Demonstration of polycrystalline thin film coatings on glass for spin Seebeck energy harvesting
Source abstract
Abstract
The spin Seebeck effect, a newly discovered phenomena, has been suggested as a potential ‘game changer’ for thermoelectric technology due to the possibility of separating the electric and thermal conductivities. This is due to a completely different device architecture where, instead of an arrangement of p‐ and n‐type pillars between two ceramic blocks, a thermopile could be deposited directly onto a magnetic film of interest. Here we report on the spin Seebeck effect in polycrystalline Fe3O4:Pt bilayers deposited onto amorphous glass substrates with a view for economically viable energy harvesting. Crucially, these films exhibit large coercive fields (197 Oe) and retain 75% of saturation magnetisation, in conjunction with energy conversion comparable to epitaxially grown films. This demonstrates the potential of this technology for widespread application in harvesting waste heat for electricity.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Metamaterials and Metasurfaces Applications · Quantum and electron transport phenomena · Advanced Thermoelectric Materials and Devices
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics Loughborough University Loughborough LE11 3TU United Kingdom
Loughborough Materials Characterisation Centre Department of Materials, Loughborough University Loughborough LE11 3TU United Kingdom
Warwick Manufacturing Group University of Warwick Coventry CV4 7AL United Kingdom
References (26)
Show source-provided references
1. 10.1088/0953-8984/26/34/34320210.1088/0953-8984/26/34/343202 ↗
2. 10.1038/nmat330110.1038/nmat3301 ↗
3. 10.1143/APEX.5.09300110.1143/APEX.5.093001 ↗
4. 10.1063/1.479348610.1063/1.4793486 ↗
5. 10.1109/TMAG.2013.226294710.1109/TMAG.2013.2262947 ↗
6. Uchida K. · J. Appl. Phys · 2010 · 107 · 09A95110.1063/1.3357413 ↗
7. 10.1038/nmat285610.1038/nmat2856 ↗
8. 10.1038/nmat286010.1038/nmat2860 ↗
9. 10.7567/APEX.8.08300110.7567/APEX.8.083001 ↗
10. 10.1038/nature1122110.1038/nature11221 ↗
11. 10.1103/PhysRevLett.111.18720110.1103/PhysRevLett.111.187201 ↗
12. 10.1063/1.352994410.1063/1.3529944 ↗
13. 10.1103/PhysRevLett.110.06720710.1103/PhysRevLett.110.067207 ↗
14. 10.1038/srep0442910.1038/srep04429 ↗
15. 10.1063/1.491676210.1063/1.4916762 ↗
16. 10.1103/PhysRevB.65.06441710.1103/PhysRevB.65.064417 ↗
17. 10.1186/1556-276X-9-9610.1186/1556-276X-9-96 ↗
18. 10.1103/PhysRev.126.42710.1103/PhysRev.126.427 ↗
19. 10.1088/0022-3719/20/8/01310.1088/0022-3719/20/8/013 ↗
20. 10.1103/PhysRevLett.107.04660110.1103/PhysRevLett.107.046601 ↗
21. 10.1103/PhysRevLett.111.17660110.1103/PhysRevLett.111.176601 ↗
22. 10.1063/1.481946010.1063/1.4819460 ↗
23. 10.7567/APEX.7.09300110.7567/APEX.7.093001 ↗
24. 10.1103/PhysRevB.88.09441010.1103/PhysRevB.88.094410 ↗
25. R. W.Powell C. Y.Ho andP. E.Liley in: Thermal Conductivity of Selected Materials (National Standard Reference Series National Bureau of Standards 1966).10.6028/NBS.NSRDS.8 ↗
26. 10.1063/1.293067910.1063/1.2930679 ↗