Matthias Schmitt , Deepnarayan Biswas , Olena Tkach , Olena Fedchenko , Jieyi Liu , Hans-Joachim Elmers , Michael Sing , Ralph Claessen , Tien-Lin Lee , Gerd Schönhense
{"title":"在金刚石光源的软x射线光束线I09上,结合半球形和飞行时间电子分析仪的动量显微镜","authors":"Matthias Schmitt , Deepnarayan Biswas , Olena Tkach , Olena Fedchenko , Jieyi Liu , Hans-Joachim Elmers , Michael Sing , Ralph Claessen , Tien-Lin Lee , Gerd Schönhense","doi":"10.1016/j.ultramic.2025.114169","DOIUrl":null,"url":null,"abstract":"<div><div>The three-dimensional recording scheme of time-of-flight momentum microscopes (ToF-MMs) is advantageous for fast mapping of the photoelectron distribution in (<em>E</em>,<strong><em>k</em></strong>) parameter space over the entire Brillouin zone. However, the 2 ns pulse period of most synchrotrons is too short for pure ToF photoelectron spectroscopy. The use of a hemispherical analyzer (HSA) as a pre-filter allows ToF-MM at such high pulse rates. The first HSA & ToF hybrid MM is operated at the soft X-ray branch of beamline I09 at the Diamond Light Source, UK. The photon energy ranges from 105 eV to 2 keV, with circular polarization available for hν ≥ 145 eV. The HSA reduces the transmitted energy band to typically 0.5 eV, which is then further analyzed by ToF recording. In initial experiments, the overall efficiency gain when switching from the standard 2D (<em>k</em><sub>x</sub>,<em>k</em><sub>y</sub>) mode to the 3D (<em>k</em><sub>x</sub>,<em>k</em><sub>y</sub>,<em>E</em><sub>kin</sub>) hybrid mode was about 24. This value is determined by the number of resolved kinetic energies (here 12) and the transmission gain of the electron optics due to the high pass energy of the HSA in hybrid mode (<em>E</em><sub>pass</sub> up to 500 eV). The transmission gain depends on the size of the photon footprint on the sample. Under <em>k</em>-imaging conditions, the energy and momentum resolution are 10.2 meV (FWHM) (4.2 meV with 200 μm slits and <em>E</em><sub>pass</sub> = 8 eV) and 0.010 Å<sup>-1</sup>. The energy filtered X-PEEM mode showed a spatial resolution of 250 nm. As examples, we show 2D band mapping of bilayer graphene, 3D mapping of the Fermi surface of Cu, circular dichroic ARPES for intercalated indenene layers, and the <em>sp</em> valence band of Au. Full-field photoelectron diffraction patterns of Ge show rich structure in <em>k</em>-field diameters of up to 6 Å<sup>-1</sup>.</div></div>","PeriodicalId":23439,"journal":{"name":"Ultramicroscopy","volume":"276 ","pages":"Article 114169"},"PeriodicalIF":2.0000,"publicationDate":"2025-05-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Momentum microscopy with combined hemispherical and time-of-flight electron analyzers at the soft X-ray beamline I09 of the diamond light source\",\"authors\":\"Matthias Schmitt , Deepnarayan Biswas , Olena Tkach , Olena Fedchenko , Jieyi Liu , Hans-Joachim Elmers , Michael Sing , Ralph Claessen , Tien-Lin Lee , Gerd Schönhense\",\"doi\":\"10.1016/j.ultramic.2025.114169\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>The three-dimensional recording scheme of time-of-flight momentum microscopes (ToF-MMs) is advantageous for fast mapping of the photoelectron distribution in (<em>E</em>,<strong><em>k</em></strong>) parameter space over the entire Brillouin zone. However, the 2 ns pulse period of most synchrotrons is too short for pure ToF photoelectron spectroscopy. The use of a hemispherical analyzer (HSA) as a pre-filter allows ToF-MM at such high pulse rates. The first HSA & ToF hybrid MM is operated at the soft X-ray branch of beamline I09 at the Diamond Light Source, UK. The photon energy ranges from 105 eV to 2 keV, with circular polarization available for hν ≥ 145 eV. The HSA reduces the transmitted energy band to typically 0.5 eV, which is then further analyzed by ToF recording. In initial experiments, the overall efficiency gain when switching from the standard 2D (<em>k</em><sub>x</sub>,<em>k</em><sub>y</sub>) mode to the 3D (<em>k</em><sub>x</sub>,<em>k</em><sub>y</sub>,<em>E</em><sub>kin</sub>) hybrid mode was about 24. This value is determined by the number of resolved kinetic energies (here 12) and the transmission gain of the electron optics due to the high pass energy of the HSA in hybrid mode (<em>E</em><sub>pass</sub> up to 500 eV). The transmission gain depends on the size of the photon footprint on the sample. Under <em>k</em>-imaging conditions, the energy and momentum resolution are 10.2 meV (FWHM) (4.2 meV with 200 μm slits and <em>E</em><sub>pass</sub> = 8 eV) and 0.010 Å<sup>-1</sup>. The energy filtered X-PEEM mode showed a spatial resolution of 250 nm. As examples, we show 2D band mapping of bilayer graphene, 3D mapping of the Fermi surface of Cu, circular dichroic ARPES for intercalated indenene layers, and the <em>sp</em> valence band of Au. Full-field photoelectron diffraction patterns of Ge show rich structure in <em>k</em>-field diameters of up to 6 Å<sup>-1</sup>.</div></div>\",\"PeriodicalId\":23439,\"journal\":{\"name\":\"Ultramicroscopy\",\"volume\":\"276 \",\"pages\":\"Article 114169\"},\"PeriodicalIF\":2.0000,\"publicationDate\":\"2025-05-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Ultramicroscopy\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0304399125000658\",\"RegionNum\":3,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MICROSCOPY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Ultramicroscopy","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0304399125000658","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MICROSCOPY","Score":null,"Total":0}
Momentum microscopy with combined hemispherical and time-of-flight electron analyzers at the soft X-ray beamline I09 of the diamond light source
The three-dimensional recording scheme of time-of-flight momentum microscopes (ToF-MMs) is advantageous for fast mapping of the photoelectron distribution in (E,k) parameter space over the entire Brillouin zone. However, the 2 ns pulse period of most synchrotrons is too short for pure ToF photoelectron spectroscopy. The use of a hemispherical analyzer (HSA) as a pre-filter allows ToF-MM at such high pulse rates. The first HSA & ToF hybrid MM is operated at the soft X-ray branch of beamline I09 at the Diamond Light Source, UK. The photon energy ranges from 105 eV to 2 keV, with circular polarization available for hν ≥ 145 eV. The HSA reduces the transmitted energy band to typically 0.5 eV, which is then further analyzed by ToF recording. In initial experiments, the overall efficiency gain when switching from the standard 2D (kx,ky) mode to the 3D (kx,ky,Ekin) hybrid mode was about 24. This value is determined by the number of resolved kinetic energies (here 12) and the transmission gain of the electron optics due to the high pass energy of the HSA in hybrid mode (Epass up to 500 eV). The transmission gain depends on the size of the photon footprint on the sample. Under k-imaging conditions, the energy and momentum resolution are 10.2 meV (FWHM) (4.2 meV with 200 μm slits and Epass = 8 eV) and 0.010 Å-1. The energy filtered X-PEEM mode showed a spatial resolution of 250 nm. As examples, we show 2D band mapping of bilayer graphene, 3D mapping of the Fermi surface of Cu, circular dichroic ARPES for intercalated indenene layers, and the sp valence band of Au. Full-field photoelectron diffraction patterns of Ge show rich structure in k-field diameters of up to 6 Å-1.
期刊介绍:
Ultramicroscopy is an established journal that provides a forum for the publication of original research papers, invited reviews and rapid communications. The scope of Ultramicroscopy is to describe advances in instrumentation, methods and theory related to all modes of microscopical imaging, diffraction and spectroscopy in the life and physical sciences.