SEMICONDUCTOR PHYSICS

First-principle study on energy gap of CNT superlattice structure

Zhonghua Yang1, 2, Guili Liu1, Yingdong Qu2 and Rongde Li2

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Abstract: By using the CASTEP modules based on density functional theory, the electronic structures of B/N pair co-doping (5, 5) CNT rings superlattice have been investigated.The calculation results show that the formation energies of B/N pair co-doping CNT rings are negative, indicating that the new type construction will probably be stable.The band structure and state density of the new type construction show that the energy gap is opened by B/N co-doping in (5, 5) metallic CNT and the metallic CNT is changed into a semiconductor.The energy gap of pure CNT is strongly sensitive to the changes of CNT diameter but the energy gap of B/N co-doping CNT rings remains stable when the diameters are in a reasonable scope, which means that the requirements for the production of CNT have been reduced.The compressive deformation effects mean that the energy gaps are narrowed, which is equivalent to enhancing the doping volume concentration.However, the changes of the energy gap under the tensile deformation effect are opposite.Achieving control of the electrical conductivity of CNT has an important significance for electron devices.

Key words: carbon nanotubedopingdensity functional theoryelectrical conductivity



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Fig. 1.  The supercell structure of a pure CNT.rs

Fig. 2.  (Color online) The structure of a B/N pair co-doping CNT ring.

Fig. 3.  Energy gap structure and state density. (a) Pure CNT. (b) B/N co-doping CNT superlattice structure.

Fig. 4.  Partial density of states (PDOS) of the pure (5,5) CNT.

Fig. 5.  Partial density of states (PDOS) of the CNT superlattice structure.

Fig. 6.  (Color online) The imposed deformation.

Fig. 7.  The curve of the relation between deformation and energy gap width.

Fig. 8.  The curve of the relation between deformation and state density.

Table 1.   Relation between tube radius and energy gap width.

C-C bond length({\AA})1.381.391.401.411.42
Radius ({\AA})6.596.646.686.736.78
Energy gap of pure CNT (eV)0.2220.1380.0490.0410.023
Energy gap of doping CNT (eV)1.6781.8081.9292.0492.030
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Table 2.   Energy gap widths of different superlattice structures.

Structure typeType 1 $\times $ 1Type 3 $\times $ 1Type 5 $\times $ 1Type 7 $\times $ 1Type 9 $\times $ 1
$E_{\rm g}$ (eV)2.0301.0620.4940.3900.2870.023
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    Received: 02 April 2015 Revised: Online: Published: 01 October 2015

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      Zhonghua Yang, Guili Liu, Yingdong Qu, Rongde Li. First-principle study on energy gap of CNT superlattice structure[J]. Journal of Semiconductors, 2015, 36(10): 102002. doi: 10.1088/1674-4926/36/10/102002 Z H Yang, G L Liu, Y D Qu, R D Li. First-principle study on energy gap of CNT superlattice structure[J]. J. Semicond., 2015, 36(10): 102002. doi: 10.1088/1674-4926/36/10/102002.Export: BibTex EndNote
      Citation:
      Zhonghua Yang, Guili Liu, Yingdong Qu, Rongde Li. First-principle study on energy gap of CNT superlattice structure[J]. Journal of Semiconductors, 2015, 36(10): 102002. doi: 10.1088/1674-4926/36/10/102002

      Z H Yang, G L Liu, Y D Qu, R D Li. First-principle study on energy gap of CNT superlattice structure[J]. J. Semicond., 2015, 36(10): 102002. doi: 10.1088/1674-4926/36/10/102002.
      Export: BibTex EndNote

      First-principle study on energy gap of CNT superlattice structure

      doi: 10.1088/1674-4926/36/10/102002
      Funds:

      Project supported by the National Natural Science Foundation of China (Nos.51274142, 50671069).

      • Received Date: 2015-04-02
      • Accepted Date: 2015-05-27
      • Published Date: 2015-01-25

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