東華大學圖書館 |

語系: 繁體中文

說明(常見問題)

回圖書館首頁

手機版館藏查詢

登入

回首頁

切換: 標籤 | MARC模式 | ISBD

Raman spectroscopy of carbon nanotub...

University of Southern California., Electrical Engineering.

FindBook

Google Book

Amazon

博客來

Raman spectroscopy of carbon nanotubes under axial strain and surface-enhanced Raman spectroscopy of individual carbon nanotubes.

紀錄類型:	書目-電子資源 : Monograph/item
正題名/作者:	Raman spectroscopy of carbon nanotubes under axial strain and surface-enhanced Raman spectroscopy of individual carbon nanotubes./
作者:	Kumar, Rajay.
面頁冊數:	177 p.
附註:	Adviser: Stephen B. Cronin.
Contained By:	Dissertation Abstracts International69-06B.
標題:	Engineering, Electronics and Electrical. -
電子資源:	http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3317994
ISBN:	9780549678229

Raman spectroscopy of carbon nanotubes under axial strain and surface-enhanced Raman spectroscopy of individual carbon nanotubes.
Kumar, Rajay.

Raman spectroscopy of carbon nanotubes under axial strain and surface-enhanced Raman spectroscopy of individual carbon nanotubes. - 177 p.

Adviser: Stephen B. Cronin.

Thesis (Ph.D.)--University of Southern California, 2008.

In this thesis, I present resonant Raman spectroscopy of individual carbon nanotube bundles under axial strains up to 17%. The main effect of this strain is to cause nanotube debundling. The G band Raman spectra of metallic and semiconducting nanotubes are found to respond differently to strain and debundling, giving insight into the nature of the broad metallic G- band lineshape. For metallic nanotubes, the G- band upshifts and becomes narrower with strain, making it appear more semiconductor-like. Surprisingly, this metal to semiconductor transition is irreversible with strain, indicating that nanotube-nanotube coupling plays a significant role in the observed G - band of metallic nanotubes. The vibrational and electronic properties of these nanotubes under strain are modeled using tight-binding calculations.

ISBN: 9780549678229Subjects--Topical Terms:

626636
Engineering, Electronics and Electrical.

Raman spectroscopy of carbon nanotubes under axial strain and surface-enhanced Raman spectroscopy of individual carbon nanotubes.
LDR:03473nmm 2200325 a 45 001 867487
005 20100804
008 100804s2008 ||||||||||||||||| ||eng d
020 $a 9780549678229
035 $a (UMI)AAI3317994
035 $a AAI3317994
040 $a UMI $c UMI
100 1 $a Kumar, Rajay. $3 1036222
245 1 0 $a Raman spectroscopy of carbon nanotubes under axial strain and surface-enhanced Raman spectroscopy of individual carbon nanotubes.
300 $a 177 p.
500 $a Adviser: Stephen B. Cronin.
500 $a Source: Dissertation Abstracts International, Volume: 69-06, Section: B, page: 3750.
502 $a Thesis (Ph.D.)--University of Southern California, 2008.
520 $a In this thesis, I present resonant Raman spectroscopy of individual carbon nanotube bundles under axial strains up to 17%. The main effect of this strain is to cause nanotube debundling. The G band Raman spectra of metallic and semiconducting nanotubes are found to respond differently to strain and debundling, giving insight into the nature of the broad metallic G- band lineshape. For metallic nanotubes, the G- band upshifts and becomes narrower with strain, making it appear more semiconductor-like. Surprisingly, this metal to semiconductor transition is irreversible with strain, indicating that nanotube-nanotube coupling plays a significant role in the observed G - band of metallic nanotubes. The vibrational and electronic properties of these nanotubes under strain are modeled using tight-binding calculations.
520 $a This thesis also presents a systematic study of surface enhanced Raman spectroscopy (SERS) of carbon nanotubes. Raman spectra of individual carbon nanotubes are measured by scanning a focused laser spot (0.5 mum diameter) over a large area (100 mum2) before and after depositing silver nanoparticles. Local regions exhibiting SERS enhancement were located relative to a lithographically patterned grid, allowing subsequent scanning electron microscopy to be performed. The uniquely large aspect ratio of carbon nanotubes enables imaging of the nanoparticle geometry together with the SERS active molecule. By measuring the same individual carbon nanotube before and after metal nanoparticle deposition, the SERS enhancement factor is determined unambiguously. SERS enhancement factors up to 134,000, a consistent upshift in the G band Raman frequency and nanoparticle heating in excess of 600°C are revealed.
520 $a Nanotubes are also strained through top-down microprocessing. By straining nanotubes to the bottom of a trench made deeper through etching, we induce changes in nanotubes' resonance with an incident laser. This causes increases in intensity for all the bands, most notably the radial breathing mode. From the radial breathing mode intensity, we calculate the changes to the density of states. Furthermore, we observe two peaks in the G ' band spectrum, which also reflects changes in the density of states. All nanotubes measured experienced irreversible changes in their D bands, indicating the build up of residue on the nanotube surface from etching.
590 $a School code: 0208.
650 4 $a Engineering, Electronics and Electrical. $3 626636
650 4 $a Physics, Electricity and Magnetism. $3 1019535
690 $a 0544
690 $a 0607
710 2 $a University of Southern California. $b Electrical Engineering. $3 1020963
773 0 $t Dissertation Abstracts International $g 69-06B.
790 $a 0208
790 1 0 $a Cronin, Stephen B., $e advisor
790 1 0 $a Thompson, Mark E. $e committee member
790 1 0 $a Zhou, Chongwu $e committee member
791 $a Ph.D.
792 $a 2008
856 4 0 $u http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3317994