Anjli Chhikara et al 1999 J. Phys.: Condens. Matter 11 L229 doi:10.1088/0953-8984/11/22/101
Anjli Chhikara
, K R Priolkar
, P R Sarode
, R B Prabhu
and A V Narlikar![]()
In this letter we report our measurements of Er and Pr L3 edges in Er1-xPrxBa2Cu4O8, 0
x
0.6. The normalized L3-edge intensity is seen to closely follow the behaviour of Tc 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 I I 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 4f2L and 4f1 at the Pr site, where L is a ligand hole.
74.62.Dh Effects of crystal defects, doping and substitution
74.72.Jt Other cuprates, including Tl and Hg-based cuprates
Issue 22 (7 June 1999)
Received 10 March 1999, in final form 29 April 1999
Anjli Chhikara et al 1999 J. Phys.: Condens. Matter 11 L229
Jerzy Dajka et al 2007 J. Phys. A: Math. Theor. 40 F879
Hiroko Shinnaga et al 2004 ApJ 616 L47
L Li et al 2009 J. Phys. G: Nucl. Part. Phys. 36 125107
M Katsikini et al 2009 J. Phys.: Conf. Ser. 190 012065
Adam Doliwa 2007 J. Phys. A: Math. Theor. 40 12539
T Skrypnyk 2009 J. Phys. A: Math. Theor. 42 472004
M. Schneider et al 2009 Nucl. Fusion 49 125005
Helena Uusijärvi et al 2008 Phys. Med. Biol. 53 4369
D Baye et al 2009 J. Phys. B: At. Mol. Opt. Phys. 42 225102