High-temperature scanning tunneling microscopy (STM) observation of metastable structures on quenched Si(111) surfaces

High temperature scanning tunneling microscopy (STM) observation has been performed to investigate the energetic stability of metastable structures of Si(111) surfaces. Upon supercooling from 1100°C, 5×5 and 9×9 structures have been observed at 600°C, as well as the reconstructed 7×7 and disordered...

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Veröffentlicht in:Japanese Journal of Applied Physics 1995-06, Vol.34 (6B), p.3346-3350
Hauptverfasser: HOSHINO, T, KOKUBUN, K, KUMAMOTO, K, ISHIMARU, T, OHDOMARI, I
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container_issue 6B
container_start_page 3346
container_title Japanese Journal of Applied Physics
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creator HOSHINO, T
KOKUBUN, K
KUMAMOTO, K
ISHIMARU, T
OHDOMARI, I
description High temperature scanning tunneling microscopy (STM) observation has been performed to investigate the energetic stability of metastable structures of Si(111) surfaces. Upon supercooling from 1100°C, 5×5 and 9×9 structures have been observed at 600°C, as well as the reconstructed 7×7 and disordered 1×1 areas. The 5×5 and 9×9 areas shrink to disappear as a consequence of the growth of 7×7 domains. The smaller domain size and the faster shrinking speed of the 9×9 structure indicate its lower stability compared to the 5×5 structure. The 11×11 and 13×13 DAS structures were occasionally observed at above 500°C, however, suggesting lower stability than the (2 n +1)×(2 n +1) DAS structures with smaller n . The √3×√3 structures also appear at high-temperatures below 550°C, whereas the 2×2, c 2×4, and c 2×8 structures are observed only at room temperatures. Clear STM images of the √3×√3 structure can rarely be obtained at temperatures higher than 600°C, which is considered to be due to the thermally excited random motion of Si adatoms.
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Upon supercooling from 1100°C, 5×5 and 9×9 structures have been observed at 600°C, as well as the reconstructed 7×7 and disordered 1×1 areas. The 5×5 and 9×9 areas shrink to disappear as a consequence of the growth of 7×7 domains. The smaller domain size and the faster shrinking speed of the 9×9 structure indicate its lower stability compared to the 5×5 structure. The 11×11 and 13×13 DAS structures were occasionally observed at above 500°C, however, suggesting lower stability than the (2 n +1)×(2 n +1) DAS structures with smaller n . The √3×√3 structures also appear at high-temperatures below 550°C, whereas the 2×2, c 2×4, and c 2×8 structures are observed only at room temperatures. Clear STM images of the √3×√3 structure can rarely be obtained at temperatures higher than 600°C, which is considered to be due to the thermally excited random motion of Si adatoms.</abstract><cop>Tokyo</cop><pub>Japanese journal of applied physics</pub><doi>10.1143/jjap.34.3346</doi><tpages>5</tpages></addata></record>
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subjects Condensed matter: structure, mechanical and thermal properties
Electron, ion, and scanning probe microscopy
Exact sciences and technology
Physics
Scanning probe microscopy: scanning tunneling, atomic force, scanning optical, magnetic force, etc
Solid surfaces and solid-solid interfaces
Structure of solids and liquids
crystallography
Surface structure and topography
Surfaces and interfaces
thin films and whiskers (structure and nonelectronic properties)
title High-temperature scanning tunneling microscopy (STM) observation of metastable structures on quenched Si(111) surfaces
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