Theoretical study of hydrogen atom adsorbed on carbon-doped BN nanotubes

We have investigated the electronic structures of C-doped (9,0) boron nitride nanotubes (BNNTs) and hydrogen-decorated C-doped (9,0) BNNTs using density functional theory (DFT). It is found that the doping effect of C-doped BNNTs can be compensated by adsorption of H atom on the C sites. The adsorption energies for hydrogen atoms on different adsorption sites on BNNTs and C-doped BNNTs are obtained by using ONIOM method. The results indicate that the most favorable configuration of the adsorption structures is a hydrogen atom adsorbed on the C site of C-doped BNNT.

[1]  Parr,et al.  Development of the Colle-Salvetti correlation-energy formula into a functional of the electron density. , 1988, Physical review. B, Condensed matter.

[2]  Keiji Morokuma,et al.  The IMOMO method: Integration of different levels of molecular orbital approximations for geometry optimization of large systems: Test for n‐butane conformation and SN2 reaction: RCl+Cl− , 1996 .

[3]  Magnetism in BN nanotubes induced by carbon doping , 2005, cond-mat/0501104.

[4]  Jinlong Yang,et al.  Deformation-induced site selectivity for hydrogen adsorption on boron nitride nanotubes , 2004 .

[5]  Kleinman,et al.  4f resonances with norm-conserving pseudopotentials. , 1990, Physical review. B, Condensed matter.

[6]  Leonard Kleinman,et al.  Efficacious Form for Model Pseudopotentials , 1982 .

[7]  L. B. Ebert Science of fullerenes and carbon nanotubes , 1996 .

[8]  Feliu Maseras,et al.  IMOMM: A new integrated ab initio + molecular mechanics geometry optimization scheme of equilibrium structures and transition states , 1995, J. Comput. Chem..

[9]  Martins,et al.  Efficient pseudopotentials for plane-wave calculations. , 1991, Physical review. B, Condensed matter.

[10]  Steven G. Louie,et al.  Boron Nitride Nanotubes , 1995, Science.

[11]  A. Becke Density-functional thermochemistry. III. The role of exact exchange , 1993 .

[12]  J. Sudmeier,et al.  Cadmium-113 nuclear magnetic resonance studies of 113Cd(ii)-substituted human carbonic anhydrase B. , 1977, Journal of the American Chemical Society.

[13]  C. Bauschlicher,et al.  High Coverages of Hydrogen on a (10,0) Carbon Nanotube , 2001 .

[14]  Y. Bando,et al.  SINGLE-WALLED B-DOPED CARBON, B/N-DOPED CARBON AND BN NANOTUBES SYNTHESIZED FROM SINGLE-WALLED CARBON NANOTUBES THROUGH A SUBSTITUTION REACTION , 1999 .

[15]  Y. Bando,et al.  A novel precursor for synthesis of pure boron nitride nanotubes. , 2002, Chemical communications.

[16]  A. Zunger,et al.  Self-interaction correction to density-functional approximations for many-electron systems , 1981 .

[17]  Hongwei Zhu,et al.  Hydrogen uptake in boron nitride nanotubes at room temperature. , 2002, Journal of the American Chemical Society.

[18]  Soler,et al.  Self-consistent order-N density-functional calculations for very large systems. , 1996, Physical review. B, Condensed matter.

[19]  H. Monkhorst,et al.  SPECIAL POINTS FOR BRILLOUIN-ZONE INTEGRATIONS , 1976 .

[20]  A. Fazzio,et al.  Theoretical study of native defects in BN nanotubes , 2003 .

[21]  Cohen,et al.  Theory of graphitic boron nitride nanotubes. , 1994, Physical review. B, Condensed matter.

[22]  D. Sánchez-Portal,et al.  The SIESTA method for ab initio order-N materials simulation , 2001, cond-mat/0111138.

[23]  Daniel Sánchez-Portal,et al.  Density‐functional method for very large systems with LCAO basis sets , 1997 .