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Aug 22, 2022 at 18:00 history edited Stanislav Dolgopolov CC BY-SA 4.0
the thermal distributions at low Tc are rather quantized than smooth, so thermal excitations are rather a few kT than much larger values.
Aug 22, 2022 at 17:42 history edited Stanislav Dolgopolov CC BY-SA 4.0
Answer to point 2 (couldn't some of the 'high' energy particles destroy the superconductivity briefly locally ?)
Aug 17, 2022 at 5:48 comment added Stanislav Dolgopolov Very good question. Indeed, there are two (thermal) energies: one splits the pair (say kT*), the second one breaks the Bose-Einstein-Condensation (say kTbec). In metals, usually, T*<Tbec, so the energy kT* splits the pairs at Tbec and there is no any BEC above T*. Above T* the pairs recombinate very fast, so the state is not a bosonic liquid, but rather a Fermi sea of free electrons. Thus, in superconducting metals kT* is the energy quant, breaking the supercurrent due to boson breaking.
Aug 16, 2022 at 18:52 comment added jp314 but there is still thermal energy in the system (with a distribution) -- so can that occasionally split a pair ? would it recover ?
Aug 16, 2022 at 16:50 history edited Stanislav Dolgopolov CC BY-SA 4.0
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Aug 16, 2022 at 16:48 history answered Stanislav Dolgopolov CC BY-SA 4.0