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...
Main Author: | |
---|---|
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 |
id |
doaj-4d1267767e3f464fad2154fa9858243c |
---|---|
record_format |
Article |
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 |
work_keys_str_mv |
AT etetik theelectronicpropertiesofdopedsinglewalledcarbonnanotubesandcarbonnanotubesensors AT etetik electronicpropertiesofdopedsinglewalledcarbonnanotubesandcarbonnanotubesensors |
_version_ |
1725485725925769216 |