Monte Carlo simulation of oxygen diffusion in planar model of 123 YBCO Low-temperature regime and effect of trapping barrier

Abstract The asymmetric next-nearest neighbour lattice gas model is used for describing the oxygen-vacancy phase diffusion in the basal plane of 123 YBaCuO superconducting ceramics at low temperatures. A finite value Q for the trapping potential barrier is added. The Monte Carlo technique has been used to obtain the components of the (tracer) diffusion coefficient. The character of its dependence on the coverage is shown to vary, from convex at high temperatures to concave at lower ones. The temperature of the transition depends on the trapping barrier height. The activation energy (obtained from an Arrhenius plot) is seen to be varying as a function of coverage and the trapping barrier, and is not symmetrical with respect to c =0.5 if Q is finite. The same of course is true for the diffusion coefficient. The value of the “final-state-energy” is reported and compared to the ground-state energy. This indicates the likely occurence of fine structure at specific coverage values corresponding to a recently predicted devil's staircase distribution of superstructure phases. The time evolution of twins is also reported. A discussion of the limited validity of the model for describing the 123 structural phase diagram is presented.

[1]  Khachaturyan,et al.  Structural transformations in nonstoichiometric YBa2Cu3O6+ delta. , 1992, Physical review. B, Condensed matter.

[2]  V. Matić An Ising model approach to the problem of oxygen ordering in the basal plane of YBa2Cu3O6 + 2c , 1992 .

[3]  A. Aligia,et al.  Thermodynamics of O ordering in YBa2Cu3O6+x: Effect of Coulomb repulsion , 1992 .

[4]  R Gomer Diffusion of adsorbates on metal surfaces , 1990 .

[5]  R. Gomer,et al.  A Monte Carlo study of surface diffusion coefficients in the presence of adsorbate–adsorbate interactions. III. Repulsive nearest‐neighbor and attractive next‐nearest‐neighbor interactions , 1991 .

[6]  R. Gronsky,et al.  Long-range interactions, long-range order and a devil's staircase in YBa2Cu3Oz , 1992 .

[7]  G. Ceder,et al.  On the Asymmetric Next-Nearest-Neighbor Ising Model of Oxygen Ordering in YBa2Cu3Oz , 1992 .

[8]  Khachaturyan,et al.  Kinetics of strain-related morphology transformation in YBa2Cu3O7- delta. , 1991, Physical review letters.

[9]  Salomons,et al.  Monte Carlo study of tracer and chemical diffusion of oxygen in YBa2Cu3O6+2c. , 1990, Physical review. B, Condensed matter.

[10]  H. Verweij,et al.  3-D vacancy ordered superstructures in “homogeneous” YBa2Cu3O7-δ , 1989 .

[11]  Zhang,et al.  Molecular-dynamics study of oxygen diffusion in YBa2Cu3O6.91. , 1992, Physical review. B, Condensed matter.

[12]  D. de Fontaine,et al.  Low-temperature long-range oxygen order in YBa2Cu3O z , 1990, Nature.

[13]  M. D. Fontaine,et al.  COMPUTATION OF THE OI-OII-OIII PHASE DIAGRAM AND LOCAL OXYGEN CONFIGURATIONS FOR YBA2CU3OZ WITH Z BETWEEN 6.5 AND 7 , 1991 .

[14]  THERMODYNAMICS OF OXYGEN ORDERING IN YBa2Cu3Oz , 1988 .

[15]  de Fontaine D,et al.  Oxygen-vacancy phase equilibria in YBa2Cu3Oz calculated by the cluster variation method. , 1988, Physical review. B, Condensed matter.

[16]  B. Dabrowski,et al.  Defects, defect ordering, structural coherence and superconductivity in the 123 copper oxides , 1991 .

[17]  B. Batlogg Physical Properties of High‐Tc Superconductors , 1991 .

[18]  A. Aligia,et al.  Phase separation and devil's staircase in models for O ordering in RBa2Cu3O6+x , 1994 .

[19]  M. Islam Computer simulation study of oxygen migration in YBa2Cu3O7 , 1990 .

[20]  M. Marezio Oxygen stoichiometry in high‐Tc superconductors , 1991 .

[21]  R. Gomer,et al.  A Monte Carlo study of surface diffusion coefficients in the presence of adsorbate–adsorbate interactions. I. Repulsive interactions , 1991 .

[22]  K. Binder,et al.  Diffusion of absorbed atoms in ordered and disordered monolayers at surfaces , 1983 .