全部 标题 作者
关键词 摘要

OALib Journal期刊
ISSN: 2333-9721
费用:99美元

查看量下载量

相关文章

更多...

Atomistic Frictional Properties of the C(100)2x1-H Surface

DOI: 10.1155/2013/850473

Full-Text   Cite this paper   Add to My Lib

Abstract:

Density functional theory- (DFT-) based ab initio calculations were used to investigate the surface-to-surface interaction and frictional behavior of two hydrogenated C(100) dimer surfaces. A monolayer of hydrogen atoms was applied to the fully relaxed C(100)2x1 surface having rows of C=C dimers with a bond length of 1.39??. The obtained C(100)2x1-H surfaces (C–H bond length 1.15??) were placed in a large vacuum space and translated toward each other. A cohesive state at a surface separation of 4.32?? that is stabilized by approximately 0.42?eV was observed. An increase in the charge separation in the surface dimer was calculated at this separation having a 0.04?e transfer from the hydrogen atom to the carbon atom. The Mayer bond orders were calculated for the C–C and C–H bonds and were found to be 0.962 and 0.947, respectively. σ C–H bonds did not change substantially from the fully separated state. A significant decrease in the electron density difference between the hydrogen atoms on opposite surfaces was seen and assigned to the effects of Pauli repulsion. The surfaces were translated relative to each other in the (100) plane, and the friction force was obtained as a function of slab spacing, which yielded a 0.157 coefficient of friction. 1. Introduction Carbon-based surface films are now ubiquitous as frictional barriers that lower the wear rates of interacting bodies. They have found extensive use within the information storage industry as films for protecting both the hard disk surface and the sensitive read-write transducers from damage due friction during incremental and in some instances purposeful head-to-disk contact [1, 2]. Because of this industrial importance, a rich and extensive literature exists of both theoretical and experimental studies probing the fundamental properties of these complicated and diverse surface films [3, 4]. Within the range of these studies single crystal diamond surfaces have been extensively employed as models of the more important larger-scale industrial surfaces. Insight gained from these studies has helped the community understand surface energetic processes, including the recent manifestation of super lubricity of hydrogen-covered surfaces [5, 6]. Carbon films deposited under energetic conditions assume complicated amorphous structures, which depend on the exact conditions of deposition. Specifically, the extent of surface wear protection has been attributed to film properties that can be tailored through the manipulation of deposition parameters, precursor materials, and postdeposition processing, the

References

[1]  A. Anders, W. Fong, A. V. Kulkarni, F. W. Ryan, and C. S. Bhatia, “Ultrathin diamond-like carbon films deposited by filtered carbon vacuum arcs,” IEEE Transactions on Plasma Science, vol. 29, no. 5 I, pp. 768–775, 2001.
[2]  C. M. Mate, “Nanotribology studies of carbon surfaces by force microscopy,” Wear, vol. 168, no. 1-2, pp. 17–20, 1993.
[3]  J. Robertson, “Diamond-like amorphous carbon,” Materials Science and Engineering (R), vol. 37, no. 4–6, pp. 129–281, 2002.
[4]  D. R. McKenzie, “Tetrahedral bonding in amorphous carbon,” Reports on Progress in Physics, vol. 59, no. 12, pp. 1611–1664, 1996.
[5]  A. Erdemir, “Superlubricity and wearless sliding in diamondlike carbon films,” in Surface Engineering 2001—Fundamentals and Applications, vol. 697 of MRS Proceedings, pp. 391–403, November 2001.
[6]  S. Dag and S. Ciraci, “Atomic scale study of superlow friction between hydrogenated diamond surfaces,” Physical Review B, vol. 70, no. 24, Article ID 241401(R), 4 pages, 2004.
[7]  F. Demichelis, C. F. Pirri, A. Tagliaferro et al., “Mechanical and thermophysical properties of diamond-like carbon (DLC) films with different sp3/sp2 ratios,” Diamond and Related Materials, vol. 2, no. 5–7, pp. 890–892, 1993.
[8]  J. T. Titantah, D. Lamoen, E. Neyts, and A. Bogaerts, “The effect of hydrogen on the electronic and bonding properties of amorphous carbon,” Journal of Physics Condensed Matter, vol. 18, no. 48, pp. 10803–10815, 2006.
[9]  L. Diederich, P. Aebi, O. M. Küttel, and L. Schlapbach, “NEA peak of the differently terminated and oriented diamond surfaces,” Surface Science, vol. 424, no. 2, pp. L314–L320, 1999.
[10]  J. van der Weide, Z. Zhang, P. K. Baumann, M. G. Wensell, J. Bernholc, and R. J. Nemanich, “Negative-electron-affinity effects on the diamond (100) surface,” Physical Review B, vol. 50, no. 8, pp. 5803–5806, 1994.
[11]  H. Kawarada, “Hydrogen-terminated diamond surfaces and interfaces,” Surface Science Reports, vol. 26, no. 7, pp. 205–259, 1996.
[12]  S. J. Sque, R. Jones, and P. R. Briddon, “Structure, electronics, and interaction of hydrogen and oxygen on diamond surfaces,” Physical Review B, vol. 73, no. 8, Article ID 085313, 15 pages, 2006.
[13]  J. Furthmüller, J. Hafner, and G. Kresse, “Dimer reconstruction and electronic surface states on clean and hydrogenated diamond (100) surfaces,” Physical Review B, vol. 53, no. 11, pp. 7334–7351, 1996.
[14]  G. Zilibotti, M. Ferrario, C. M. Bertoni, and M. C. Righi, “Ab initio calculation of adhesion and potential corrugation of diamond (001) interfaces,” Computer Physics Communications, vol. 182, no. 9, pp. 1796–1799, 2011.
[15]  K. Hayashi, K. Tezuka, N. Ozawa, T. Shimazaki, K. Adachi, and M. Kubo, “Tribochemical reaction dynamics simulation of hydrogen on a diamond-like carbon surface based on tight-binding quantum chemical molecular dynamics,” Journal of Physical Chemistry C, vol. 115, no. 46, pp. 22981–22986, 2011.
[16]  O. L. Eryilmaz and A. Erdemir, “On the hydrogen lubrication mechanism(s) of DLC films: an imaging TOF-SIMS study,” Surface and Coatings Technology, vol. 203, no. 5–7, pp. 750–755, 2008.
[17]  F. G. Sen, Y. Qi, and A. T. Alpas, “Surface stability and electronic structure of hydrogen-and fluorine-terminated diamond surfaces: a first principles investigation,” Journal of Materials Research, vol. 24, no. 8, pp. 2461–2470, 2009.
[18]  J. A. Johnson, J. B. Woodford, X. Chen, J. Andersson, A. Erdemir, and G. R. Fenske, “Insights into near-frictionless carbon films,” Journal of Applied Physics, vol. 95, no. 12, pp. 7765–7771, 2004.
[19]  A. Erdemir, “Developing a near-frictionless carbon coating,” Tribology and Lubrication Technology, vol. 61, no. 10, pp. 12–14, 2005.
[20]  J. A. Harrison, C. T. White, R. J. Colton, and D. W. Brenner, “Molecular-dynamics simulations of atomic-scale friction of diamond surfaces,” Physical Review B, vol. 46, no. 15, pp. 9700–9708, 1992.
[21]  M. Garvey, M. Weinert, and W. T. Tysoe, “On the pressure dependence of shear strengths in sliding, boundary-layer friction,” Tribology Letters, vol. 44, no. 1, pp. 67–73, 2011.
[22]  G. Zilibotti and M. C. Righi, “Ab initio calculation of the adhesion and ideal shear strength of planar diamond interfaces with different atomic structure and hydrogen coverage,” Langmuir, vol. 27, no. 11, pp. 6862–6867, 2011.
[23]  G. Gao, R. J. Cannara, R. W. Carpick, and J. A. Harrison, “Atomic-scale friction on diamond: a comparison of different sliding directions on (001) and (111) surfaces using MD and AFM,” Langmuir, vol. 23, no. 10, pp. 5394–5405, 2007.
[24]  G. T. Wang, S. F. Bent, J. N. Russell Jr., J. E. Butler, and M. P. D'Evelyn, “Functionalization of diamon (100) by diels-alder chemistry,” Journal of the American Chemical Society, vol. 122, no. 4, pp. 744–745, 2000.
[25]  T. Halicioglu, “Calculation of surface energies for low index planes of diamond,” Surface Science, vol. 259, no. 1-2, pp. L714–L718, 1991.
[26]  R. H. Telling, C. J. Pickard, M. C. Payne, and J. E. Field, “Theoretical strength and cleavage of diamond,” Physical Review Letters, vol. 84, no. 22, pp. 5160–5163, 2000.
[27]  B. Delley, “An all-electron numerical method for solving the local density functional for polyatomic molecules,” The Journal of Chemical Physics, vol. 92, no. 1, pp. 508–517, 1990.
[28]  B. Delley, “A standard tool for density functional calculations: review and advances,” in Modern Density Functional Theory: A Tool for Chemistry, J. M. Seminario and P. Politzer, Eds., vol. 2 of Theoretical and Computational Chemistry, Elsevier Science B, Amsterdam, The Netherlands, 1995.
[29]  J. P. Perdew and Y. Wang, “Accurate and simple analytic representation of the electron-gas correlation energy,” Physical Review B, vol. 45, no. 23, pp. 13244–13249, 1992.
[30]  D. Henwood and J. D. Carey, “Ab initio investigation of molecular hydrogen physisorption on graphene and carbon nanotubes,” Physical Review B, vol. 75, no. 24, Article ID 245413, 10 pages, 2007.
[31]  S. K. Nayak, B. K. Rao, and P. Jena, “Equilibrium geometries, electronic structure and magnetic properties of small manganese clusters,” Journal of Physics Condensed Matter, vol. 10, no. 48, pp. 10863–10877, 1998.
[32]  T. Bu?ko, J. Hafner, S. Lebègue, and J. G. ángyán, “Improved description of the structure of molecular and layered crystals: Ab initio DFT calculations with van der Waals corrections,” Journal of Physical Chemistry A, vol. 114, no. 43, pp. 11814–11824, 2010.
[33]  Y. Liu and W. A. Goddard, “First-principles-based dispersion augmented density functional theory: from molecules to crystals,” Journal of Physical Chemistry Letters, vol. 1, no. 17, pp. 2550–2555, 2010.
[34]  I. Mayer, “Bond orders and valences from ab initio wave functions,” International Journal of Quantum Chemistry, vol. 29, no. 3, pp. 477–483, 1986.
[35]  R. S. Mulliken, “Electronic population analysis on LCAO-MO molecular wave functions. II. Overlap populations, bond orders, and covalent bond energies,” The Journal of Chemical Physics, vol. 23, no. 10, pp. 1841–1846, 1955.
[36]  L. Ostrovskaya, V. Perevertailo, V. Ralchenko, A. Dementjev, and O. Loginova, “Wettability and surface energy of oxidized and hydrogen plasma-treated diamond films,” Diamond and Related Materials, vol. 11, no. 3-6, pp. 845–850, 2002.
[37]  G. Tanasa, Atomic scale friction: a scanning probe study on crystalline surfaces [Ph.D. thesis], Eindhoven University of Technology, 2005.
[38]  P. L. Piotrowski, R. J. Cannara, G. Gao, J. J. Urban, R. W. Carpick, and J. A. Harrison, “Atomistic factors governing adhesion between diamond, amorphous carbon and model diamond nanocomposite surfaces,” Journal of Adhesion Science and Technology, vol. 24, no. 15-16, pp. 2471–2498, 2010.
[39]  R. Neitola and T. A. Pakkanen, “Ab initio studies on the atomic-scale origin of friction between diamond (111) surfaces,” Journal of Physical Chemistry B, vol. 105, no. 7, pp. 1338–1343, 2001.
[40]  M. D. Perry and J. A. Harrison, “Universal aspects of the atomic-scale friction of diamond surfaces,” Journal of Physical Chemistry, vol. 99, no. 24, pp. 9960–9965, 1995.
[41]  W. Zhong and D. Tom?nek, “First-principles theory of atomic-scale friction,” Physical Review Letters, vol. 64, no. 25, pp. 3054–3057, 1990.
[42]  T. A. Albright, J. K. Burdett, and M. H. Whangbo, Orbital Interactions in Chemistry, John Wiley & Sons, New York, 1985.
[43]  T. ?a?in, J. Che, M. N. Gardos, A. Fijany, and W. A. Goddard, “Simulation and experiments on friction and wear of diamond: a material for MEMS and NEMS application,” Nanotechnology, vol. 10, no. 3, pp. 278–284, 1999.
[44]  Y. Mo, K. T. Turner, and I. Szlufarska, “Friction laws at the nanoscale,” Nature, vol. 457, no. 7233, pp. 1116–1119, 2009.
[45]  D. S. Grierson, E. E. Flater, and R. W. Carpick, “Accounting for the JKR-DMT transition in adhesion and friction measurements with atomic force microscopy,” Journal of Adhesion Science and Technology, vol. 19, no. 3–5, pp. 291–311, 2005.
[46]  E. C. Gage, T. W. Mcdaniel, W. A. Challener et al., “Heat assisted magnetic recording,” Proceedings of the IEEE, vol. 96, no. 11, pp. 1810–1835, 2008.
[47]  R. Z. Lei, A. J. Gellman, and P. Jones, “Thermal stability of Fomblin Z and Fomblin Zdol thin films on amorphous hydrogenated carbon,” Tribology Letters, vol. 11, no. 1, pp. 1–5, 2001.

Full-Text

comments powered by Disqus

Contact Us

service@oalib.com

QQ:3279437679

WhatsApp +8615387084133

WeChat 1538708413