The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors

We present ab initio calculations on the band structure and density of states of single wall semiconducting carbon nanotubes with high degrees (up to 25%) of B, Si and N substitution. The doping process consists of two phases: different carbon nanotubes (CNTs) for a constant doping rate and differen...

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Main Author: E. Tetik
Format: Article
Language:English
Published: Institute for Condensed Matter Physics 2014-12-01
Series:Condensed Matter Physics
Subjects:
Online Access:http://dx.doi.org/10.5488/CMP.17.43301
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spelling doaj-4d1267767e3f464fad2154fa9858243c2020-11-24T23:48:32ZengInstitute for Condensed Matter PhysicsCondensed Matter Physics1607-324X2014-12-011744330110.5488/CMP.17.43301The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensorsE. TetikWe present ab initio calculations on the band structure and density of states of single wall semiconducting carbon nanotubes with high degrees (up to 25%) of B, Si and N substitution. The doping process consists of two phases: different carbon nanotubes (CNTs) for a constant doping rate and different doping rates for the zigzag (8, 0) carbon nanotube. We analyze the doping dependence of nanotubes on the doping rate and the nanotube type. Using these results, we select the zigzag (8, 0) carbon nanotube for toxic gas sensor calculation and obtain the total and partial densities of states for CNT (8, 0). We have demonstrated that the CNT (8, 0) can be used as toxic gas sensors for CO and NO molecules, and it can partially detect Cl<sub>2</sub> toxic molecules but cannot detect H<sub>2</sub>S. To overcome these restrictions, we created the B and N doped CNT (8, 0) and obtained the total and partial density of states for these structures. We also showed that B and N doped CNT (8, 0) can be used as toxic gas sensors for such molecules as CO, NO, Cl<sub>2</sub> and H<sub>2</sub>S.http://dx.doi.org/10.5488/CMP.17.43301ab initio calculationscarbon nanotubes structuregas sensorsdoping and substitution effects
collection DOAJ
language English
format Article
sources DOAJ
author E. Tetik
spellingShingle E. Tetik
The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
Condensed Matter Physics
ab initio calculations
carbon nanotubes structure
gas sensors
doping and substitution effects
author_facet E. Tetik
author_sort E. Tetik
title The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
title_short The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
title_full The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
title_fullStr The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
title_full_unstemmed The electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
title_sort electronic properties of doped single walled carbon nanotubes and carbon nanotube sensors
publisher Institute for Condensed Matter Physics
series Condensed Matter Physics
issn 1607-324X
publishDate 2014-12-01
description We present ab initio calculations on the band structure and density of states of single wall semiconducting carbon nanotubes with high degrees (up to 25%) of B, Si and N substitution. The doping process consists of two phases: different carbon nanotubes (CNTs) for a constant doping rate and different doping rates for the zigzag (8, 0) carbon nanotube. We analyze the doping dependence of nanotubes on the doping rate and the nanotube type. Using these results, we select the zigzag (8, 0) carbon nanotube for toxic gas sensor calculation and obtain the total and partial densities of states for CNT (8, 0). We have demonstrated that the CNT (8, 0) can be used as toxic gas sensors for CO and NO molecules, and it can partially detect Cl<sub>2</sub> toxic molecules but cannot detect H<sub>2</sub>S. To overcome these restrictions, we created the B and N doped CNT (8, 0) and obtained the total and partial density of states for these structures. We also showed that B and N doped CNT (8, 0) can be used as toxic gas sensors for such molecules as CO, NO, Cl<sub>2</sub> and H<sub>2</sub>S.
topic ab initio calculations
carbon nanotubes structure
gas sensors
doping and substitution effects
url http://dx.doi.org/10.5488/CMP.17.43301
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