pith. sign in

(S15) This leads to the actions iSψ =i Z p,ε ¯Ψ(p, ε)G−1 0 (p, ε)Ψ(p, ε), iSϕ =i Z q,ω ¯ϕ(q, ω)D−1 0 (q, ω)ϕ(q, ω), iSint =−ig Z p,ε,q,ω ¯Ψ(p+q, ε+ω)Φ(q, ω)Ψ(p, ε)

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Tunable viscosity across the BCS-BEC crossover

cond-mat.quant-gas · 2026-04-12 · unverdicted · novelty 5.0

Shear viscosity in ultracold Fermi gases varies by orders of magnitude near the BCS-BEC crossover, enabling tunable high-Reynolds-number flows.

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  • Tunable viscosity across the BCS-BEC crossover cond-mat.quant-gas · 2026-04-12 · unverdicted · none · ref 29

    Shear viscosity in ultracold Fermi gases varies by orders of magnitude near the BCS-BEC crossover, enabling tunable high-Reynolds-number flows.