Figure 3. Possible pseudogap formation below T* evidenced by NMR and transport measurements.

(a) Temperature dependence of the NMR relaxation rate divided by temperature 1/T₁T. Inset: at 14.5 T, the temperature dependence of 1/T₁T between ∼10 and 70 K is fitted to a Curie–Weiss law ∝(T+16 K)⁻¹ (dashed line). Main panel: the difference between the Curie–Weiss fit and the low-field data Δ(1/T₁T) is plotted as a function of temperature. (b) Hall coefficient, R_H. (c) Seebeck coefficient, S. (d) Nernst coefficient, ν, in the zero-field limit as functions of temperature. Inset in d is a schematic of the measurement set-up of the thermoelectric coefficients.