DOI: 10.31274/rtd-180813-2251
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The superconducting properties of high purity niobium

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Cited by 2 publications
(3 citation statements)
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“…1 where this length scale was determined from the direct EM imaging, providing further evidence of the importance of the film morphology in determining the magnetic response. Overall, our films show a much larger magnetic hysteresis compared to the bulk samples and single crystals [36,43]. However, a very large demagnetizing factor and thin-film geometry play a significant role in diminishing the interval and the magnitude of the reversible magnetic moment, which is proportional to a very small film volume, whereas irreversible Bean currents flow in the entire sample [44][45][46][47][48].…”
Section: Resultsmentioning
confidence: 82%
“…1 where this length scale was determined from the direct EM imaging, providing further evidence of the importance of the film morphology in determining the magnetic response. Overall, our films show a much larger magnetic hysteresis compared to the bulk samples and single crystals [36,43]. However, a very large demagnetizing factor and thin-film geometry play a significant role in diminishing the interval and the magnitude of the reversible magnetic moment, which is proportional to a very small film volume, whereas irreversible Bean currents flow in the entire sample [44][45][46][47][48].…”
Section: Resultsmentioning
confidence: 82%
“…2(c)], without breaking the reservoir's own superconductivity. Our choice, Niobium, as the large gap superconductor has a higher critical field (B 0 ∼ 0.82 T) compared to Tantalum (B 0 ∼ 0.08 T) [11][12][13]. Therefore Niobium can sustain the supercurrent that produce the magnetizing B field without breaking its own superconductivity.…”
Section: (B)mentioning
confidence: 97%
“…Niobium is also type II, and therefore it can enter a mixed state with normal vortices. It is still acceptable as the lower critical field above which Niobium enters a mixed state has been measured around 0.19 T [12,13], which is still higher than the critical field of Tantalum. We also assume that the Kapitza coupling [14][15][16] across the tunnel junctions can be avoided by carefully choosing the disordered tunnel barriers such that it causes phonon mismatch, and prevents phonon mediated heat transport.…”
Section: (B)mentioning
confidence: 98%