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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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stoichiometric composition is metastable at room temperature and is only stable at1940°C. The aluminium content <strong>of</strong> the A15 phase decreases with decreasingtemperature; the homogeneity range at 1000°C is 19~22 at.% Al.Nb 3 GeThe most striking feature <strong>of</strong> Nb 3 Ge phase field is that the stoichiometriccomposition is not included at equilibrium, the highest solubility <strong>of</strong> Germaniumbeing 23 at.%. At 1000°C, the homogeneity range <strong>of</strong> the A15 phase is very narrowand is centered at 18 at.% with total width <strong>of</strong> 1 at.%. It has not been possible torise T C above 17~18 K in bulk sample either by quenching or other means.Metastable stoichiometric, or near stoichiometric, Nb 3 Ge can be prepared as thinfilms with critical temperature <strong>of</strong> 23 K. But the big problem is that the material isvery brittle, which meaning is that a strike or vibration can change the A15structure and cease the superconductor.Nb 3 SnNb 3 Sn is the only A15 material that has given promising results when appliedto the construction <strong>of</strong> a real cavity [19] : Tin was reactively diffused into an Nb bulkcavity and the Q-factor was in the order <strong>of</strong> 10 11 , the accelerating field beinglimited to about 12 MV/m.Fig.1.7The Niobium-Tin phase diagramAccording the phase diagram <strong>of</strong> Fig. 1.7, the A15 phase is unstable below14

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