Crystal Structures And Sign Reversal Hall Resistivities In Iron-Based Superconductors Li-X(C3h10n2)(0.32)Fese (0.15 < X < 0.4)

Heavy electron-doped FeSe-derived materials have attracted attention due to their uncommon electronic structures with only 'electron pockets', and they are different from other iron-based superconductors. Here, we report the crystal structures, superconductivities and normal state properties of two new Li-doped FeSe-based materials, i.e., Li-0.15(C3H10N2)(0.32)FeSe (P-4) and Li-x (C3H10N2)(0.32)FeSe (P4/nmm, 0.25 < x < 0.4) with superconducting transition temperatures ranging from 40 K to 46 K. The determined crystal structures reveal a coupling between Li concentration and the orientation of 1,3-diaminopropane molecules within the largely expanded FeSe layers. Superconducting fluctuations appear in the resistivity of the two superconductors and are fitted in terms of the quasi two-dimensional (2D) Lawrence-Doniach model. The existence of a crossing point and scaling behavior in the T-dependence of diamagnetic response also suggests that the two superconductors belong to the quasi-2D system. Interestingly, with the increase of temperature, a sign of Hall coefficient (R-H) reversing from negative to positive is observed at similar to 185 K in both phases, suggesting that `hole pockets' emerge in these electron-doped FeSe materials. First principle calculations indicate that the increase in FeSe layer distance will lift up a 'hole band' associated with d(x2-y2) character and increase the hole carriers. Our findings suggest that the increase in two dimensionalities may lead to the sign-reversal Hall resistivity in Li-x(C3H10N2)(0.32)FeSe at high temperature.