dc.contributor.author |
Serrao, Claudy Rayan
|
|
dc.contributor.author |
Krupanidhi, S B
|
|
dc.contributor.author |
Bhattacharjee, Joydeep
|
|
dc.contributor.author |
Waghmare, Umesh V
|
|
dc.contributor.author |
Kundu, Asish K
|
|
dc.contributor.author |
Rao, C N R
|
|
dc.date.accessioned |
2011-03-22T08:38:49Z |
|
dc.date.available |
2011-03-22T08:38:49Z |
|
dc.date.issued |
2006-10-01 |
|
dc.identifier |
0021-8979 |
en_US |
dc.identifier.citation |
Journal of Applied Physics 100(7) , 076104-1-2 (2006) |
en_US |
dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/74 |
|
dc.description.abstract |
InMnO3 which has a hexagonal structure similar to that of YMnO3 is found to show a canted antiferromagnetic behavior below 50 K (T-N) and a ferroelectric (FE) transition at 500 K accompanied by hystersis. We have determined the structure, polarization, and energetics of the FE and paraelectric (PE) phases of InMnO3 using first-principles density functional theory calculations based on pseudopotentials and a plane-wave basis, and find the polarization of the PE phase to be a half-integer quantum. The difference in polarization of the FE and PE phases calculated along a simple path is different from the absolute value of polarization of the FE phase. A weak piezoelectric response is exhibited by InMnO3 to uniaxial strain. (c) 2006 American Institute of Physics. |
en_US |
dc.description.uri |
http://dx.doi.org/10.1063/1.2356093 |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
American Institute of Physics |
en_US |
dc.rights |
© 2006 American Institute of Physics |
en_US |
dc.subject |
Magnetic Ferroelectrics |
en_US |
dc.subject |
Ymno3 |
en_US |
dc.subject |
Polarization |
en_US |
dc.subject |
Transition |
en_US |
dc.title |
InMnO3: A biferroic |
en_US |
dc.type |
Article |
en_US |