosynthesis, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - 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
| | - Tod A Pascal
- ATLAS Materials Science Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, California, 92023, USA
- Materials Science and Engineering, University of California San Diego, La Jolla, California, 92023, USA
- Sustainable Power and Energy Center, University of California San Diego, La Jolla, California, 92023, USA
| | - Alfred Zong
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - Michael Zuerch
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Fritz Haber Institute of the Max Planck Society, 14195 Berlin, Germany
- Friedrich Schiller University Jena, 07743 Jena, Germany
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6
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Schwartz CP, Raj SL, Jamnuch S, Hull CJ, Miotti P, Lam RK, Nordlund D, Uzundal CB, Das Pemmaraju C, Mincigrucci R, Foglia L, Simoncig A, Coreno M, Masciovecchio C, Giannessi L, Poletto L, Principi E, Zuerch M, Pascal TA, Drisdell WS, Saykally RJ. Angstrom-Resolved Interfacial Structure in Buried Organic-Inorganic Junctions. PHYSICAL REVIEW LETTERS 2021; 127:096801. [PMID: 34506179 DOI: 10.1103/physrevlett.127.096801] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/24/2021] [Accepted: 07/02/2021] [Indexed: 06/13/2023]
Abstract
Charge transport processes at interfaces play a crucial role in many processes. Here, the first soft x-ray second harmonic generation (SXR SHG) interfacial spectrum of a buried interface (boron-Parylene N) is reported. SXR SHG shows distinct spectral features that are not observed in x-ray absorption spectra, demonstrating its extraordinary interfacial sensitivity. Comparison to electronic structure calculations indicates a boron-organic separation distance of 1.9 Å, with changes of less than 1 Å resulting in easily detectable SXR SHG spectral shifts (ca. hundreds of milli-electron volts).
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Affiliation(s)
- Craig P Schwartz
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - Sumana L Raj
- Department of Chemistry, University of California, Berkeley, California 94720, USA
| | - Sasawat Jamnuch
- ATLAS Materials Science Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, California 92023, USA
| | - Chris J Hull
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Department of Chemistry, University of California, Berkeley, California 94720, USA
| | - Paolo Miotti
- Institute of Photonics and Nanotechnologies, National Research Council of Italy, via Trasea 7, I-35131 Padova, Italy
- Department of Information Engineering, University of Padova, via Gradenigo 6/B, I-35131 Padova, Italy
| | - Royce K Lam
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Department of Chemistry, University of California, Berkeley, California 94720, USA
| | - Dennis Nordlund
- Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - Can B Uzundal
- Department of Chemistry, University of California, Berkeley, California 94720, USA
| | - Chaitanya Das Pemmaraju
- Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - Riccardo Mincigrucci
- Elettra-Sincrotrone Trieste S.C.p.A., Strada Statale 14-km 163.5, 34149 Trieste, Italy
| | - Laura Foglia
- Elettra-Sincrotrone Trieste S.C.p.A., Strada Statale 14-km 163.5, 34149 Trieste, Italy
| | - Alberto Simoncig
- Elettra-Sincrotrone Trieste S.C.p.A., Strada Statale 14-km 163.5, 34149 Trieste, Italy
| | - Marcello Coreno
- ISM-CNR, Istituto di Struttura della Materia, LD2 Unit, 34149 Trieste, Italy
- Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Frascati, Via E. Fermi 54, 00044 Frascati, Italy
| | - Claudio Masciovecchio
- Elettra-Sincrotrone Trieste S.C.p.A., Strada Statale 14-km 163.5, 34149 Trieste, Italy
| | - Luca Giannessi
- Elettra-Sincrotrone Trieste S.C.p.A., Strada Statale 14-km 163.5, 34149 Trieste, Italy
- Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Frascati, Via E. Fermi 54, 00044 Frascati, Italy
| | - Luca Poletto
- Institute of Photonics and Nanotechnologies, National Research Council of Italy, via Trasea 7, I-35131 Padova, Italy
| | - Emiliano Principi
- Elettra-Sincrotrone Trieste S.C.p.A., Strada Statale 14-km 163.5, 34149 Trieste, Italy
| | - Michael Zuerch
- Department of Chemistry, University of California, Berkeley, California 94720, USA
- Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Institute for Optics and Quantum Electronics, Abbe Center of Photonics, University of Jena, 07745 Jena, Germany
- Fritz Haber Institute of the Max Planck Society, 14195 Berlin, Germany
| | - Tod A Pascal
- ATLAS Materials Science Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, California 92023, USA
- Materials Science and Engineering, University of California San Diego, La Jolla, California 92023, USA
- Sustainable Power and Energy Center, University of California San Diego, La Jolla, California 92023, USA
| | - Walter S Drisdell
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Joint Center for Artificial Photosynthesis, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - Richard J Saykally
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
- Department of Chemistry, University of California, Berkeley, California 94720, USA
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7
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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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8
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Matsuda I, Kubota Y. Recent Progress in Spectroscopies Using Soft X-ray Free-electron Lasers. CHEM LETT 2021. [DOI: 10.1246/cl.200881] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/14/2022]
Affiliation(s)
- Iwao Matsuda
- The Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan
- Trans-scale Quantum Science Institute, The University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan
| | - Yuya Kubota
- RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
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9
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Helk T, Berger E, Jamnuch S, Hoffmann L, Kabacinski A, Gautier J, Tissandier F, Goddet JP, Chang HT, Oh J, Pemmaraju CD, Pascal TA, Sebban S, Spielmann C, Zuerch M. Table-top extreme ultraviolet second harmonic generation. SCIENCE ADVANCES 2021; 7:7/21/eabe2265. [PMID: 34138744 PMCID: PMC8133706 DOI: 10.1126/sciadv.abe2265] [Citation(s) in RCA: 9] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/02/2020] [Accepted: 03/30/2021] [Indexed: 05/27/2023]
Abstract
The lack of available table-top extreme ultraviolet (XUV) sources with high enough fluxes and coherence properties has limited the availability of nonlinear XUV and x-ray spectroscopies to free-electron lasers (FELs). Here, we demonstrate second harmonic generation (SHG) on a table-top XUV source by observing SHG near the Ti M2,3 edge with a high-harmonic seeded soft x-ray laser. Furthermore, this experiment represents the first SHG experiment in the XUV. First-principles electronic structure calculations suggest the surface specificity and separate the observed signal into its resonant and nonresonant contributions. The realization of XUV-SHG on a table-top source opens up more accessible opportunities for the study of element-specific dynamics in multicomponent systems where surface, interfacial, and bulk-phase asymmetries play a driving role.
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Affiliation(s)
- Tobias Helk
- Institute of Optics and Quantum Electronics, Abbe Center of Photonics, Friedrich-Schiller University, 07743 Jena, Germany.
- Helmholtz Institute Jena, 07743 Jena, Germany
| | - Emma Berger
- Department of Chemistry, University of California, Berkeley, Berkeley, CA 94720, USA
- Materials Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
| | - Sasawat Jamnuch
- ATLAS Materials Physics Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, CA 92023, USA
| | - Lars Hoffmann
- Fritz Haber Institute of the Max Planck Society, 14195 Berlin, Germany
| | - Adeline Kabacinski
- Laboratoire d'Optique Appliquée, ENSTA Paris, Ecole Polytechnique, CNRS, Institut Polytechnique de Paris, Palaiseau, France
| | - Julien Gautier
- Laboratoire d'Optique Appliquée, ENSTA Paris, Ecole Polytechnique, CNRS, Institut Polytechnique de Paris, Palaiseau, France
| | - Fabien Tissandier
- Laboratoire d'Optique Appliquée, ENSTA Paris, Ecole Polytechnique, CNRS, Institut Polytechnique de Paris, Palaiseau, France
| | - Jean-Philipe Goddet
- Laboratoire d'Optique Appliquée, ENSTA Paris, Ecole Polytechnique, CNRS, Institut Polytechnique de Paris, Palaiseau, France
| | - Hung-Tzu Chang
- Department of Chemistry, University of California, Berkeley, Berkeley, CA 94720, USA
| | - Juwon Oh
- Department of Chemistry, University of California, Berkeley, Berkeley, CA 94720, USA
| | - C Das Pemmaraju
- Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford, CA 94025, USA
| | - Tod A Pascal
- ATLAS Materials Physics Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, CA 92023, USA
- Materials Science and Engineering, University of California, San Diego, La Jolla, CA 92023, USA
- Sustainable Power and Energy Center, University of California, San Diego, La Jolla, CA 92023, USA
| | - Stephane Sebban
- Laboratoire d'Optique Appliquée, ENSTA Paris, Ecole Polytechnique, CNRS, Institut Polytechnique de Paris, Palaiseau, France
| | - Christian Spielmann
- Institute of Optics and Quantum Electronics, Abbe Center of Photonics, Friedrich-Schiller University, 07743 Jena, Germany.
- Helmholtz Institute Jena, 07743 Jena, Germany
| | - Michael Zuerch
- Institute of Optics and Quantum Electronics, Abbe Center of Photonics, Friedrich-Schiller University, 07743 Jena, Germany.
- Department of Chemistry, University of California, Berkeley, Berkeley, CA 94720, USA
- Materials Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
- Fritz Haber Institute of the Max Planck Society, 14195 Berlin, Germany
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Ellipsometer Equipped with Multiple Mirrors for Element-selective Soft X-ray Experiments. E-JOURNAL OF SURFACE SCIENCE AND NANOTECHNOLOGY 2020. [DOI: 10.1380/ejssnt.2020.231] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/20/2022]
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11
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Egawa S, Owada S, Motoyama H, Yamaguchi G, Matsuzawa Y, Kume T, Kubota Y, Tono K, Yabashi M, Ohashi H, Mimura H. Full-field microscope with twin Wolter mirrors for soft X-ray free-electron lasers. OPTICS EXPRESS 2019; 27:33889-33897. [PMID: 31878448 DOI: 10.1364/oe.27.033889] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/12/2019] [Accepted: 10/21/2019] [Indexed: 06/10/2023]
Abstract
We developed a full-field microscope with twin Wolter mirrors for soft X-ray free-electron lasers. The Wolter mirrors for a condenser and an objective were fabricated using an electroforming process with a precisely figured master mandrel. In the imaging system constructed at SACLA BL1, sub-micrometer spatial resolution was achieved at wavelengths of 10.3 and 3.4 nm. Single-shot bright-field images were acquired with a maximum illumination intensity of 7×1014 W/cm2.
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12
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Yang G, Li LH, Wu C, Humphrey MG, Zhang C. Ionothermal Synthesis of Metal Chalcogenides M 2Ag 3Sb 3S 7 (M = Rb, Cs) Displaying Nonlinear Optical Activity in the Infrared Region. Inorg Chem 2019; 58:12582-12589. [PMID: 31553591 DOI: 10.1021/acs.inorgchem.9b01262] [Citation(s) in RCA: 15] [Impact Index Per Article: 2.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/28/2022]
Abstract
Two interesting non-centrosymmetric metal chalcogenides, Rb2Ag3Sb3S7 and Cs2Ag3Sb3S7, were synthesized by an ionothermal approach. Crystals of compounds Rb2Ag3Sb3S7 and Cs2Ag3Sb3S7 possess isomorphic configuration, consisting of two-dimensional (2D) anionic networks ∞[Ag3Sb3S7]2-, which are split by alkali-metal M+ cations. The band gaps are 2.11 and 2.02 eV for Rb2Ag3Sb3S7 and Cs2Ag3Sb3S7, respectively. Second-harmonic generation (SHG) studies revealed that Rb2Ag3Sb3S7 affords a powder SHG performance of ∼0.5 × AgGaS2 with type-I phase matching, while Cs2Ag3Sb3S7 shows a slightly stronger SHG performance of ∼0.6 × AgGaS2 with type-I phase matching. Both compounds possess broad transparency ranges (∼0.6-20 μm), suggesting their potential as infrared (IR) nonlinear optical (NLO) materials. The laser damage thresholds (LDTs) of both Rb2Ag3Sb3S7 and Cs2Ag3Sb3S7 are about 2.3 × AgGaS2. The calculated birefringence indexes Δn are 0.1885 and 0.1944 at 1.064 μm, respectively, which are sufficiently large enough to achieve phase matching. Theoretical studies using density functional theory have been implemented to further understand the relationship between their NLO properties and band structures.
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Affiliation(s)
- Gang Yang
- China-Australia Joint Research Center for Functional Molecular Materials, School of Chemical and Material Engineering , Jiangnan University , Wuxi 214122 , P. R. China.,School of Chemical Science and Engineering , Tongji University , Shanghai 200092 , P. R. China
| | - Long-Hua Li
- School of Chemistry and Chemical Engineering , Jiangsu University , Zhenjiang 212013 , P. R. China
| | - Chao Wu
- School of Chemical Science and Engineering , Tongji University , Shanghai 200092 , P. R. China
| | - Mark G Humphrey
- School of Chemical Science and Engineering , Tongji University , Shanghai 200092 , P. R. China.,Research School of Chemistry , Australian National University , Canberra , ACT 2601 , Australia
| | - Chi Zhang
- China-Australia Joint Research Center for Functional Molecular Materials, School of Chemical and Material Engineering , Jiangnan University , Wuxi 214122 , P. R. China.,School of Chemical Science and Engineering , Tongji University , Shanghai 200092 , P. R. China
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13
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Owada S, Nakajima K, Togashi T, Katayama T, Yumoto H, Ohashi H, Yabashi M. Arrival timing diagnostics at a soft X-ray free-electron laser beamline of SACLA BL1. JOURNAL OF SYNCHROTRON RADIATION 2019; 26:887-890. [PMID: 31074453 PMCID: PMC6510193 DOI: 10.1107/s1600577519002315] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 10/04/2018] [Accepted: 02/12/2019] [Indexed: 06/09/2023]
Abstract
An arrival timing monitor for the soft X-ray free-electron laser (XFEL) beamline of SACLA BL1 has been developed. A small portion of the soft XFEL pulse is branched using the wavefront-splitting method. The branched FEL pulse is one-dimensionally focused onto a GaAs wafer to induce a transient reflectivity change. The beam branching method enables the simultaneous operation of the arrival timing diagnostics and experiments. The temporal resolution evaluated from the imaging system is ∼22 fs in full width at half-maximum, which is sufficient considering the temporal durations of the soft XFEL and the optical laser pulses.
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Affiliation(s)
- Shigeki Owada
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
| | - Kyo Nakajima
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
| | - Tadashi Togashi
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
| | - Tetsuo Katayama
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
| | - Hirokatsu Yumoto
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
| | - Haruhiko Ohashi
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
| | - Makina Yabashi
- Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun 6795198, Japan
- RIKEN SPring-8 Center, Sayo-cho, Sayo-gun 6795148, Japan
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14
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Beye M, Engel RY, Schunck JO, Dziarzhytski S, Brenner G, Miedema PS. Non-linear soft x-ray methods on solids with MUSIX-the multi-dimensional spectroscopy and inelastic x-ray scattering endstation. JOURNAL OF PHYSICS. CONDENSED MATTER : AN INSTITUTE OF PHYSICS JOURNAL 2019; 31:014003. [PMID: 30504529 DOI: 10.1088/1361-648x/aaedf3] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
With the intense and coherent x-ray pulses available from free-electron lasers, the possibility to transfer non-linear spectroscopic methods from the laser lab to the x-ray world arises. Advantages especially regarding selectivity and thus information content as well as an improvement of signal levels are expected. The use of coherences is especially fruitful and the example of coherent x-ray/optical sum-frequency generation is discussed. However, many non-linear x-ray methods still await discovery, partially due to the necessity for extremely adaptable and versatile instrumentation that can be brought to free-electron lasers for the analysis of the spectral content emitted from the sample into a continuous range of emission angles. Such an instrument (called MUSIX) is being developed and employed at FLASH, the free-electron laser in Hamburg and is described in this contribution together with first results.
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Affiliation(s)
- M Beye
- Deutsches Elektronen Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany. Physics Department, Universität Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany
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