dc.contributor.author |
Muthu, D V S
|
|
dc.contributor.author |
Sashikala, M N
|
|
dc.contributor.author |
Sood, A K
|
|
dc.contributor.author |
Seshadri, R
|
|
dc.contributor.author |
Rao, C N R
|
|
dc.date.accessioned |
2012-12-07T05:36:36Z |
|
dc.date.available |
2012-12-07T05:36:36Z |
|
dc.date.issued |
1994-01-07 |
|
dc.identifier |
0009-2614 |
en_US |
dc.identifier.citation |
Chemical Physics Letters 217(1-2), 146-151 (1994) |
en_US |
dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/1239 |
|
dc.description |
Restricted Access |
en_US |
dc.description.abstract |
Raman studies on powder samples of C-60.TDAE are reported in the temperature range of 296 to 14 K. The strongest line A(g)(2) shows a doublet at 1454 and 1463 cm(-1) whose relative intensities are strongly temperature dependent. The relative intensities of the H-g(7) and H-g(8) modes at 296 K are much higher than those in pure C-60 and these intensities increase at low temperatures. The phonon softening and broadening are compared with the results on alkali-doped C-60 and the theoretical calculations. |
en_US |
dc.description.uri |
http://dx.doi.org/10.1016/0009-2614(93)E1347-J |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Elsevier Science BV |
en_US |
dc.rights |
© 1994 Elsevier Science BV |
en_US |
dc.subject |
Superconductivity |
en_US |
dc.subject |
Ferromagnetism |
en_US |
dc.subject |
C60 |
en_US |
dc.subject |
Raman study |
en_US |
dc.title |
Raman study of the doped fullerene C60·TDAE |
en_US |
dc.type |
Article |
en_US |