Polarization-Resolved Extreme-Ultraviolet Second-Harmonic Generation from LiNbO_{3}.


Journal

Physical review letters
ISSN: 1079-7114
Titre abrégé: Phys Rev Lett
Pays: United States
ID NLM: 0401141

Informations de publication

Date de publication:
03 Dec 2021
Historique:
received: 02 04 2021
revised: 21 08 2021
accepted: 15 10 2021
entrez: 22 12 2021
pubmed: 23 12 2021
medline: 23 12 2021
Statut: ppublish

Résumé

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.

Identifiants

pubmed: 34936786
doi: 10.1103/PhysRevLett.127.237402
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

237402

Auteurs

Can B Uzundal (CB)

Department of Chemistry, University of California, Berkeley, California 94720, USA.
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.

Sasawat Jamnuch (S)

ATLAS Materials Science Laboratory, Department of NanoEngineering and Chemical Engineering, University of California, San Diego, La Jolla, California, 92023, USA.

Emma Berger (E)

Department of Chemistry, University of California, Berkeley, California 94720, USA.
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.

Clarisse Woodahl (C)

Department of Chemistry, University of California, Berkeley, California 94720, USA.
University of Florida, Gainesville, Florida 32611, USA.

Paul Manset (P)

Ecole Normale Superieure de Paris, Paris, France.

Yasuyuki Hirata (Y)

National Defense Academy of Japan, Yokosuka, Kanagawa 239-8686, Japan.

Toshihide Sumi (T)

Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan.

Angelique Amado (A)

Department of Chemistry, University of California, Berkeley, California 94720, USA.
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.

Hisazumi Akai (H)

Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan.

Yuya Kubota (Y)

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 (S)

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 (K)

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 (M)

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 (JW)

Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA.

Craig P Schwartz (CP)

Nevada Extreme Conditions Laboratory, University of Nevada, Las Vegas, Las Vegas, Nevada 89154, USA.

Walter S Drisdell (WS)

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 (I)

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 (TA)

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 (A)

Department of Chemistry, University of California, Berkeley, California 94720, USA.
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.

Michael Zuerch (M)

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.

Classifications MeSH