Laser-Induced High Local Temperature in Carbon Nanotube

2007 ◽  
Vol 121-123 ◽  
pp. 331-336 ◽  
Author(s):  
Ming Liu ◽  
K.L. Jiang ◽  
Q.Q. Li ◽  
H.T. Yang ◽  
S.S. Fan

Laser irradiated carbon nanotubes in vacuum can emit dazzling yellow light due to the laser heating effect. We investigated the phonon frequency shifts of as irradiated carbon nanotube bundles by Raman spectroscopy under ultraviolet laser illumination (325 nm, 2.4 mW), the G band peak position was found to shift 50 cm-1 to lower wave number. By considering the temperature coefficient of the G band shift, the local temperature of the illuminated spot was predicted to be nearly 2000K. This temperature had a linear relationship with the incident laser power, and also was greatly influenced by the pressure of the vacuum chamber. The photoluminescence of the CNT bundle was also studied, which exhibits an oscillation of 0.1 eV, a possible origin of the oscillation was discussed.

2007 ◽  
Vol 308 (1) ◽  
pp. 276-284 ◽  
Author(s):  
Shigenori Utsumi ◽  
Mamiko Kanamaru ◽  
Hiroaki Honda ◽  
Hirofumi Kanoh ◽  
Hideki Tanaka ◽  
...  

Author(s):  
Shuiliang Wang ◽  
Zhequn Huang ◽  
Wenbo Shi ◽  
Dongwook Lee ◽  
Qixiang Wang ◽  
...  

2013 ◽  
Vol 39 (5) ◽  
pp. 441-445 ◽  
Author(s):  
M. I. Bagatskii ◽  
M. S. Barabashko ◽  
V. V. Sumarokov

2005 ◽  
Vol 34 (9) ◽  
pp. 1218-1219 ◽  
Author(s):  
Bunshi Fugetsu ◽  
Wenhai Han ◽  
Noriaki Endo ◽  
Yuichi Kamiya ◽  
Toshio Okuhara

2001 ◽  
Vol 223 (2) ◽  
pp. 479-487 ◽  
Author(s):  
P.V. Teredesai ◽  
A.K. Sood ◽  
S.M. Sharma ◽  
S. Karmakar ◽  
S.K. Sikka ◽  
...  

Langmuir ◽  
2008 ◽  
Vol 24 (11) ◽  
pp. 5746-5754 ◽  
Author(s):  
Sandeep Agnihotri ◽  
Pyoungchung Kim ◽  
Yijing Zheng ◽  
José P. B. Mota ◽  
Liangcheng Yang

1999 ◽  
Vol 82 (26) ◽  
pp. 5305-5308 ◽  
Author(s):  
W. Teizer ◽  
R. B. Hallock ◽  
E. Dujardin ◽  
T. W. Ebbesen

RSC Advances ◽  
2016 ◽  
Vol 6 (33) ◽  
pp. 27260-27266 ◽  
Author(s):  
G. Ramos-Sanchez ◽  
G. Chen ◽  
A. R. Harutyunyan ◽  
P. B. Balbuena

Lithium stored in interstitial sites reflects the actual low capacity observed from the 2nd cycle and beyond.


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