Electrons repel — yet just below Tc they quietly pair through the lattice and condense into one frictionless quantum state. The Fermi sea is unstable to any attraction; a gap 2Δ opens, and the critical temperature is exponentially small in the coupling. Rendered, not quoted.
source Bardeen, Cooper & Schrieffer, “Theory of Superconductivity,” Phys. Rev. 108, 1175 (1957) — doi:10.1103/PhysRev.108.1175
Two electrons added above a filled Fermi sea, with a weak phonon-mediated attraction acting only within a Debye shell ±ħωD of EF.
Cooper binding: Eb = 2ħωD·e−2/N₀V — nonzero for any N₀V>0.
Gap & Tc: Δ(0)=2ħωDe−1/N₀V, kBTc=1.134ħωDe−1/N₀V.
Cooper pairs from a phonon attraction, a gap 2Δ=3.53 kBTc, an isotope effect Tc∝M−½.
This is the microscopic engine behind the-meissner-effect — the condensate that expels B is exactly this paired ground state. Neighbour sphere in THE FOLD.
Live re-check of the engine. Confirms the untampered laws; flips red the instant the gap is voided.
witness idleCoupling N₀V, Debye temperature ΘD, ionic mass M. Constants: e, kB, me, ħ.
The proven result of the run:
booting…Superconductivity is a perfect classical conductor (σ→∞ only).
→ It is a distinct thermodynamic phase that expels field (Meissner); a perfect conductor would merely freeze flux in.
The gap is a fixed material constant.
→ Δ(T) collapses to 0 at Tc; only the ratio 2Δ(0)/kBTc≈3.53 is universal.
Isotope mass is irrelevant to an electronic effect.
→ Tc∝M−½ — the phonon fingerprint that proved the lattice mediates the pairing.
Planted void: force the gap to zero (2Δ=0), so pairing yields no gap and the 3.53 ratio dies. The Witness (7) catches it live.