Magnetic proximity effect in YBCO/STO/LCMO multilayers
dc.contributor.author | Paull, O | en_AU |
dc.contributor.author | Causer, GL | en_AU |
dc.contributor.author | Pan, AV | en_AU |
dc.contributor.author | Klose, F | en_AU |
dc.date.accessioned | 2022-05-27T06:41:00Z | en_AU |
dc.date.available | 2022-05-27T06:41:00Z | en_AU |
dc.date.issued | 2017-01-31 | en_AU |
dc.date.statistics | 2021-09-24 | en_AU |
dc.description.abstract | Tailoring of the electronic properties of complex oxide heterostructures, thin films, and superlattices with atomically sharp interfaces is at the frontline of materials research at present [1, 2, 3]. Interfaces exhibit novel states that are not possible in bulk materials as a result of broken symmetry, induced strains, and modified exchange interactions. In this work we examined the interaction between a superconducting YBa2Cu3O7-δ thin film layer and a ferromagnetic La2/3Ca1/3MnO3 layer using polarised neutron reflectometry. The interaction at the interface between YBCO/LCMO multilayers has resulted in a variety of observed phenomena such as induced ferromagnetic moments in YBCO layers that are antiparallel to neighbouring LCMO layers, and a strong reduction in magnetization in LCMO near the interface. Prajapat et al. investigated the YBCO/LCMO interface using SrTiO3 (STO) as an intermediate insulating layer, and reported that the magnetic depletion (MD) in LCMO near the interface is dependent on the critical temperature of YBCO and the thickness of the LCMO layer, and claimed that the origin of the MD in LCMO is due to Cooper pairs tunneling through the STO interlayer across the interface [5]. Our work has verified the observation of the MD layer in LCMO near the interface as claimed in the past report, and additionally studied the effect of a magnetic field on this layer. Polarised neutron reflectometry measurements performed at ANSTO on the PLATYPUS reflectometer indicate that the effect of applying fields at 0.03 T and 1 T is to cause a small restoration of magnetization in this depleted layer. This result supports the mechanism proposed by Prajapat et al. of a superconductivity-induced MD from tunneling through STO. | en_AU |
dc.identifier.citation | Paull, O., Causer, G., Pan, A. V., Klose, F. (2017). Magnetic proximity effect in YBCO/STO/LCMO multilayers. Poster presented to the 41st Annual Condensed Matter and Materials Meeting, Charles Sturt University, Wagga Wagga, NSW, Australia, 31st January - 3rd February 2017, (pp. 53). Retrieved from: https://physics.org.au/wp-content/uploads/cmm/2017/Wagga_2017_Conference_Handbook.pdf | en_AU |
dc.identifier.conferenceenddate | 3 February 2017 | en_AU |
dc.identifier.conferencename | Australian and New Zealand Institutes of Physics 41st Annual Condensed Matter and Materials Meeting | en_AU |
dc.identifier.conferenceplace | Wagga Wagga, NSW | en_AU |
dc.identifier.conferencestartdate | 31 January 2017 | en_AU |
dc.identifier.other | WP12 | en_AU |
dc.identifier.pagination | 53 | en_AU |
dc.identifier.uri | https://physics.org.au/wp-content/uploads/cmm/2017/Wagga_2017_Conference_Handbook.pdf | en_AU |
dc.identifier.uri | https://apo.ansto.gov.au/dspace/handle/10238/13221 | en_AU |
dc.language.iso | en | en_AU |
dc.publisher | Australian Institute of Physics | en_AU |
dc.subject | Oxides | en_AU |
dc.subject | Thin films | en_AU |
dc.subject | Crystal lattices | en_AU |
dc.subject | Layers | en_AU |
dc.subject | Materials | en_AU |
dc.subject | Symmetry | en_AU |
dc.subject | Interactions | en_AU |
dc.subject | Copper pairs | en_AU |
dc.subject | Tunnel effect | en_AU |
dc.title | Magnetic proximity effect in YBCO/STO/LCMO multilayers | en_AU |
dc.type | Conference Poster | en_AU |