Using Blonder-Tinkham-Klapwijk (BTK) formalism we studied the transport properties in silicene-based normal/ferromagnetic p-wave superconductor (N/FpS) junctions. Our study shows that the amplitude of the normalized conductance strongly depends on the pairing symmetry in superconductor such as p_x, p_y and p_x+ip_y-wave symmetries, the applied electric field (E_Z) and the exchange field (h) in FpS. In N/Fp_xS-silicene junctions the zero-bias conductance peak is obtained due to the Andreev bound states. When the electric field and magnetic field are parallel, called P configuration, there is one conductance dip (CD) for the voltage $eV=lEz-{\lambda }_{SO}$ with λ_SO the spin obit coupling term and 2l the distance between two sublattices in the buckled silicene. In the anti-parallel (AP) configuration there is one CD at $eV=lEz-{\lambda }_{SO}$ for $0<lEz-{\lambda }_{SO}<h$ and for $lEz-{\lambda }_{SO}\ge h$ there are two CDs at $eV=h$ and $eV=lEz-{\lambda }_{SO}$, respectively. A sudden transition of conductance from zero to maximum (henceforth referred to as“switching of conductance”) at $eV=lEz-{\lambda }_{SO}$ occurs in both N/Fp_yS-silicene junction and N/Fp_x+ip_yS-silicene junction. In N/Fp_yS-silicene junction the Andreev resonant peak appears at $eV=h$ for $l{E}_z-{\lambda }_{SO}-h=0.1{\Delta }_{00}$ in the AP case, where Δ₀₀ is the zero temperature gap of the FpS. In N/Fp_x+ip_yS-silicene junctions the maximum value of the conductance appears at $eV={\Delta }_{00}-h$ in P junction while in AP junction at $eV={\Delta }_{00}+h$.

使用Blonder-Tinkham-Klapwijk（BTK）形式主义，我们研究了硅基正/铁磁p波超导体（N / F p S）结中的传输性质。我们的研究表明，归一化电导的幅度很大程度上取决于超导体中的配对对称性，例如p _x，p _y和p _x + i p _y波对称性，施加电场（E _Z）和交换场（h）在F p S中。在N / F p _x中由于Andreev键合态，获得了S-硅结的零偏置电导峰。当电场和磁场平行时，称为P配置，电压有一个电导降（CD）$ËV=升Ëž-{\lambda }_{\mathrm{小号}Ø}$与λ _SO自旋讣告耦合项和2升在扣住硅烯两类子晶格之间的距离。在反并行（AP）配置中，一张CD位于$ËV=升Ëž-{\lambda }_{\mathrm{小号}Ø}$ 对于 $0<升Ëž-{\lambda }_{\mathrm{小号}Ø}<H$ 和为 $升Ëž-{\lambda }_{\mathrm{小号}Ø}\ge H$ 有两张CD $ËV=H$ 和 $ËV=升Ëž-{\lambda }_{\mathrm{小号}Ø}$， 分别。电导突然从零变到最大值（以下称为“电导转换”）$ËV=升Ëž-{\lambda }_{\mathrm{小号}Ø}$在N / F p _y S-硅结和N / F p _x + ip _y S-硅结中都出现。在N / F p _y S-硅结中，Andreev共振峰出现在$ËV=H$ 对于 $升{Ë}_{ž}-{\lambda }_{\mathrm{小号}Ø}-H=0.1{\Delta }_{00}$在AP的情况下，其中Δ ₀₀是F的零温度间隙p S.于N / F p _X + IP _ý S-硅烯结的最大电导出现的值$ËV={\Delta }_{00}-H$ 在P结处，而在AP结处 $ËV={\Delta }_{00}+H$。