Magneto-transport in La2/3Sr1/3MnO3/YBa2Cu3O7/Alq3/Co spin-valves
Cerreta, AndreaPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland
Gaina, RoxanaPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland
Nuccio, LauraPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland
Marozau, IvanPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland - CSEM S, Neuchâtel, Switzerland
Sen, KaushikPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland - Institute for Solid State Physics, Karlsruhe Institute of Technology, Eggenstein- Leopoldshafen, Germany
De Andrés Prada, RobertoPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland - Department of Physics, Stockholm University, Stockholm, Sweden
Sarkar, SubhrangsuPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland
Bernhard, ChristianPhysics Department and Fribourg Center for Nanomaterials (FriMat), University of Fribourg, Switzerland
English
We studied how an additional layer of the high superconductor YBCO affects the magneto-transport across a LSMO/Alq3/Co spin-valve structure. We found that up to a thickness of at least 10 nm the YBCO layer on top of LSMO hardly changes the spin-valve effect, since the device resistance still depends on the relative orientation of the LSMO and Co magnetization. The spin-valve effect persists even when the superconducting YBCO layer acts as bottom electrode, with no spin-polarized current injected from LSMO into YBCO. This highlights that the charge carriers of a thin YBCO layer on top of LSMO are strongly spin-polarized, most likely due to a magnetic proximity effect involving a transfer of spin-polarized electrons from LSMO to YBCO. Evidence for a strongly underdoped state of the YBCO layers close to the interface with LSMO is indeed obtained from the dI/dV curves in zero magnetic field which reveal a pseudogap persisting well above .