in two dimensions in [@zwicknagl_critical_2017].

The Zeeman field-temperature phase diagrams have been obtained numerically using the self-consistency relations for arbitrary strength of the spin-orbit coupling. These phase diagrams exhibit anisotropy effects related to the angle between the Zeeman field and the wire axis. We have plotted the phase diagram in the case of strong spin-orbit coupling for different orientations of the Zeeman field and several values of the spin-orbit constant, and highlighted the anisotropy caused by SOC. At last we have shown that increasing $\alpha$ and the ratio $h_x/h_z$ allows superconductivity at larger temperature.

Finally, the results above also pertain for the case of quasi-one dimensional organic superconductors consisting in weakly coupled one-dimensional chains, although the spin-orbit should be due to the bulk structure of the crystal instead of the surface Rashba coupling.

Some perspectives result from this work. Because of its sensitivity to impurities [@azlamazov_influence_1969], it has been extremely difficult to observe experimentally the FFLO state. However, spin-orbit interaction should be sufficient to protect the modulated phase [@michaeli_superconducting_2012]. Thus one could emphasize that the nonuniform phase would be directly observable in an experimental system made of a superconductor coupled to a ferromagnet with strong spin-orbit interaction.

Our model may 