|
|
|
|
| LEADER |
01535 am a22002413u 4500 |
| 001 |
88689 |
| 042 |
|
|
|a dc
|
| 100 |
1 |
0 |
|a Hasdeo, Eddwi H.
|e author
|
| 100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science
|e contributor
|
| 100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Physics
|e contributor
|
| 100 |
1 |
0 |
|a Dresselhaus, Mildred
|e contributor
|
| 700 |
1 |
0 |
|a Nugraha, Ahmad R. T.
|e author
|
| 700 |
1 |
0 |
|a Sato, Kentaro
|e author
|
| 700 |
1 |
0 |
|a Dresselhaus, Mildred
|e author
|
| 700 |
1 |
0 |
|a Saito, Riichiro
|e author
|
| 245 |
0 |
0 |
|a Electronic Raman scattering and the Fano resonance in metallic carbon nanotubes
|
| 260 |
|
|
|b American Physical Society,
|c 2014-08-13T13:01:53Z.
|
| 856 |
|
|
|z Get fulltext
|u http://hdl.handle.net/1721.1/88689
|
| 520 |
|
|
|a The Fano resonance spectra for the G band in metallic carbon nanotubes are calculated as a function of laser excitation energy, in which the origin of the resonance is given by an interference between the continuous electronic Raman spectra and the discrete phonon spectra. We found that the second-order scattering process of the q ≠ 0 electron-electron interaction is more relevant to the continuous spectra rather than the q = 0 first-order process because the q = 0 direct Coulomb interaction vanishes due to the symmetry of the two sublattices of a carbon nanotube.
|
| 520 |
|
|
|a National Science Foundation (U.S.). Division of Materials Research (Grant 10-04147)
|
| 546 |
|
|
|a en_US
|
| 655 |
7 |
|
|a Article
|
| 773 |
|
|
|t Physical Review B
|
