Origin of the 60K plateau in YBa_2Cu_3O_6+x

Details Origin of the 60K plateau in YBa_2Cu_3O_6+x Origin of the 60K plateau in YBa_2Cu_3O_6+x

2007-04-14

arxiv.org/abs/0704.1887v4

J. Phys.: Condens. Matter 19 (2007) 346230

Physics

Condensed Matter

Superconductivity

5 pages of text, 3 figures, corrected two typing errors: in paragraph 1 of page 2 "p(x)=0.94 - replaced by p(x)=0.094", in par

Scientific paper

10.1088/0953-8984/19/34/346230

A model for charge transfer mechanism in YBa2Cu3O6+x high-Tc cuprate based on critical chain length concept is proposed to account for 60K and 90K plateaus in Tc(x) dependence. It has been shown, when the statistics of CuO chain formation was described in terms of two dimensional asymmetric next-to-nearest neighbor Ising (ASYNNNI) model, that at any constant temperature below the top of OII phase there exists a uniquely defined value of critical chain length lcr(T) that yields a constant doping p(x)=const over the regime of OII phase (related to 60K plateau of Tc(x)), while 90K plateau coincides with the monotonously increasing p(x) over optimal doping level p=0.16 in the regime of OI phase. Short length chains (llcr(T)), are taken as not capable of attracting electrons from CuO2 planes.. It is shown that only a part (41%) of the remaining l-lcr(T)+1 holes in the long chains can capture electrons. The results obtained indicate that the ASYNNNI model and two-plateaus-like behavior of Tc(x) in YBa2Cu3O6+x are closely connected.

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