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Magnetron sputtering of Superconducting Multilayer Nb3Sn Thin Film

Magnetron sputtering of Superconducting Multilayer Nb3Sn Thin Film

Magnetron sputtering of Superconducting Multilayer Nb3Sn Thin Film

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Table 3.7 the description <strong>of</strong> the peaks <strong>of</strong> Run s50.52940.5292<strong>Nb3Sn</strong>thoerycubic edge length (nm)0.52900.52880.52860.52841.0 1.2 1.4 1.6 1.8current (A)Fig.3.25 the cubic edge length versus Nb <strong>sputtering</strong> currentUsing the same method <strong>of</strong> 2.3.3.3 section, we can obtain the cubic edge length <strong>of</strong>each sample. According to Fig.3.25, the cubic edge length increases with the Nb<strong>sputtering</strong> current increasing, except the point <strong>of</strong> 1.4A.3.3 Deposition on Nb sampleIf we fabricate the accelerator cavity with thin film, the thin film should bedeposited on substrate, which including the Nb and copper. The advantage <strong>of</strong> the Nbsubstrate is that Nb is superconductor, which means that when the part zone <strong>of</strong> thethin film is not the superconductor, the Nb is still the superconductor which make sure<strong>of</strong> that the whole accelerator cavity is superconductor. But the disadvantage is that thethermal conductor <strong>of</strong> the Nb is poor. The advantage <strong>of</strong> the copper substrate is that thethermal conductor and the mechanical property are very good. The good thermalconductor can quickly transfer the heat produced by the microwave in the thin film,which can reduce the thermal unstable <strong>of</strong> the superconductor because that if the heatcan not transfer in time, the temperature <strong>of</strong> some zone <strong>of</strong> the thin film will increaseand higher than T c . The good mechanical property can reduce the detuning <strong>of</strong> the54

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