• Title/Summary/Keyword: buckled Si dimer

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The buckled structure of clean Si(001) surface : $a(2\times1)과\; c(4\times2)$ (깨끗한 Si(001) 표면의 buckled dimer 구조 연구 : $a(2\times1)과\; c(4\times2)$)

  • 김성수;김용욱;박노길;조원석;조원석;김주영;채근화;황정남;김기석
    • Journal of the Korean Vacuum Society
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    • v.7 no.1
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    • pp.5-10
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    • 1998
  • The geometric structure of dimer atoms on clean Si(001) surface was studied using CAICISS. We confirmed that dimer atoms were certainly buckled, and also found that asymmetry (2$\times$1) and c(4$\times$2) were coexisted. The intradimer bond length and the buckling angle of a dimer measured by CAICISS system were 2.3$\pm$0.1 $\AA$ and 18$\pm$$1^{\circ}$, respectively.

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Regular Distribution of -OH Fragments on a Si (001)-c(4×2) Surface by Dissociation of Water Molecules (물 분자의 해리에 의한 Si (001)-c(4×2) 표면에서의 수산화기의 균일한 분포)

  • Lee, Soo-Kyung;Oh, Hyun-Chul;Kim, Dae-Hee;Jeong, Yong-Chan;Baek, Seung-Bin;Kim, Yeong-Cheol
    • Korean Journal of Materials Research
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    • v.20 no.9
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    • pp.457-462
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    • 2010
  • Adsorption of a water molecule on a Si (001) surface and its dissociation were studied using density functional theory to study the distribution of -OH fragments on the Si surface. The Si (001) surface was composed of Si dimers, which buckle in a zigzag pattern below the order-disorder transition temperature to reduce the surface energy. When a water molecule approached the Si surface, the O atom of the water molecule favored the down-buckled Si atom, and the H atom of the water molecule favored the up-buckled Si atom. This is explained by the attractions between the negatively charged O of the water and the positively charged down-buckled Si atom and between the positively charged H of the water and the negatively charged up-buckled Si atom. Following the adsorption of the first water molecule on the surface, a second water molecule adsorbed on either the inter-dimer or intra-dimer site of the Si dimer. The dipole-dipole interaction of the two adsorbed water molecules led to the formation of the water dimer, and the dissociation of the water molecules occurred easily below the order-disorder transition temperature. Therefore, the 1/2 monolayer of -OH on the water-terminated Si (001) surface shows a regular distribution. The results shed light on the atomic layer deposition process of alternate gate dielectric materials, such as $HfO_2$.

The Effect of H₂O Chemisorption on the Reconstruction of the Si(100) Surface : a Theoretical Approach

  • 양성은;김호징
    • Bulletin of the Korean Chemical Society
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    • v.16 no.11
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    • pp.1028-1032
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    • 1995
  • The structure and electronic properties of the Si(100) surface is studied using the atom superposition and electron delocalization method. The energy released when the symmetric dimer surface is reconstructed to form the buckled dimer surface with p(2X2) symmetry is calculated to be 0.99 eV per dimer in the case of ideal clean surfaces. This indicates that the surface dimer buckling is intrinsic from the viewpoint of thermodynamics. The relaxation energy, when water is adsorbed on the clean symmetric dimer surface to form the buckled dimer surface, is 2.25 eV per dimer for appropriate coverages. These results show that H2O molecule could induce a reconstruction of the surface structure through adsorption. The buckling of the surface dimer is, therefore, more favorable under the existence of water vapour. This conclusion supports the recently obtained experimental observations by Chander et al.

Indium Nanowire Growth on Si (001) Surface Using Density Functional Theory (Density Functional Theory를 이용한 Si (001) 표면 위의 In 나노선 성장 연구)

  • Kim, Dae-Hyun;Kim, Dae-Hee;Seo, Hwa-Il;Kim, Yeong-Cheol
    • Korean Journal of Materials Research
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    • v.19 no.3
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    • pp.137-141
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    • 2009
  • Density functional theory was utilized to investigate the growth of an indium nanowire on a Si (001) buckled surface. A site between the edge of two Si dimers is most favorable when the first In atom is adsorbed on the surface at an adsorption energy level of 2.26 eV. The energy barriers for migration from other sites to the most favorable site are low. When the second In atom is adsorbed next to the first In atom to form an In dimer perpendicular to the Si dimer row, the adsorption energy is the highest among all adsorption sites. The third In atom prefers either of the sites next to the In dimer along the In dimer direction. The fourth In atom exhibited the same tendency showed by the second atom. The second and fourth In adsorption energy levels are higher than the first and third levels as the In atoms consume the third valence electron by forming In dimers. Therefore, the In nanowire grows perpendicular to the Si dimer row on the Si (001) surface, as it satisfies the bonding of the three valence electrons of the In atoms.