High quality ferromagnetic 0 and pi Josephson tunnel junctions
| dc.creator | Weides, M. | |
| dc.creator | Kemmler, M. | |
| dc.creator | Kohlstedt, H. | |
| dc.creator | Buzdin, A. | |
| dc.creator | Goldobin, E. | |
| dc.creator | Koelle, D. | |
| dc.creator | Kleiner, R. | |
| dc.date | 2006-04-04 | |
| dc.date | 2006-08-24 | |
| dc.date.accessioned | 2026-07-07T07:05:16Z | |
| dc.date.available | 2026-07-07T07:05:16Z | |
| dc.description | We fabricated high quality $\Nb/\Al_2Ø_3/\Ni_{0.6}\Cu_{0.4}/\Nb$ superconductor-insulator-ferromagnet-superconductor Josephson tunnel junctions. Depending on the thickness of the ferromagnetic $\Ni_{0.6}\Cu_{0.4}$ layer and on the ambient temperature, the junctions were in the 0 or $π$ ground state. All junctions have homogeneous interfaces showing almost perfect Fraunhofer patterns. The $\Al_2Ø_3$ tunnel barrier allows to achieve rather low damping, which is desired for many experiments especially in the quantum domain. The McCumber parameter $β_c$ increases exponentially with decreasing temperature and reaches $β_c\approx700$ at $T=2.1 {\rm K}$. The critical current density in the $π$ state was up to $5\:\rm{A/cm^2}$ at $T=2.1 {\rm K}$, resulting in a Josephson penetration depth $λ_J$ as low as $160\:\rm{μm}$. Experimentally determined junction parameters are well described by theory taking into account spin-flip scattering in the $\Ni_{0.6}\Cu_{0.4}$ layer and different transparencies of the interfaces. | |
| dc.description | Changed content and Corrected typos | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0604097 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0604097 | |
| dc.identifier | Appl. Phys. Lett. 89, 122511 (2006) | |
| dc.identifier | doi:10.1063/1.2356104 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/109610 | |
| dc.subject | Superconductivity | |
| dc.title | High quality ferromagnetic 0 and pi Josephson tunnel junctions | |
| dc.type | text |