2020
DOI: 10.1007/978-3-030-46906-1_13
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Imaging at the Mesoscale (LEEM, PEEM)

Abstract: TO BE PUBLISHED IN SPRINGER HANDBOOK OF SURFACE SCIENCE (SPRINGER VERLAG)TABLE OF CONTENTS 1. INTRODUCTION 2. CATHODE LENS MICROSCOPY 2.1. OPERATING PRINCIPLES 2.2. INSTRUMENTATION 2.2.1. BEAM SEPARATOR 2.2.2. ENERGY ANALYZERS 2.2.3. ABERRATION CORRECTORS 2.2.4. ELECTRON AND PHOTON SOURCES 2.3. PERFORMANCES 3. LOW ENERGY ELECTRON MICROSCOPY 3.0.1 BASIC IMAGE CONTRAST 3.0.2 IMAGE FORMATION 3.1 IMAGING MODE 3.1.1 LEEM AND LEEM-IV 3.1.2 BRIGHTFIELD AND DARKFIELD LEEM 3.1.3 MIRROR ELECTRON MICROSCOPY 3.1.4 SPIN PO… Show more

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Cited by 4 publications
(5 citation statements)
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References 126 publications
(242 reference statements)
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“…Angle-resolved photoemission spectroscopy. ARPES k // maps and electron momentum distribution curves (MDC) were collected in UHV (base p < 7 × 10 −11 mbar) using the spectroscopic photoemission and low-energy electron microscope (SPELEEM) instrument 29 that is located at the nanospectroscopy beamline of the Elettra synchrotron radiation facility, Trieste, Italy. 30 The photon beam (hn = 65 eV) was focused on the sample, and the area from which ARPES data is collected was further reduced by using a eld-limiting aperture, yielding an effective probed region of 2 mm diameter.…”
Section: Sample Preparationmentioning
confidence: 99%
“…Angle-resolved photoemission spectroscopy. ARPES k // maps and electron momentum distribution curves (MDC) were collected in UHV (base p < 7 × 10 −11 mbar) using the spectroscopic photoemission and low-energy electron microscope (SPELEEM) instrument 29 that is located at the nanospectroscopy beamline of the Elettra synchrotron radiation facility, Trieste, Italy. 30 The photon beam (hn = 65 eV) was focused on the sample, and the area from which ARPES data is collected was further reduced by using a eld-limiting aperture, yielding an effective probed region of 2 mm diameter.…”
Section: Sample Preparationmentioning
confidence: 99%
“…Photoemission spectroscopy techniques-wherein one photoemits an electron from a material using a high-energy photon and studies its properties-can provide unparalleled insight into materials and condensed matter systems. Among these, two particularly powerful and complementary techniques exist: with ARPES, the kinetic energy and emission angle of the photoemitted electron provide direct knowledge of the electronic structure of the material [121]; on the other hand, PEEM images a material's surface in real space and can deliver detailed knowledge about surface morphology, electronic and chemical properties, and magnetic structures with nanometer-scale spatial resolution [122].…”
Section: Statusmentioning
confidence: 99%
“…For example, when dimensions of a system go down to the nanoscale the uniform magnetization hypothesis is unreliable and properties become exclusive. Local regions with uniform magnetization (i.e., magnetic domains), their boundary structure (i.e., domain walls), the directions of magnetization and the magnetization extent can be revealed under both static or dynamic conditions (i.e., magnetization reversal and time-reversal behaviors) from the cryogenic cooling to high temperature [92][93][94][95].…”
Section: Imaging Of the Domain Structure And Beyondmentioning
confidence: 99%
“…Shrewd interpretation of the variety of magnetic visualization techniques is used in this section both to begin the readers who are not familiar with these techniques and to help those more expert to figure out their own matter. extent can be revealed under both static or dynamic conditions (i.e., magnetization reversal and time-reversal behaviors) from the cryogenic cooling to high temperature [92][93][94][95]. Electrons, photons, neutrons and X-rays are four kinds of modern probes offering a plethora of opportunities for the investigation of the magnetic properties (Figure 8).…”
Section: Imaging Of the Domain Structure And Beyondmentioning
confidence: 99%
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