Electromagnetic and plasma properties across the RFs along the X direction. Left column shows the results from the asymmetric reconnection at time ﹩t=90{{\rm{\Omega }}}_{{ci}}^{-1}﹩, while the right column is for the symmetric reconnection at ﹩t=53{{\rm{\Omega }}}_{{ci}}^{-1}﹩. From the top to the bottom are ((a)–(b)) magnetic field B_z; ((c)–(d)) plasma density N_i; ((e)–(f)) current density J_y (black), J_iy (red), and J_ey (blue); ((g)–(h)) energy conversion ﹩{\boldsymbol{J}}\cdot {\boldsymbol{E}}﹩ (black), ﹩{{\boldsymbol{J}}}_{{\boldsymbol{i}}}\cdot {\boldsymbol{E}}﹩ (red), and ﹩{{\boldsymbol{J}}}_{{\boldsymbol{e}}}\cdot {\boldsymbol{E}}﹩ (blue); ((i)–(j)) energy dissipation ﹩{\boldsymbol{J}}\cdot {{\boldsymbol{E}}}_{{\boldsymbol{i}}}^{{\prime} }﹩; ((k)–(l)) ion bulk velocity v_ix and v_iy; ((m)–(n)) electron bulk velocity v_ex and v_ey; ((o)–(p)) ion temperatures; and ((q)–(r)) electron temperatures. The average ion temperature Ti_aver is equal to (Ti_para + 2Ti_perp)/3, and the average electron temperature Te_aver is equal to (Te_para + 2Te_perp)/3.