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Superconductivity in LnBa2Cu3O7 − δ with Ln = Nd, Eu, Gdand Dy has been investigated as a function of δ, closely following the accompanying changes in crystal structure. Orthorhombic GdBa2Cu3O7 − δ and DyBa2Cu3O7 − δ show a T c of ≈ 90 K up to δ = 0.2 and a lower T c plateau (40–50 K) in the δ range 02 to 0.4, similar to that found in YBa2Cu3O7 − δ. The orthorhombic structure II in the lower T c regions is different from the structure I in the 90 K T c (low δ) region. The unit cell parameters of the orthorhombic I structure in the high T c region bear the relationship of a a ≠ b ∼ c/3. This relationship is not seen in the low T c plateau. The low T c plateau region does not distinctly manifest itself in NdBa2Cu3O7 − δ just as in LaBa2Cu3O7 − δ.
Epitaxial thin films of ferromagnetic La 0.7 Sr 0.3 MnO 3 (LSMO) and charge‐ordered, antiferromagnetic Y 0.5 Ca 0.5 MnO 3 (YCMO) were deposited on SrTiO 3 (100) substrates by pulsed laser deposition (PLD). The heterostructure undergoes tetragonal distortion due to strong biaxial tensile strain imposed by the substrate. The LSMO–YCMO bilayers exhibit significant exchange bias (EB) across the interface even in a very small remnant magnetic field (∼5 Oe) present in the superconductor magnet. The unidirectional exchange anisotropy at the interface can be switched by reversing the polarity of the remnant magnetic field. magnified image Significant asymmetry in the M ( H ) loop is exhibited by the heterostructure interface under cooling in the presence of small remnant magnetic field ( H r ∼ 5 Oe). (© 2016 WILEY‐VCH Verlag GmbH &Co. KGaA, Weinheim)