Fig. 4: ℓ0, Tc and kF.
From: Doping dependence of the dipolar correlation length scale in metallic SrTiO3

a Doping evolution of ℓ0=\(\frac{{v}_{TO}}{{\omega }_{TO}}\) for Nb-doped (blue points), La-doped (red points), reduced SrTiO3 (in green points estimated from ref. 30, see the text) and \(\frac{a}{2}\) (in gray dot line) where a = 3.9 Å is the lattice parameter of SrTiO3. b Doping evolution of the Fermi momentum (kF) in the three sub-bands i = 1,2 and 3. c Doping evolution of the superconducting critical temperature (Tc) according to11,12,46. The gray areas in (a, c) mark the end of the superconducting dome concomitant with the saturation of ℓ0 to about \(\frac{a}{2}\). d \({k}_{F}^{i}{\ell }_{0}\)vs.n for each sub-band. e Comparison of the carrier dependence of ℓ0 and Tc in linear scale. f Sketch of the electron doping evolution of 2ℓ0 (blue disk) and 2kF (black dot arrows). With electron doping ℓ0 decreases and saturates to about \(\frac{a}{2}\), the Ti-O distance, while kF increases. The summit of the superconducting dome occurs when \({k}_{F}^{3}{\ell }_{0}\) is the largest, see the text. Error bars on Tc are from11,12,46.