Figure - available from: Journal of Superconductivity and Novel Magnetism
This content is subject to copyright. Terms and conditions apply.
![(a) R(T,B=0T)R0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\frac{R(T, B = 0 T)}{R_0}$$\end{document} curves recorded for zero-field case [Cu spacer thickness (dCu\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{Cu}$$\end{document}) = 0 (orange); 2.5 (green) and 5.0 nm (black)] and (b) the behavior of TC\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$T_\mathrm{C}$$\end{document} of the 20-nm-thick Nb film as a function of dCu\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{Cu}$$\end{document} in hybrid Nb/Cu(dCu\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{Cu}$$\end{document})/Py/Cu/Co. The full line in (b) is result of a fit with linear function, also shown](publication/355216380/figure/fig3/AS:1079041775931430@1634275015675/a-RT-B0TR0documentclass12ptminimal-usepackageamsmath-usepackagewasysym.png)
(a) R(T,B=0T)R0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\frac{R(T, B = 0 T)}{R_0}$$\end{document} curves recorded for zero-field case [Cu spacer thickness (dCu\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{Cu}$$\end{document}) = 0 (orange); 2.5 (green) and 5.0 nm (black)] and (b) the behavior of TC\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$T_\mathrm{C}$$\end{document} of the 20-nm-thick Nb film as a function of dCu\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{Cu}$$\end{document} in hybrid Nb/Cu(dCu\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{Cu}$$\end{document})/Py/Cu/Co. The full line in (b) is result of a fit with linear function, also shown
Source publication
![(a) R(T,B=0T)R0\documentclass[12pt]{minimal} \usepackage{amsmath}...](publication/355216380/figure/fig3/AS:1079041775931430@1634275015675/a-RT-B0TR0documentclass12ptminimal-usepackageamsmath-usepackagewasysym_Q320.jpg)
![M(B) loops recorded for the B⊥\documentclass[12pt]{minimal}...](publication/355216380/figure/fig4/AS:1079041775927322@1634275015750/MB-loops-recorded-for-the-Bdocumentclass12ptminimal-usepackageamsmath_Q320.jpg)
Hybrid Nb(20)/Cu(5)/Py(2), Nb(20)/Cu(5)/Co(40) and Nb(20)/Cu(d\(_{Cu}\))/Py(2)/Cu(5)/Co(40) heterostructures (values in nanometers and d\(_{Cu}\) = 0, 2.5 and 5.0) were fabricated using a confocal DC magnetron sputtering setup. Performing magnetotransport measurements and using the anisotropic Ginzburg–Landau approach, the stray field values in zer...
Similar publications
The investigation of two-dimensional atomically thin superconductors—especially those hosting topological states—attracts growing interest in condensed-matter physics. Here we report the observation of spin–orbit–parity coupled superconducting state in centrosymmetric atomically thin 2M-WS2, a material that has been predicted to exhibit topological...
