title: ÐÐ¾Ð´ÐµÐ»Ð¸ÑÐ¾Ð²Ð°Ð½Ð¸Ðµ Ð²Ð·Ð°Ð¸Ð¼Ð¾Ð´ÐµÐ¹ÑÑÐ²Ð¸Ñ Ð¸ Ð¾ÑÐ°Ð¶Ð´ÐµÐ½Ð¸Ñ ÑÑÐ»Ð»ÐµÑÐµÐ½Ð° Ð½Ð° Ð¿Ð¾Ð²ÐµÑÑ Ð½Ð¾ÑÑÑ ÑÐ¸ÑÐ°Ð½Ð°
title: Ð²ÑÐ¿ÑÑÐºÐ½Ð°Ñ ÐºÐ²Ð°Ð»Ð¸ÑÐ¸ÐºÐ°ÑÐ¸Ð¾Ð½Ð½Ð°Ñ ÑÐ°Ð±Ð¾ÑÐ° Ð±Ð°ÐºÐ°Ð»Ð°Ð²ÑÐ°
titleType: Subtitle
title: Modeling of the interaction and deposition of fullerene on the surface of titanium
Creators: name: Ð¡Ð°ÑÐ¾Ð½Ð¾Ð², ÐÐ»ÑÑ
Publisher: name: Ð¡Ð°Ð½ÐºÑ-ÐÐµÑÐµÑÐ±ÑÑÐ³ÑÐºÐ¸Ð¹ Ð¿Ð¾Ð»Ð¸ÑÐµÑÐ½Ð¸ÑÐµÑÐºÐ¸Ð¹ ÑÐ½Ð¸Ð²ÐµÑÑÐ¸ÑÐµÑ ÐÐµÑÑÐ° ÐÐµÐ»Ð¸ÐºÐ¾Ð³Ð¾
Year: 2019
Subjects: Ð¼Ð¾Ð»ÐµÐºÑÐ»ÑÑÐ½Ð°Ñ Ð´Ð¸Ð½Ð°Ð¼Ð¸ÐºÐ°
ÑÑÐ»Ð»ÐµÑÐµÐ½
ÑÐ¸ÑÐ°Ð½
ÑÐ¸ÑÐ»ÐµÐ½Ð½Ð¾Ðµ Ð¼Ð¾Ð´ÐµÐ»Ð¸ÑÐ¾Ð²Ð°Ð½Ð¸Ðµ
molecular dynamics
fullerene
titanium
numerical simulation

description: Ð Ð°Ð±Ð¾ÑÐ° Ð·Ð°ÐºÐ»ÑÑÐ°Ð»Ð°ÑÑ Ð² ÑÐ¾Ð·Ð´Ð°Ð½Ð¸Ð¸ Ð¸ Ð¸ÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ð¸ Ð¼Ð¾Ð´ÐµÐ»Ð¸ Ð¿Ð°Ð´ÐµÐ½Ð¸Ñ Ð¼Ð¾Ð»ÐµÐºÑÐ»Ñ ÑÑÐ»Ð»ÐµÑÐµÐ½Ð° Ð½Ð° Ð¿Ð¾Ð²ÐµÑÑÐ½Ð¾ÑÑÑ ÐºÑÐ¸ÑÑÐ°Ð»Ð»Ð¸ÑÐµÑÐºÐ¾Ð³Ð¾ ÑÐ¸ÑÐ°Ð½Ð° Î±-Ð¼Ð¾Ð´Ð¸ÑÐ¸ÐºÐ°ÑÐ¸Ð¸, Ð½Ð°Ð³ÑÐµÑÐ¾Ð³Ð¾ Ð´Ð¾ ÐºÐ¾Ð¼Ð½Ð°ÑÐ½Ð¾Ð¹ ÑÐµÐ¼Ð¿ÐµÑÐ°ÑÑÑÑ. Ð¡Ð¸ÑÑÐµÐ¼Ð° Ð±ÑÐ»Ð° Ð¿ÑÐ¾Ð¼Ð¾Ð´ÐµÐ»Ð¸ÑÐ¾Ð²Ð°Ð½Ð° Ð¿ÑÐ¸ ÑÐ°Ð·Ð»Ð¸ÑÐ½ÑÑ Ð·Ð½Ð°ÑÐµÐ½Ð¸ÑÑ Ð½Ð°ÑÐ°Ð»ÑÐ½Ð¾Ð¹ ÑÐ½ÐµÑÐ³Ð¸Ð¸ Ð´Ð²Ð¸Ð¶ÐµÐ½Ð¸Ñ ÑÐµÐ½ÑÑÐ° Ð¼Ð°ÑÑ ÑÑÐ»Ð»ÐµÑÐµÐ½Ð°. ÐÑÐ»Ð¾ Ð²ÑÐ´ÐµÐ»ÐµÐ½Ð¾ ÑÑÐ¸ ÑÐ°Ð·Ð»Ð¸ÑÐ½ÑÑ ÑÐ¸Ð¿Ð° Ð¿Ð¾Ð²ÐµÐ´ÐµÐ½Ð¸Ñ ÑÑÐ¾Ð¹ ÑÐ¸ÑÑÐµÐ¼Ñ Ð² Ð·Ð°Ð²Ð¸ÑÐ¸Ð¼Ð¾ÑÑÐ¸ Ð¾Ñ Ð½Ð°ÑÐ°Ð»ÑÐ½Ð¾Ð¹ ÑÐ½ÐµÑÐ³Ð¸Ð¸ Ð´Ð²Ð¸Ð¶ÐµÐ½Ð¸Ñ ÑÑÐ»Ð»ÐµÑÐµÐ½Ð°. ÐÐ¾ 1000 eV ÐºÐ»Ð°ÑÑÐµÑ Ð¡60 Ð¾ÑÐ°Ð¶Ð´Ð°Ð»ÑÑ Ð½Ð° Ð¿Ð¾Ð²ÐµÑÑÐ½Ð¾ÑÑÑ ÑÐ¸ÑÐ°Ð½Ð°, Ð½Ðµ Ð¿ÑÐ¸Ð²Ð¾Ð´Ñ Ð½Ð¸ Ðº ÐºÐ°ÐºÐ¸Ð¼ Ð½ÐµÑÐ¿ÑÑÐ³Ð¸Ð¼ Ð¿ÑÐ¾ÑÐµÑÑÐ°Ð¼. Ð Ð¸Ð½ÑÐµÑÐ²Ð°Ð»Ðµ ÑÐ½ÐµÑÐ³Ð¸Ð¹ Ð¾Ñ 1000 eV Ð´Ð¾ 22000 eV ÑÑÐ»Ð»ÐµÑÐµÐ½, ÐºÐ°Ðº ÑÐµÐ»Ð¾Ðµ Ð¸ Ð½Ðµ Ð¸ÑÐ¿ÑÑÑÐ²Ð°Ñ ÑÐ°Ð·ÑÑÑÐµÐ½Ð¸Ñ ÑÐ¾Ð±ÑÑÐ²ÐµÐ½Ð½Ð¾Ð¹ ÑÑÑÑÐºÑÑÑÑ, Ð¿ÑÐ¾Ð½Ð¸ÐºÐ°ÐµÑ Ð² ÑÐµÑÐµÑÐºÑ ÑÐ¸ÑÐ°Ð½Ð°. ÐÑÐ¸ ÑÐ½ÐµÑÐ³Ð¸ÑÑ Ð±Ð¾Ð»ÑÑÐ¸Ñ, ÑÐµÐ¼ 22000 eV ÑÐ³Ð»ÐµÑÐ¾Ð´Ð½ÑÑ ÐºÐ»Ð°ÑÑÐµÑ Ð½Ð°ÑÐ¸Ð½Ð°ÐµÑ ÑÐ°Ð·ÑÑÑÐ°ÑÑÑÑ Ð¸ Ð¿ÑÐ¾Ð½Ð¸ÐºÐ°ÑÑ Ð² ÑÐµÑÐµÑÐºÑ ÑÐ¸ÑÐ°Ð½Ð° ÑÐ¶Ðµ Ð² ÐºÐ°ÑÐµÑÑÐ²Ðµ Ð¾ÑÐ´ÐµÐ»ÑÐ½ÑÑ Ð°ÑÐ¾Ð¼Ð¾Ð² ÑÐ³Ð»ÐµÑÐ¾Ð´Ð°. ÐÑÐ»Ð° Ð¿Ð¾Ð»ÑÑÐµÐ½Ð° Ð¼Ð°ÐºÑÐ¸Ð¼Ð°Ð»ÑÐ½Ð°Ñ Ð³Ð»ÑÐ±Ð¸Ð½Ð° Ð¿ÑÐ¾Ð½Ð¸ÐºÐ½Ð¾Ð²ÐµÐ½Ð¸Ñ Ð¼Ð¾Ð»ÐµÐºÑÐ»Ñ ÑÑÐ»Ð»ÐµÑÐµÐ½Ð° Ð² ÑÐµÑÐµÑÐºÑ ÑÐ¸ÑÐ°Ð½Ð°. ÐÐ½Ð° Ð¾ÐºÐ°Ð·Ð°Ð»Ð°ÑÑ ÑÐ°Ð²Ð½Ð¾Ð¹ 4.5 Ð½Ð¼.
description: Work on the creation and study of models of changes in the density of Î±-modifications, heated to room temperature. The lattice of titanium and the fullerene molecule were modeled. This is due to the addition of periodic conditions at the boundary of the simulation. The system was modeled at different values of the initial energy of motion of the central mass of fullerene. 
Three different types of behavior of this system were identified, depending on the initial energy of motion of the fullerene. Up to 1000 eV, the C60 cluster was deposited on the surface of titanium, resulting in no inelastic process. In the energy range from 1000 to 22000 eV, the fullerene, as a whole, and did not experience the destruction of its own structure, penetrates into the titanium lattice. At energies greater than 22000 eV, the carbon cluster begins to break down and penetrate into the titanium lattice. The maximum depth of penetration of the fullerene molecule into the titanium lattice was obtained. It was equal to 4.5 nm.