Abstract
In recent years thin Nb3Sn coatings have shown quite promising results for rf applications in the superconducting state [1–6]. These layers were grown in carefully prepared pure niobium rf cavities by heating them in a saturated tin vapor at a temperature of 1050°C for several hours. This procedure results in coatings several microns thick, consisting of Nb3Sn single crystal columns about 1 µm in diameter [3–5]
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Abbreviations
- B c :
-
thermodynamic critical field
- B c2 :
-
upper critical field
- B DC :
-
stationary magnetic field
- B crit :
-
rf critical magnetic field
- E p :
-
peak electric field at the cavity surface
- ƒ:
-
frequency
- F p :
-
volume pinning force
- j c :
-
critical current density
- k:
-
Boltzmann constant
- l:
-
mean free path
- R(T):
-
measured surface resistance
- R BCS :
-
surface resistance, as described by the BCS theory
- R res :
-
residual surface resistance
- T c :
-
transition temperature
- 2Δ:
-
energy gap
- Δb :
-
screening field
- λl :
-
London penetration depth
- ξgl :
-
Ginzburg-Landau coherence length
- ξ0 :
-
BCS coherence length
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Kneisel, P., Küpfer, H., Stoltz, O., Halbritter, J. (1978). Properties of Superconducting Nb3Sn Layers Used in RF Cavities. In: Timmerhaus, K.D., Reed, R.P., Clark, A.F. (eds) Advances in Cryogenic Engineering. Advances in Cryogenic Engineering, vol 24. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-9853-0_49
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