Type I vs Type II Superconductors
How the ratio κ = λL / ξ determines whether flux is excluded or penetrates as quantized vortices
κ = λL / ξ 0.50 Type I
κ = 0.1 ← Type I · Type II → κ = 2.0
Length Scale Cross-Section
Surface λL ξ Bext
Complete Flux Exclusion
B = 0 Complete Meissner effect Single critical field Hc
Screening currents / λL
Counter-rotating vortex / ξ
External magnetic flux
Superconducting bulk
Why This Type
ξ > λL — The pair vortex is spatially larger than the screening depth. A flux line would need to penetrate a region smaller than the pair to enter — but doing so would rupture the vortex, destroying the pair. The condensate excludes all flux until the field overwhelms it at a single critical field Hc.
Examples
Type I: Pb (κ ≈ 0.48), Hg (κ ≈ 0.15), Sn (κ ≈ 0.15), Al (κ ≈ 0.01)

Type II: Nb (κ ≈ 1.1), NbTi (κ ≈ 60), YBCO (κ ≈ 95)