Exciton Effects in Carbon Nanotube

碩士 === 崑山科技大學 === 電機工程研究所 === 93 === This thesis mainly studies the electronic properties and exciton effects of the carbon nanotube, including the effects of radius, stress, and magnetic field. In the thesis, the energy dispersion relation is calculated by the tight-binding method, and the electron...

Full description

Bibliographic Details
Main Authors: Chun-I Chang, 張鈞奕
Other Authors: To-Sing Li
Format: Others
Language:zh-TW
Published: 2005
Online Access:http://ndltd.ncl.edu.tw/handle/yj5246
id ndltd-TW-093KSUT5442052
record_format oai_dc
spelling ndltd-TW-093KSUT54420522019-05-15T20:33:45Z http://ndltd.ncl.edu.tw/handle/yj5246 Exciton Effects in Carbon Nanotube 奈米碳管中的激子效應 Chun-I Chang 張鈞奕 碩士 崑山科技大學 電機工程研究所 93 This thesis mainly studies the electronic properties and exciton effects of the carbon nanotube, including the effects of radius, stress, and magnetic field. In the thesis, the energy dispersion relation is calculated by the tight-binding method, and the electron effective mass is obtained. The exciton binding energy is evaluated by means of the variational method. From the simulation results, the energy gap of the nanotube is inversely proportional to the radius. When the tube radius is large, the Coulomb interaction between the electron and the hole is weak because of the large distance which causes the exciton binding energy to be weak. Consequently, the exciton binding energy decreases with increasing radius. Since stress alters the positions of the carbon atoms, it is necessary to recalculate the transfer integral, and the band structure and exciton binding energy are obtained. When stress increases, the conductivity of the nanotube is changed from semiconductor into metal. The nanotube, the conductivity is changed from semiconductor into metal when stress decreases. For nanotube, the conductivity is changed from metal into semiconductor. When energy gap is smaller than the binding energy, exciton state does not exist. Consider a uniform magnetic field parallel to the tube axis, and it changes the angular momentum from to . For metallic nanotube, the energy gap is proportional to the magnetic flux, while the semiconducting nanotube is inversely proportional to the magnetic flux. Consequently, when magnetic flux increases, the energy gap of the semiconducting nanotube is changed regularly. For semiconducting nanotube, when the magnetic flux is large, and the energy gap is smaller than the binding energy, therefore the exciton state does not exist. As to the metallic nanotube, when the magnetic flux is weak, the exciton state does not exist. To-Sing Li 李道聖 2005 學位論文 ; thesis 80 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 碩士 === 崑山科技大學 === 電機工程研究所 === 93 === This thesis mainly studies the electronic properties and exciton effects of the carbon nanotube, including the effects of radius, stress, and magnetic field. In the thesis, the energy dispersion relation is calculated by the tight-binding method, and the electron effective mass is obtained. The exciton binding energy is evaluated by means of the variational method. From the simulation results, the energy gap of the nanotube is inversely proportional to the radius. When the tube radius is large, the Coulomb interaction between the electron and the hole is weak because of the large distance which causes the exciton binding energy to be weak. Consequently, the exciton binding energy decreases with increasing radius. Since stress alters the positions of the carbon atoms, it is necessary to recalculate the transfer integral, and the band structure and exciton binding energy are obtained. When stress increases, the conductivity of the nanotube is changed from semiconductor into metal. The nanotube, the conductivity is changed from semiconductor into metal when stress decreases. For nanotube, the conductivity is changed from metal into semiconductor. When energy gap is smaller than the binding energy, exciton state does not exist. Consider a uniform magnetic field parallel to the tube axis, and it changes the angular momentum from to . For metallic nanotube, the energy gap is proportional to the magnetic flux, while the semiconducting nanotube is inversely proportional to the magnetic flux. Consequently, when magnetic flux increases, the energy gap of the semiconducting nanotube is changed regularly. For semiconducting nanotube, when the magnetic flux is large, and the energy gap is smaller than the binding energy, therefore the exciton state does not exist. As to the metallic nanotube, when the magnetic flux is weak, the exciton state does not exist.
author2 To-Sing Li
author_facet To-Sing Li
Chun-I Chang
張鈞奕
author Chun-I Chang
張鈞奕
spellingShingle Chun-I Chang
張鈞奕
Exciton Effects in Carbon Nanotube
author_sort Chun-I Chang
title Exciton Effects in Carbon Nanotube
title_short Exciton Effects in Carbon Nanotube
title_full Exciton Effects in Carbon Nanotube
title_fullStr Exciton Effects in Carbon Nanotube
title_full_unstemmed Exciton Effects in Carbon Nanotube
title_sort exciton effects in carbon nanotube
publishDate 2005
url http://ndltd.ncl.edu.tw/handle/yj5246
work_keys_str_mv AT chunichang excitoneffectsincarbonnanotube
AT zhāngjūnyì excitoneffectsincarbonnanotube
AT chunichang nàimǐtànguǎnzhōngdejīzixiàoyīng
AT zhāngjūnyì nàimǐtànguǎnzhōngdejīzixiàoyīng
_version_ 1719100851545440256