Fig. 4: Orbital and energy selective enhancement of EPC in Cs(V0.93Nb0.07)3Sb5.
From: Testing electron–phonon coupling for the superconductivity in kagome metal CsV3Sb5

a Temperature dependence of magnetic susceptibility for pristine CsV3Sb5 and Cs(V0.93Nb0.07)3Sb5. Both zero-field cooling (ZFC) and field cooling (FC) curves are presented. b ARPES intensity plots of the α and β bands along the Γ−Κ direction for Cs(V0.93Nb0.07)3Sb5. The false color is adjusted for better visualization. c Extracted band dispersions for the α and β bands shown in (b). The black lines are the corresponding bare bands. d Extracted ReΣ(ω) for the α (top panel) and β (bottom panel) bands. The error bars for ReΣ(ω) are determined from the standard deviation of the MDC fits, which is converted to energy by multiplying the velocity of the bare band. The ReΣ(ω) of pristine CsV3Sb5 is plotted as colored shadows for a direct comparison. The solid black curves are the reproduced ReΣ(ω) via maximum entropy method. The dashed blue and gray line represents the slope of the ReΣ(ω) at EF in Cs(V0.93Nb0.07)3Sb5 and CsV3Sb5, respectively. e Extracted Eliashberg function α2F(ω). f EPC strength λ estimated from the α2F(ω), which is plotted as a function of Tc. The error bar for λ is determined by the standard deviation of the ReΣ(ω).