The Josephson diode effect (JDE) is a novel phenomenon in which a superconducting junction exhibits asymmetric Josephson currents with respect to the superconducting phase difference. In this study, we theoretically investigate how the interplay between a static exchange field and Rashba spin-orbit interaction (RSOI) influences the JDE. By employing the quasiclassical Green’s function method and perturbative calculations, we derive analytical expressions for the Josephson current in a junction composed of a ferromagnetic layer and a normal metal with RSOI. Remarkably, the JDE is found to emerge even in the absence of any external magnetic field. In this regime, the Josephson current is exclusively carried by spin-triplet Cooper pairs, as spin-singlet components are strongly suppressed by the ferromagnet. Furthermore, our results show that the efficiency of the JDE can be enhanced by tuning the thickness of the normal metal and the strength of the RSOI. These findings offer valuable theoretical guidelines for the design of superconducting devices exhibiting nonreciprocal transport effects.

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