Interface bands in carbon nanotube superlattices

Physica Status Solidi (C) Current Topics in Solid State Physics

Volumn 7, Issue 2, 2010, Pages 382-385

  Jask Olski W ^a   Pelc, M ^a   Santos, H ^b   Chico, L ^b   Ayuela, A ^c  

^a NICOLAUS COPERNICUS UNIVERSITY   (Poland)

^b INSTITUTO DE CIENCIA DE MATERIALES DE MADRID   (Spain)

^c DONOSTIA INTERNATIONAL PHYSICS CENTER DIPC   (Spain)

Author keywords

[No Author keywords available]

Indexed keywords

BAND STRUCTURE; CARBON NANOTUBES; INTERFACE STATES; METALLIC SUPERLATTICES; NANOSCIENCE; SEMICONDUCTOR JUNCTIONS; YARN;

ANTIBONDING; ELECTRONIC BAND STRUCTURE; FRIEDEL OSCILLATIONS; METALLIC TUBES; ROTATIONAL SYMMETRIES;

SEMICONDUCTOR SUPERLATTICES;

EID: 77954318194     PISSN: 18626351     EISSN: 16101642     Source Type: Journal    
DOI: 10.1002/pssc.200982487     Document Type: Conference Paper

References (15)

1. D. Wei, and Y. Liu, Adv. Mater. 20, 2815 (2008).
2. C. Jin, K. Suenaga, and S. Iijima, Nature Nanotech. 3, 17 (2008).
3. Y. Yao, Q. Li, J. Zhang, R. Liu, L. Jiao, Y. T. Zhu, and Z. Liu, Nature Mater. 6, 283 (2007).
4. A. Rochefort, and Ph. Avouris, Nano Lett. 2, 253 (2002).
5. M. B. Nardelli, Phys. Rev. B 60, 7828 (1999).
6. L. Chico and W. Jaskólski, Phys. Rev. B 69, 085406 (2004).
7. W. Jaskólski and L. Chico, Phys. Rev. B 71, 155405 (2005).
8. A. Ayuela, L. Chico, and W. Jaskólski, Phys. Rev. B 77, 085435 (2008).
9. A. Ayuela, W. Jaskólski, M. Pelc, H. Santos, and L. Chico, Appl. Phys. Lett 93, 1 (2008).
10. H. Santos, A. Ayuela, W. Jaskólski, M. Pelc, and L. Chico, Phys. Rev. B 80, 035436 (2009).
11. M. Fujita, K.Wakabayashi, K. Nakada, and K. Kusakabe, J. Phys. Soc. Jpn. 65, 1920 (1996);
12. K.Wakabayashi, M. Fujita, and A. Ajiki, Phys. Rev. B 59, 8271 (1999).
13. L. Chico, A. Ayuela, M. Pelc, H. Santos, and W. Jaskólski, Acta Phys. Pol. A 114, 1085 (2008).
14. The one-dimensional k vector is reciprocal to the translation vector, which connects the centers of the left (L) and right (R) sides of the SL unit cell.
15. We have checked that the corresponding wavefunction is localized mainly at the interface octagon defect and slowly vanishes inside the joined tubes. This interface state deserves further investigation.