Fig. 3: Diode effect in a long Dayem bridge. | Communications Physics

Fig. 3: Diode effect in a long Dayem bridge.

From: Sign reversal diode effect in superconducting Dayem nanobridges

Fig. 3

a Magnetic field dependence of the switching current for positive \({I}_{sw}^{+}\)(green dots) and negative \(| {I}_{sw}^{-}|\)(orange dots) bias current recorded at 50 mK. b ΔIsw obtained from panel a. The rectification efficiency increases linearly in Bz until Bz 015 T. Red and black dashed lines mark the magnetic field values corresponding to sign reversal (BR) and maximum rectification (Bmax), respectively. Inset: Blow-up of ΔIsw for large positive (black) and negative (brown) fields displaying several changes of signs. c IV characteristics with negative \({I}_{sw}^{+} < | {I}_{sw}^{-}|\) and positive \({I}_{sw}^{+} > | {I}_{sw}^{-}|\) rectification recorded at the magnetic fields marked by bars in panel a. d Color plot of the rectification efficiency as a function of temperature and magnetic field, η(Bz, T). Dashed lines are guides for the eye to highlight the different temperature trends in Bmax and BR. e Rectification parameters: ηmax ≡ (ηmax(Bz > 0) + ηmax(Bz < 0))/2 (green dots), field-to-rectification efficiency transfer function Γ (blue dots) (i), Bmax (red dots) and BR (black dots) magnetic fields (ii) versus normalized temperature. \({T}_{c}^{L}\) denotes the critical temperature of the long bridge. ηmax is the rectification value of the low-field peak at Bmax. f \({\eta }_{{B}_{z}}\) for selected bath temperatures marked by dashed lines in panel d. Curves are vertically offset for clarity.

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