2019
DOI: 10.1149/09202.0087ecst
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(Invited) Molecular Dynamics Analysis on the Behavior of Water and Alcohol Liquids on a OH-Terminated SiO2 Surface

Abstract: In this study, we carried molecular dynamics (MD) simulations of water and various alcohol liquids on a flat SiO2 surface terminated by hydroxyl groups in order to examine the microscopic structures of these liquids near the solid surface and diffusion property for the fundamental understanding of the wet process during the semiconductor fabrication. As an equilibrium state, water as well as methanol, ethanol and isopropyl alcohol (IPA) molecules formed a multiple layered structure on the solid surface; howeve… Show more

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Cited by 4 publications
(6 citation statements)
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“…1b. For both pure water and pure IPA liquid, the density distribution of liquid molecules aligns with the earlier report by Yamaguchi et al 23 Water displays a damped oscillation pattern, whereas IPA demonstrates a pattern of a first peak, a void layer with zero density, followed by a second peak.…”
Section: Methodssupporting
confidence: 89%
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“…1b. For both pure water and pure IPA liquid, the density distribution of liquid molecules aligns with the earlier report by Yamaguchi et al 23 Water displays a damped oscillation pattern, whereas IPA demonstrates a pattern of a first peak, a void layer with zero density, followed by a second peak.…”
Section: Methodssupporting
confidence: 89%
“…Similar adsorption behavior of IPA has also been reported for the c-SiO 2 (1 1 1) surface terminated by hydroxyl groups. 23 Based on these RDF plots, we considered a liquid molecule to be adsorbed on the silanol group by forming a hydrogen bond if the distance between the H atom of the silanol group and the O atom of the OH group of the liquid molecule was within 2.20 β„«. Next, to investigate the relative preference of adsorption on the silanol groups between water and IPA molecules, we analyzed the MD trajectories at several mixing ratios.…”
Section: Resultsmentioning
confidence: 99%
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“…Then the free energy Δ𝐺 needed to induce the change from πœ† = 0 to πœ† = 1 is equal to π‘Š 𝐴 plus the work needed to lift the top piston. Thus, π‘Š is given by π‘Š = Δ𝐺 𝐴 βˆ’ 𝑝Δ𝑧 [15] using Δ𝐺 calculated by the TI, pressure 𝑝 and the displacement of the top piston Δ𝑧 ≑ 𝑧 | βˆ’ 𝑧 | . By using 𝛾 easily calculated in a liquid-vapor coexistence system via Eq.…”
Section: Thermodynamic Routementioning
confidence: 99%
“…[4] mentioned above as well, the relative SL interfacial tension 𝛾 βˆ’ 𝛾 is obtained from Eqs. [13][14][15].…”
Section: Thermodynamic Routementioning
confidence: 99%