TY  - JOUR
AU  - Milić, Mirjana M.
AU  - Lazarov, Nenad Đ.
AU  - Karbunar, Lazar
PY  - 2012
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/4798
AB  - In the present study, we have employed two dimensional ASYNNNI model to investigate how the Ortho-II structure formation influences doping, p, of the superconducting CuO2 planes in YBa2Cu3O6+x high-T-c superconductor. It was shown, that if the direct repulsive interaction between next nearest oxygen atoms (V-3), present in the Hamiltonian of the ASYNNNI model, is neglected, the Ortho-II ordering is destroyed and doping p becomes a linearly increasing function of oxygen concentration x in the range 0.50 LT = x LT = 0.65, for any choice of critical chain length l(cr) (defined so that CuO chains of length l LT l(cr) cannot transfer holes to the CuO2 planes). Consequently, the T-c(x) dependence, obtained by the employment of the universal T-c vs. p relation, does not exhibit experimentally observed 60 K plateau. The results presented here confirm that establishment of Ortho-II structural phase is a key factor for the 60 K plateau formation in the T-c(x) dependence. (C) 2012 Elsevier B. V. All rights reserved.
T2  - Physica. C: Superconductivity and Its Applications
T1  - Influence of Ortho-II structural phase on the 60 K plateau formation in YBa2Cu3O6+x
VL  - 476
SP  - 63
EP  - 67
DO  - 10.1016/j.physc.2012.02.008
ER  - 

@article{
author = "Milić, Mirjana M. and Lazarov, Nenad Đ. and Karbunar, Lazar",
year = "2012",
abstract = "In the present study, we have employed two dimensional ASYNNNI model to investigate how the Ortho-II structure formation influences doping, p, of the superconducting CuO2 planes in YBa2Cu3O6+x high-T-c superconductor. It was shown, that if the direct repulsive interaction between next nearest oxygen atoms (V-3), present in the Hamiltonian of the ASYNNNI model, is neglected, the Ortho-II ordering is destroyed and doping p becomes a linearly increasing function of oxygen concentration x in the range 0.50 LT = x LT = 0.65, for any choice of critical chain length l(cr) (defined so that CuO chains of length l LT l(cr) cannot transfer holes to the CuO2 planes). Consequently, the T-c(x) dependence, obtained by the employment of the universal T-c vs. p relation, does not exhibit experimentally observed 60 K plateau. The results presented here confirm that establishment of Ortho-II structural phase is a key factor for the 60 K plateau formation in the T-c(x) dependence. (C) 2012 Elsevier B. V. All rights reserved.",
journal = "Physica. C: Superconductivity and Its Applications",
title = "Influence of Ortho-II structural phase on the 60 K plateau formation in YBa2Cu3O6+x",
volume = "476",
pages = "63-67",
doi = "10.1016/j.physc.2012.02.008"
}

Milić, M. M., Lazarov, N. Đ.,& Karbunar, L.. (2012). Influence of Ortho-II structural phase on the 60 K plateau formation in YBa2Cu3O6+x. in Physica. C: Superconductivity and Its Applications, 476, 63-67.
https://doi.org/10.1016/j.physc.2012.02.008

Milić MM, Lazarov NĐ, Karbunar L. Influence of Ortho-II structural phase on the 60 K plateau formation in YBa2Cu3O6+x. in Physica. C: Superconductivity and Its Applications. 2012;476:63-67.
doi:10.1016/j.physc.2012.02.008 .

Milić, Mirjana M., Lazarov, Nenad Đ., Karbunar, Lazar, "Influence of Ortho-II structural phase on the 60 K plateau formation in YBa2Cu3O6+x" in Physica. C: Superconductivity and Its Applications, 476 (2012):63-67,
https://doi.org/10.1016/j.physc.2012.02.008 . .