| dc.contributor.author | Chhikara, A. | |
| dc.contributor.author | Priolkar, K.R. | |
| dc.contributor.author | Sarode, P.R. | |
| dc.contributor.author | Prabhu, R.B. | |
| dc.contributor.author | Narlikar, A.V. | |
| dc.date.accessioned | 2015-06-03T07:16:59Z | |
| dc.date.available | 2015-06-03T07:16:59Z | |
| dc.date.issued | 1999 | |
| dc.identifier.citation | Journal of Physics-Condensed Matter. 11(22); 1999; L229-L233. | en_US |
| dc.identifier.uri | http://dx.doi.org/10.1088/0953-8984/11/22/101 | |
| dc.identifier.uri | http://irgu.unigoa.ac.in/drs/handle/unigoa/1106 | |
| dc.description.abstract | In this letter we report our measurements of Er and PrL(3) edges in Er(1-x)Pr(x)Ba(2)Cu(4)O(8), 0 less than or equal to x less than or equal to 0.6. The normalized L(3)-edge intensity is seen to closely follow the behaviour of T(c) with the Pr concentration in these compounds. This can be related to the fact that there is a reduction in the number of mobile carriers with increasing Pr-doping level. This picture lends support to a recent model proposed by Liechtenstein and Mazin (Liechtenstein A I and Mazin II 1995 Phys. Rev. Lett. 70 1000) according to which the holes are localized in a band which crosses the Fermi level along with a hybridized state of 4f sup(2)L and 4f sup(1) at the Pr site, where L is a ligand hole. | en_US |
| dc.publisher | IOP Publishing | en_US |
| dc.subject | Physics | en_US |
| dc.title | Superconductivity suppression in (Er(1-x)Pr(x))Ba(2)Cu(4)O(8): An x-ray absorption spectroscopic study | en_US |
| dc.type | Journal article | en_US |
| dc.identifier.impf | y |