dc.contributor.author |
Santra, A K
|
|
dc.contributor.author |
Sarma, D D
|
|
dc.contributor.author |
Rao, C N R
|
|
dc.date.accessioned |
2012-11-16T10:19:59Z |
|
dc.date.available |
2012-11-16T10:19:59Z |
|
dc.date.issued |
1991 |
|
dc.identifier |
0163-1829 |
en_US |
dc.identifier.citation |
Physical Review B 43(7), 5612-5615 (1991) |
en_US |
dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/991 |
|
dc.description |
Restricted Access |
en_US |
dc.description.abstract |
Cu 2p core-level photoemission studies of La2-xSrxCuO4, BiPbSr2Y1-xCa1-xCu2O8, and other cuprates show that the relative intensity of the satellite varies with the composition in a direction opposite to that of the hole concentration, nh. The IS/IM-nh relations in the different cuprate series can be understood in terms of the Δ/tpd ratio, where Δ is the charge-transfer excitation energy and tpd is the hybridization strength between the Cu 3d and O 2p orbitals. Interestingly, the IS/IM ratio increases with the Δ/tpd ratio in the cuprates. At a given value of nh, e.g., around the value corresponding to maximum Tc, IS/IM increases in the same direction as Tc among the different series of cuprates, suggesting thereby that Tc itself may be determined by Δ/tpd. |
en_US |
dc.description.uri |
http://dx.doi.org/10.1103/PhysRevB.43.5612 |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
American Physical Society |
en_US |
dc.rights |
© 1991 The American Physical Society |
en_US |
dc.subject |
Hole Concentration |
en_US |
dc.subject |
TC |
en_US |
dc.subject |
electronic structure |
en_US |
dc.subject |
superconductivity of cuprates |
en_US |
dc.subject |
Cu 2p core-level photoemission |
en_US |
dc.title |
Relation between the electronic structure and the superconductivity of cuprates as revealed by Cu 2p photoemission and theoretical investigations |
en_US |
dc.type |
Article |
en_US |