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Journal articles on the topic 'Low energy electron diffraction. Surfaces (Physics)'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Starke, U., J. B. Pendry, and K. Heinz. "Diffuse low-energy electron diffraction." Progress in Surface Science 52, no. 2 (1996): 53–124. http://dx.doi.org/10.1016/0079-6816(96)00007-x.

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2

Diehl, R. D., J. Ledieu, N. Ferralis, A. W. Szmodis, and R. McGrath. "Low-energy electron diffraction from quasicrystal surfaces." Journal of Physics: Condensed Matter 15, no. 3 (2003): R63—R81. http://dx.doi.org/10.1088/0953-8984/15/3/201.

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3

McRae, EC, and RA Malic. "Applications of Low-energy Electron Diffraction to Ordering at Crystal and Quasicrystal Surfaces." Australian Journal of Physics 43, no. 5 (1990): 499. http://dx.doi.org/10.1071/ph900499.

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The value of the low-energy electron diffraction (LEED) technique for the evaluation of surface ordering depends on the ability to measure the intensity profiles of diffraction beams with respect to the associated surface component of the electron momentum transfer. Beam profiles, if measured with sufficient accuracy, may be interpreted to characterise the extent of surface order (e.g. distribution of step spacings) and to differentiate between different modes of disordering (e.g. surface melting versus roughening). The ability to measure LEED intensity profiles has been enhanced by use of low

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4

Wedler, Harald, and Klaus Heinz. "Information on Surface Structure by Low Energy Electron Diffraction." Vakuum in Forschung und Praxis 7, no. 2 (1995): 107–14. http://dx.doi.org/10.1002/vipr.19950070205.

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5

Tromp, R. M., M. Mankos, M. C. Reuter, A. W. Ellis, and M. Copel. "A New Low Energy Electron Microscope." Surface Review and Letters 05, no. 06 (1998): 1189–97. http://dx.doi.org/10.1142/s0218625x98001523.

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Low energy electron microscopy (LEEM) has developed into one of the premier techniques for in situ studies of surface dynamical processes, such as epitaxial growth, phase transitions, chemisorption and strain relaxation phenomena. Over the last three years we have designed and constructed a new LEEM instrument, aimed at improved resolution, improved diffraction capabilities and greater ease of operation compared to present instruments.

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6

BONDARCHUCK, O., S. GOYSA, I. KOVAL, P. MEL'NIK, and M. NAKHODKIN. "SHORT-RANGE ORDER OF DISORDERED SOLID SURFACES FROM ELASTICALLY SCATTERED ELECTRON SPECTRA." Surface Review and Letters 04, no. 05 (1997): 965–67. http://dx.doi.org/10.1142/s0218625x97001139.

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The diffraction phenomenon of low- and middle-energy electrons for disordered solid surfaces was experimentally studied and a new electron spectroscopy technique for surface short-range order parameter determination proposed.

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7

TONG, S. Y., T. P. CHU, HUASHENG WU, and H. HUANG. "LOW-ENERGY ELECTRON HOLOGRAMS: PROPERTIES AND METHOD OF INVERSION." Surface Review and Letters 04, no. 03 (1997): 459–67. http://dx.doi.org/10.1142/s0218625x97000444.

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We examine the differences between low-energy electron-diffraction patterns (holograms) and optical holograms. We show that electron-diffraction patterns in solids are not analogous to optical holograms because of strong dynamical factors. We also show that low-energy electron holograms can be inverted by a large-wave-number small-angle integral transformation. The grid sizes in wave number and angular spaces used in the transformation are derived.

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8

Clarke, L. J., and Paul M. Marcus. "Surface Crystallography: An Introduction to Low Energy Electron Diffraction." Physics Today 40, no. 4 (1987): 83–84. http://dx.doi.org/10.1063/1.2819989.

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9

Moritz, W., J. Landskron, and M. Deschauer. "Perspectives for surface structure analysis with low energy electron diffraction." Surface Science 603, no. 10-12 (2009): 1306–14. http://dx.doi.org/10.1016/j.susc.2008.11.041.

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10

Fisher, P. J., Luxmi, N. Srivastava, S. Nie, and R. M. Feenstra. "Thickness monitoring of graphene on SiC using low-energy electron diffraction." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 28, no. 4 (2010): 958–62. http://dx.doi.org/10.1116/1.3301621.

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11

Liew, Y. F., and G. C. Wang. "High resolution low energy electron diffraction characterization of reconstructed Au(001) surfaces." Surface Science 227, no. 3 (1990): 190–96. http://dx.doi.org/10.1016/s0039-6028(05)80006-8.

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12

Pfnür, H., M. Lindroos, and D. Menzel. "Investigation of adsorbates with low energy electron diffraction at very low energies (VLEED)." Surface Science 248, no. 1-2 (1991): 1–10. http://dx.doi.org/10.1016/0039-6028(91)90055-w.

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13

Poon, H. C., S. Y. Tong, W. F. Chung, and M. S. Altman. "Low Energy Electron Diffraction Analysis of Ultrathin Ag Films on W(110)." Surface Review and Letters 05, no. 06 (1998): 1143–49. http://dx.doi.org/10.1142/s0218625x9800147x.

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We have measured low energy electron diffraction data for clean W(110), ultrathin and thick Ag films on W(110). The data are analyzed by full dynamical multiple scattering calculations to determine the structure of the Ag-film/W(110) system. The multiple scattering calculation takes into account the incommensurate scattering between the non-pseudomorphic Ag films and the W(110) substrate. We have examined the effect of dynamical inputs used in the calculation. We find that for normally incident electrons, the surface barrier at the vacuum-film interface and the inelastic damping modify mainly

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14

Abu-Samak, Mahmoud, P. Fantini, S. Gardonio, E. Magnano та C. Mariani. "Photoemission and Low-Energy Electron-Diffraction Studies of α-Sn Growth on InSb Surfaces". Physica Scripta 71, № 6 (2005): 652–55. http://dx.doi.org/10.1088/0031-8949/71/6/013.

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15

Cho, Eun-Sang, Hoon Hur, Nam-Hong Kim, et al. "Phases of Ag-Adsorbed Si Surfaces Studied by Low Energy Electron Diffraction and Auger Electron Spectroscopy." Japanese Journal of Applied Physics 42, Part 1, No. 9A (2003): 5536–38. http://dx.doi.org/10.1143/jjap.42.5536.

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16

Martin, P., Pv Blanckenhagen, U. Romahn, and W. Schommers. "The role of the renninger effect in low energy electron diffraction." Vacuum 41, no. 1-3 (1990): 349–51. http://dx.doi.org/10.1016/0042-207x(90)90355-3.

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17

Chamberlin, S. E., C. J. Hirschmugl, H. C. Poon, and D. K. Saldin. "Geometric structure of (011)(21) surface by low energy electron diffraction (LEED)." Surface Science 603, no. 23 (2009): 3367–73. http://dx.doi.org/10.1016/j.susc.2009.09.029.

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18

Cai, M., S. C. Langford, J. T. Dickinson, and L. E. Levine. "Deformation of cube-textured aluminum studied using laser-induced photoelectron emission." Journal of Materials Research 22, no. 9 (2007): 2582–89. http://dx.doi.org/10.1557/jmr.2007.0313.

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The evolution of the kinetic energy distribution of photoelectrons from a cube-oriented aluminum sample during tensile deformation was probed with a retarding field energy analyzer. Because of the anisotropy of the aluminum work function, the electron-energy distribution is altered as the area fractions of the major surface planes change during deformation. In cube-textured aluminum, deformation reduces the {100} area fraction and the relatively low energy electrons from these surfaces. Conversely, the {110} and {111} area fractions and the relatively high energy electrons from these surfaces

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19

MORITZ, W., J. LANDSKRON, and T. GRÜNBERG. "ANALYSIS OF THERMAL VIBRATIONS AND INCOMMENSURATE LAYERS BY LOW ENERGY ELECTRON DIFFRACTION." Surface Review and Letters 04, no. 03 (1997): 469–78. http://dx.doi.org/10.1142/s0218625x97000456.

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The multiple scattering theory of LEED is briefly reviewed, and recent developments concerning the analysis of thermal vibrations with LEED and the analysis of lattice modulations in incommensurate layers are discussed. Usually only isotropic thermal vibrations have been considered in LEED structure analyses. This restriction can be overcome by an extension of the theory to anisotropic and anharmonic vibrations, allowing not only a higher precision in the determination of structure parameters but also the study of dynamical processes with LEED. In the case of incommensurate layers the satellit

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20

Janzen, O., C. Hahn, T. U. Kampen, and W. Mönch. "Explanation of multiplet spots in low-energy electron diffraction patterns of clean GaN surfaces." European Physical Journal B 7, no. 1 (1999): 1–4. http://dx.doi.org/10.1007/s100510050583.

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21

TURTON, S., M. KADODWALA, and ROBERT G. JONES. "POSSIBLE "HOT" MOLECULE DESORPTION BY ELECTRON STIMULATED DECOMPOSITION OF DIHALOETHANES ON Cu(111)." Surface Review and Letters 01, no. 04 (1994): 535–38. http://dx.doi.org/10.1142/s0218625x94000606.

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The desorption of ethene from physisorbed 1, 2-dichloroethane (DCE) and 1-bromo-2-chloroethane (BCE) on Cu(111) has been observed on irradiating the surface with electrons. The techniques used were low energy electron diffraction (LEED), Auger electron spectroscopy (AES), ultraviolet photoelectron spectroscopy (UPS), and mass spectrometric detection of the desorbed species. At 110 K physisorbed DCE and BCE underwent electron capture from low energy (<1 eV ) electrons in the secondary electron yield of the surface followed by decomposition and desorption of ethene alone. The decomposition wa

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22

MATSUMOTO, Masuaki, Syohei OGURA, Katsuyuki FUKUTANI, Tatsuo OKANO, and Michio OKADA. "Dynamical Low-energy Electron Diffraction Analyses of Clean and H-adsorbed Ir(111) Surfaces." Shinku 49, no. 5 (2006): 313–16. http://dx.doi.org/10.3131/jvsj.49.313.

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23

Pussi, K., J. Smerdon, N. Ferralis, M. Lindroos, R. McGrath, and R. D. Diehl. "Dynamical low-energy electron diffraction study of graphite (0001)-(√3×√3)R30°-Xe." Surface Science 548, no. 1-3 (2004): 157–62. http://dx.doi.org/10.1016/j.susc.2003.11.001.

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24

LAN TIAN and XU FEI-YUE. "A STUDY OF GaAs(110) SURFACE RELAXATION WITH LOW-ENERGY-ELECTRON-DIFFRACTION." Acta Physica Sinica 38, no. 3 (1989): 357. http://dx.doi.org/10.7498/aps.38.357.

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25

Watson, Philip R. "Critical Compilation of Surface Structures Determined by Low‐Energy Electron Diffraction Crystallography." Journal of Physical and Chemical Reference Data 16, no. 4 (1987): 953–92. http://dx.doi.org/10.1063/1.555797.

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26

Villegas, Ignacio, Charles B. Ehlers, and John L. Stickney. "Ordering of Copper Single‐Crystal Surfaces in Solution: Confirmation by Low Energy Electron Diffraction." Journal of The Electrochemical Society 137, no. 10 (1990): 3143–48. http://dx.doi.org/10.1149/1.2086174.

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27

Li, Zhenjun, Octavio Furlong, Florencia Calaza, et al. "Surface segregation of gold for Au/Pd(111) alloys measured by low-energy electron diffraction and low-energy ion scattering." Surface Science 602, no. 5 (2008): 1084–91. http://dx.doi.org/10.1016/j.susc.2008.01.019.

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28

Yoshitake, Michiko, Santanu Bera, Yasuhiro Yamauchi, and Weijie Song. "Oxygen adsorption on Cu–9 at. %Al(111) studied by low energy electron diffraction and Auger electron spectroscopy." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 21, no. 4 (2003): 1290–93. http://dx.doi.org/10.1116/1.1560719.

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29

Bittencourt, C., E. A. Soares, and D. P. Woodruff. "Low energy electron diffraction structure determination of the Nic(2×2)–CN surface phase." Surface Science 526, no. 1-2 (2003): 33–43. http://dx.doi.org/10.1016/s0039-6028(02)02676-6.

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30

YU, Z. X., S. Y. TONG, SHIHONG XU, SIMON MA, and HUASHENG WU. "STRUCTURE DETERMINATION OF THE 1 × 1GaN(0001) SURFACE BY QUANTITATIVE LOW ENERGY ELECTRON DIFFRACTION." Surface Review and Letters 10, no. 06 (2003): 831–36. http://dx.doi.org/10.1142/s0218625x03005657.

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A quantitative structural determination of the Ga-polar 1×1 (0001) surface of GaN is performed by quantitative low energy electron diffraction (LEED). The global best-fit structure is obtained by a new frozen LEED approach connected to a simulated annealing algorithm. The global minimization frozen (GMF) LEED search finds that the ordered structure consists of 1 ML of Ga adatoms at atop sites above Ga-terminated bilayers. The Ga adatoms are bonded with a Ga–Ga bond length of 2.51 Å. The spacings within surface bilayers show a weak oscillatory trend, with the outmost bilayer thickness expanding

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31

Schindler, K. M., J. Wang, A. Chassé, H. Neddermeyer, and W. Widdra. "Low-energy electron diffraction structure determination of an ultrathin CoO film on Ag(001)." Surface Science 603, no. 16 (2009): 2658–63. http://dx.doi.org/10.1016/j.susc.2009.06.020.

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32

Kawahara, K., T. Shirasawa, R. Arafune, et al. "Determination of atomic positions in silicene on Ag(111) by low-energy electron diffraction." Surface Science 623 (May 2014): 25–28. http://dx.doi.org/10.1016/j.susc.2013.12.013.

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33

Ahmed, Rezwan, Takeshi Nakagawa, and Seigi Mizuno. "Structure determination of ultra-flat stanene on Cu(111) using low energy electron diffraction." Surface Science 691 (January 2020): 121498. http://dx.doi.org/10.1016/j.susc.2019.121498.

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34

BARTOŠ, I., P. JAROŠ, A. BARBIERI, et al. "Cu(111) SURFACE RELAXATION BY VLEED." Surface Review and Letters 02, no. 04 (1995): 477–82. http://dx.doi.org/10.1142/s0218625x95000431.

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Very-low-energy electron diffraction (VLEED) intensities from a clean Cu (111) surface have been measured in detail in the energy range 15–100 eV by low-energy electron microscope (LEEM). This enabled the elimination of possible disturbances due to stray magnetic fields. Corresponding theoretical I–V curves have been obtained in good agreement with experimental data when an image-type surface barrier and anisotropy of the electron attenuation were taken into account. The reliability factor analysis indicates a slight expansion of the topmost interatomic spacing of Cu (111) relative to its bulk

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35

Bender, M., D. Ehrlich, I. N. Yakovkin, et al. "Structural rearrangement and surface magnetism on oxide surfaces: a temperature-dependent low-energy electron diffraction-electron energy loss spectroscopy study of Cr2O3(111)/Cr(110)." Journal of Physics: Condensed Matter 7, no. 27 (1995): 5289–301. http://dx.doi.org/10.1088/0953-8984/7/27/014.

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36

FONDA, L. "EMISSION ELECTRON DIFFRACTION AND HOLOGRAPHY: A THEORETICAL SURVEY." Surface Review and Letters 03, no. 04 (1996): 1603–26. http://dx.doi.org/10.1142/s0218625x9600259x.

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The first part of this article reviews emission electron diffraction, a very powerful tool for investigating short order surface structures. Within the standard single particle approach, the correct multiple scattering formalism and its single scattering cluster, plane and spherical wave approximations are treated in detail. The simple direct methods exploiting low energy backscattering and high energy forward focusing, which can provide information on topmost crystal layers, are discussed. In general, one needs to compare experiment and theory via trial-and-error extensive multiple scattering

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37

Siegel, David A., William C. Chueh, Farid El Gabaly, Kevin F. McCarty, Juan de la Figuera, and María Blanco-Rey. "Determination of the surface structure of CeO2(111) by low-energy electron diffraction." Journal of Chemical Physics 139, no. 11 (2013): 114703. http://dx.doi.org/10.1063/1.4820826.

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38

NISHIMURA, T., K. HATTORI, K. KATAOKA, Y. SHIMAMOTO, and H. DAIMON. "ADSORPTION AND REACTION OF NITRIC OXIDE ON Si(111)-Au SURFACES." Surface Review and Letters 13, no. 02n03 (2006): 191–96. http://dx.doi.org/10.1142/s0218625x06008037.

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We studied adsorption and reaction of nitric oxide on Si (111)7 × 7, 5 × 2- Au , [Formula: see text], [Formula: see text], and 6 × 6- Au surfaces with low-energy electron diffraction, Auger electron spectroscopy, and scanning tunneling microscopy (STM). We found that NO gas reacts most strongly with the 7 × 7 surface, strongly with the 5 × 2- Au surface, and little with the other Si (111)- Au surfaces. STM results indicated that the NO exposure removes adatoms and erodes the row structure on the 5 × 2- Au surface at room temperature.

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39

LIU, Y., J. WANG, M. H. XIE, and H. S. WU. "INCOMMENSURATE METALLIC SURFACTANT LAYER ON TOP OF InN FILM." Surface Review and Letters 13, no. 06 (2006): 815–18. http://dx.doi.org/10.1142/s0218625x06008967.

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The surface structure of InN film heteroepitaxially grown on a GaN buffer layer by MBE is followed by low energy electron diffraction (LEED). The metallic surfactant layers on top of the InN surfaces show an incommensurate structure rather than being disordered. The metal in the incommensurate structure induces additional diffraction spots in the LEED. Based on the Auger experiments, not only In atoms but also Ga are present on the surface of the InN films.

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40

SCHWARZ, M., C. MAYER, P. VON BLANCKENHAGEN, and W. SCHOMMERS. "TEMPERATURE DEPENDENCE OF THE STRUCTURE OF Al(110) AND Au(110) SURFACES." Surface Review and Letters 04, no. 06 (1997): 1095–101. http://dx.doi.org/10.1142/s0218625x9700136x.

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By temperature-dependent low energy electron diffraction experiments at the Al(110) and the Au(110) surface the roughening transition temperature and the characteristic temperature for the onset of surface melting were determined.

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41

Lindsay, R., S. Tomić, A. Wander, M. García-Méndez, and G. Thornton. "Low Energy Electron Diffraction Study of TiO2(110)(2 × 1)-[HCOO]−." Journal of Physical Chemistry C 112, no. 36 (2008): 14154–57. http://dx.doi.org/10.1021/jp804016d.

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42

Cho, Eun-Sang, Jung-Woon Park, Hoon Hur, et al. "Structure of the Sb/Si(112) Surface Studied by Low Energy Electron Diffraction." Japanese Journal of Applied Physics 43, no. 4A (2004): 1312–14. http://dx.doi.org/10.1143/jjap.43.1312.

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43

ABE, Yukiko, Sin-ichi IGARASHI, Yasuo IRIE, Takato HIRAYAMA, and Ichiro ARAKAWA. "Observation by Extremely-low-current Low Energy Electron Diffraction of the Physisorbed Rare Gas Layer Growth." SHINKU 41, no. 4 (1998): 452–57. http://dx.doi.org/10.3131/jvsj.41.452.

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44

Lopes, E. L., G. J. P. Abreu, R. Paniago, E. A. Soares, V. E. de Carvalho, and H. D. Pfannes. "Atomic geometry determination of FeO(001) grown on Ag(001) by low energy electron diffraction." Surface Science 601, no. 5 (2007): 1239–45. http://dx.doi.org/10.1016/j.susc.2006.12.031.

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45

Starke, U., J. Schardt, W. Weiß, G. Rangelov, Th Fauster, and K. Heinz. "Structure of Epitaxial CoSi2 Films on Si(111) Studied with Low-Energy Electron Diffraction (LEED)." Surface Review and Letters 05, no. 01 (1998): 139–44. http://dx.doi.org/10.1142/s0218625x9800027x.

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Expitaxial films of CoSi 2 on Si(111) were investigated by low-energy electron diffraction. Films of approximately 12 Å thickness were prepared by simultaneous deposition of Co and Si and subsequent annealing. The films were found to crystallize in CaF 2 structure in (111) orientation. Two (1×1) phases of different stoichiometry exist. The surface phase that contains more Co is found to be a CoSi 2(111) bulklike structure terminated by a Si–Co–Si trilayer. The Si-rich phase is terminated by an additional nonrotated silicon bilayer with the lower silicon atoms bound to cobalt in the first CoSi

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46

Gierer, M., H. Bludau, H. Over, and G. Ertl. "The bending mode vibration of CO on Ru(0001) studied with low-energy electron-diffraction." Surface Science 346, no. 1-3 (1996): 64–72. http://dx.doi.org/10.1016/0039-6028(95)00911-6.

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47

Noguchi, Akio, Yu Takamura, Takeshi Nakagawa, Eiji Rokuta, and Seigi Mizuno. "Structural analysis of clean LaB6(100), (111), and (110) surfaces via quantitative low-energy electron diffraction." Surface Science 701 (November 2020): 121686. http://dx.doi.org/10.1016/j.susc.2020.121686.

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48

Baudoing, R., Y. Gauthier, M. Lundberg, and J. Rundgren. "Surface segregation on Pt0.1Ni0.9(111) measured two layers deep by low-energy electron diffraction." Journal of Physics C: Solid State Physics 19, no. 16 (1986): 2825–31. http://dx.doi.org/10.1088/0022-3719/19/16/003.

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49

Zipu, Hu, Li Jia, and Wu Naijuan. "Dynamical low energy electron diffraction analysis for Cs/graphite(0001)-(sqrt3×sqrt3) R30° surface." Chinese Physics Letters 6, no. 1 (1989): 20–23. http://dx.doi.org/10.1088/0256-307x/6/1/006.

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50

HUANG, H., S. Y. TONG, U. MYLER, and K. JACOBI. "ATOMIC STRUCTURE OF Si(113) 3×1-H BY DYNAMICAL LOW-ENERGY ELECTRON DIFFRACTION INTENSITY SPECTRA ANALYSIS." Surface Review and Letters 01, no. 02n03 (1994): 221–27. http://dx.doi.org/10.1142/s0218625x94000229.

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The Si ((113) 3×1-H structure has been investigated by a quantitative low-energy electron diffraction intensity analysis. A model with two Si dimers in the unit cell gives best agreement between the calculation and the experimental data. Three-dimensional atomic coordinates have been determined.

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