Intergrain flux-pinning in relation to structural phase transformation and tweed formation in..

[1]  J. Rhyner,et al.  Analysis of the low field critical state in ceramic high-Tc superconductors , 1991 .

[2]  D. Niarchos,et al.  Crystallographic, thermogravimetric and magnetizaion study of the Yba2Cu3-xFexOy superconductor (O ≤ x ≤ 0.2, 6 ≤ y ≤ 7 , 1991 .

[3]  K. Parlinski,et al.  Microstructures in high Tc superconductors , 1991 .

[4]  C. Meingast,et al.  Thermal-expansion, specific-heat, and pressure dependence of Tc in YBa2 (Cu1−xMx)3O7−δ: M=Fe and Zn , 1991 .

[5]  L. Tanner,et al.  "Tweed" structure of Fe-doped YBa2Cu3O7-δ , 1991 .

[6]  B. Batlogg,et al.  Structural anomalies, oxygen ordering and superconductivity in oxygen deficient Ba2YCu3Ox , 1990 .

[7]  W. Schmahl.  LANDAU-MODEL FOR THE LAMBDAL TRANSITION IN NANO3 , 1990 .

[8]  K. Müller.  AC susceptibility of high temperature superconductors in a critical state model , 1989 .

[9]  S. Parkin,et al.  Oxygen ordering, phase separation and the 60-K and 90-K plateaus in YBa2Cu3Ox , 1989, Nature.

[10]  A. Hoser,et al.  Structural changes of the superconductor YBa2Cu3O7 by cobalt substitution. A high-resolution neutron powder diffraction study , 1989 .

[11]  Tang,et al.  Coexistence of antiferromagnetism and superconductivity in YBa2(CU1-xFex)3O7 only for x around 0.10. , 1989, Physical review. B, Condensed matter.

[12]  K. Müller,et al.  Josephson vortices and flux penetration in high temperature superconductors , 1989 .

[13]  Goldfarb,et al.  Flux creep and activation energies at the grain boundaries of Y-Ba-Cu-O superconductors. , 1989, Physical review. B, Condensed matter.

[14]  Xu,et al.  Microstructure, lattice parameters, and superconductivity of YBa2(Cu1-xFex)3O7- delta for 0 <= x <= 0.33. , 1989, Physical review. B, Condensed matter.

[15]  S. D. Murphy,et al.  AC susceptibility of sintered high Tc superconductors — Bean's model and shielding current , 1989 .

[16]  E. Salje,et al.  X-ray diffraction study of the orientational order/disorder transition in NaNO3: Evidence for order parameter coupling , 1989 .

[17]  A. Putnis,et al.  Twin formation and structural modulations in orthorhombic and tetragonal YBa2(Cu1−xCox)3O7−δ , 1989 .

[18]  W. Schmahl,et al.  An x-ray study of coupling between acoustic and optic modes at the ferroelastic phase transition in As2O5 , 1988 .

[19]  Niu,et al.  Neutron-diffraction study of NdBa2Cu3O7+x with x=0.06 and 0.18. , 1988, Physical review. B, Condensed matter.

[20]  Blatter,et al.  New critical-state model for critical currents in ceramic high-Tc superconductors. , 1988, Physical review. B, Condensed matter.

[21]  W. F. Peck,et al.  Studies of oxygen-deficient Ba2YCu3O7−δ and superconductivity Bi(Pb)SrCaCuO , 1988 .

[22]  J. Clem.  Granular and superconducting-glass properties of the high-temperature superconductors , 1988 .

[23]  Greene,et al.  Structural and physical properties of the metal (M) substituted YBa2Cu3-xMxO7-y perovskite. , 1988, Physical review. B, Condensed matter.

[24]  Y. Takeda,et al.  Microdomain Structure in YBa2(Cu1-xFex)3O7-y Observed by Electron Microscopy , 1988 .

[25]  J. Pannetier,et al.  Crystallographic study of tetragonal, superconducting YBa2(Cu0.93Fe0.05)3O7 , 1988 .

[26]  Yinglie Liu,et al.  Superconductivity in the new high-Tc superconductors RBa2Cu3O9-y (R=Y, Nd, Sm, Eu, Gd, Dy, Er, Tm, Yb) , 1987 .

[27]  Y. Maeno,et al.  Substitution for copper in a high-Tc superconductor YBa2Cu3O7–δ , 1987, Nature.

[28]  Chu,et al.  Superconductivity above 90 K in the square-planar compound system ABa2Cu3O6+x with A=Y, La, Nd, Sm, Eu, Gd, Ho, Er and Lu. , 1987, Physical review letters.

[29]  Murphy,et al.  New superconducting cuprate perovskites. , 1987, Physical review letters.

[30]  Chu,et al.  Superconductivity at 93 K in a new mixed-phase Yb-Ba-Cu-O compound system at ambient pressure. , 1987, Physical review letters.

[31]  C. F. Hempstead,et al.  Magnetization and Critical Supercurrents , 1963 .

[32]  C. P. Bean.  Magnetization of hard superconductors , 1962 .