Figure 2 shows ρ(T) from 300 K down to 1.8 K. The compound behaves metallically (dρ/dT > 0) above 80 K with a residual‑resistivity ratio (RRR = ρ(300 K)/ρ(4 K)) ≈ 12, indicating high crystal quality. A sharp superconducting transition occurs at T_c = 44.2 K (ΔT_c ≈ 0.3 K). Application of magnetic fields up to 9 T suppresses T_c progressively, yielding an upper critical field μ₀H_c2(0) ≈ 23 T (extrapolated using the Werthamer–Helfand–Hohenberg model).
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