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Figure 1. Schematic diagram of the MgB2 Josephson junction fabrication process before He-FIB irradiation, including thin films growth, sputtering Ag electrical bonding pads, lithography, and etching.
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Figure 2. (a) Schematic diagram of a MgB2 Josephson junction fabricated by He-FIB. (b) Optical microscope photograph under bottom light where black line indicates irradiation trace. (c) R–T curves of junctions 1 and 2, where the inset is a close-up view. (d) V–I curves of junctions 1 and 2 at 2 K, where the inset shows the dV/dI–I curves.
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Figure 3. (a) and (c) The I–V curves and dV/dI–V curves of junctions 1 and 2 under magnetic field and RF radiation at 2 K where clear integer and half-integer Shapiro steps can be observed. The positions of steps are labeled by vertical lines and the corresponding normalized voltages n represent the orders of steps. (b) and (d) The vertically shifted dV/dI–V curves of junctions 1 and 2 under different frequencies of RF radiation. The voltages corresponding to the steps rise with the increase of frequency.
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Figure 4. (a) and (c) Selected I–V curves of junctions 1 and 2 under fixed RF radiation power and magnetic field at different temperatures. (b) and (d) Heatmaps of junctions 1 and 2’s I–dV/dI curves at different temperatures. The white areas indicate integer and half-integer Shapiro steps, which are labeled by red dashed lines.
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Figure 5. (a) and (c) The I–V curves of junction 1 under different RF radiation powers at magnetic fields of 27 Oe and 31.5 Oe. Half-integer steps only appear at the magnetic field of 27 Oe. (b) and (d) Heatmaps of I–dV/dI curves whose data is collected from (a) and (c), where red dashed lines label the evolution of step heights with radiation power and oscillations can be observed.
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Figure 6. (a) Colormap of V–dV/dI curves under radiation at different magnetic fields H, where blue areas indicate the appearance of steps. Half-integer steps are labeled by horizontal black dashed lines. (b) The critical current Ic that is modulated by magnetic field H for the positive and negative current directions. The data is also collected from junction 1.
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Figure 7. (a) Schematic diagram of a YBCO grain boundary junction which is composed of many superconducting and normal fragments and is actually a 1D junction array. (b) The irradiation mode of He-FIB, which is spot-by-spot, inducing many areas with different irradiation doses.
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