1994
DOI: 10.1016/0038-1098(94)90337-9
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Ba deposition on Si (1 0 0)2 × 1

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Cited by 33 publications
(21 citation statements)
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“…Submonolayer surface phases of Ba/ Si͑001͒ and Sr/ Si͑001͒ have been studied previously by low-energy electron diffraction ͑LEED͒, [6][7][8][9][10][11][12] Auger electron spectroscopy ͑AES͒, 8,11,12 reflection high energy electron diffraction ͑RHEED͒, 13 scanning tunneling microscopy ͑STM͒, [14][15][16][17][18][19] angle-integrated ultraviolet photoelectron spectroscopy ͑AIUPS͒, 20 ion scattering, 21 x-ray photoemission spectroscopy ͑XPS͒, 22 x-ray standing waves ͑XSW͒, 23,24 and density functional theory ͑DFT͒ calculations. 5,17,[25][26][27] Most of the atomic-scale structural models proposed for the various short and long-range ordered AEM/Si͑001͒ surface structures observed at AEM coverages between 0 and 1 / 2 ML consist of individual AEM adatoms occupying valley-bridge sites on a dimerized Si͑001͒ surface.…”
Section: Introductionmentioning
confidence: 99%
“…Submonolayer surface phases of Ba/ Si͑001͒ and Sr/ Si͑001͒ have been studied previously by low-energy electron diffraction ͑LEED͒, [6][7][8][9][10][11][12] Auger electron spectroscopy ͑AES͒, 8,11,12 reflection high energy electron diffraction ͑RHEED͒, 13 scanning tunneling microscopy ͑STM͒, [14][15][16][17][18][19] angle-integrated ultraviolet photoelectron spectroscopy ͑AIUPS͒, 20 ion scattering, 21 x-ray photoemission spectroscopy ͑XPS͒, 22 x-ray standing waves ͑XSW͒, 23,24 and density functional theory ͑DFT͒ calculations. 5,17,[25][26][27] Most of the atomic-scale structural models proposed for the various short and long-range ordered AEM/Si͑001͒ surface structures observed at AEM coverages between 0 and 1 / 2 ML consist of individual AEM adatoms occupying valley-bridge sites on a dimerized Si͑001͒ surface.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast, little attention has been paid to the alkaline earth metals such as Ba, although the element in many aspects behaves similarly to the AM. 7 According to the limited reports obtained from various techniques such as x-ray photoelectron spectroscopy ͑XPS͒, 8,9 Auger electron spectroscopy ͑AES͒, 10,11 low-energy electron diffraction ͑LEED͒, [10][11][12] thermal desorption spectroscopy ͑TDS͒, 10,11,13 and metastable-atom deexcitation spectroscopy ͑MDS͒, 10,13 the behaviors of the Ba/Si(001)2ϫ1 interface can be summarized as ͑i͒ Ba grown layer by layer, ͑ii͒ ionic interaction between the first Ba overlayer and the silicon surface, leading a charge transfer from the former to the latter, ͑iii͒ the second overlayer and above having a metallic character, and ͑iv͒ no silicide formation at room temperature. The present high-resolution synchrotron radiation photoemission work on a clean Ba/Si(001)2ϫ1 interface found actually that ionic interaction does not occur, and the Ba silicides can be formed at room temperature, as long as the substrate surface is atomically clean.…”
mentioning
confidence: 99%
“…Thus, the previous conclusion of an ionic interaction due to the charge transfer is denied. 10,11,13 Instead, the polarized model is more appropriate for the Ba/Si system. 24 The present finding of Ba-silicides formation at room temperature is in great contrast to all the previous reports, which had them shown only in an annealed film.…”
mentioning
confidence: 99%
“…4,5,9,[11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27] The key question regarding these phases is whether they are simple alkaline-earth adatom structures or more complex surface alloys. Adatom models 8,28 fail to reproduce STM images of the (3×2) phase, 17,25,27 while alloy models 9,10,25 require significant Si dimer movement to occur at temperatures well below those typically required for mass transport on Si surfaces.…”
Section: Introductionmentioning
confidence: 99%