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The FM/S/FM trilayer: Inhomogeneous π-phase superconductivity, but also a possible existence π phase superconducting states in such trilayers. The presence of π magnetic
The FM/S/FM trilayer: Inhomogeneous π-phase superconductivity, but also a possible existence π phase superconducting states in such trilayers. The presence of π magnetic
Superconducting probe of electronic correlations and exchange field based on the proximity effect in F/S nanostructures, and the thickness df of the F layer are derived for F/S bilayers and F/S/F trilayers. Two new π-phase
πPhase superconductivity and magnetism in ferromagnet/superconductor/ ferromagnet trilayers and S layers. In the FM/S superlattices there are also two π-phase magnetic states (0π and ππ
Superconducting probe of electronic correlations and exchange field based on the proximity effect in F/S nanostructures, and the thickness df of the F layer are derived for F/S bilayers and F/S/F trilayers. Two new π-phase
πPhase superconductivity and magnetism in ferromagnet/superconductor/ ferromagnet trilayers and S layers. In the FM/S superlattices there are also two π-phase magnetic states (0π and ππ
Adjustment of superconductivity and ferromagnetism in the few-layered ferromagnet-superconductor nanostructures superconductivity and the 0 and π phase magnetism and nonequivalence of layers) and even the F/S superlattices
π magnetic states of ferromagnet/superconductor superlattices ferromagnetic states 00 and π0. Therefore, the Tc oscillation origin at dsπ is due to the 0 π-ππ-0π phase
π-phase magnetism in ferromagnet-superconductor superlattices dπ s is due to the phase transition cascade 0π-ππ-0π. At ds > dπ s, the Tc oscillations are caused
Adjustment of superconductivity and ferromagnetism in the few-layered ferromagnet-superconductor nanostructures superconductivity and the 0 and π phase magnetism and nonequivalence of layers) and even the F/S superlattices
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