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Using first-principles total energy method,we study the structural,the electronic and the magnetic properties of the MnNi(110) c(2×2) surface alloy.Paramagnetic,ferromagnetic,and antiferromagnetic surfaces in the top layer and the second layer are considered.It turns out that the substitutional alloy in the outermost layer with ferromagnetic surface is the most stable in all cases.The buckling of the Mn-Ni(110) c(2×2) surface alloy in the top layer is as large as 0.26 A(1 A=0.1 nm) and the weak rippling is 0.038 A in the third layer,in excellent agreement with experimental results.It is proved that the magnetism of Mn can stabilize this surface alloy.Electronic structures show a large magnetic splitting for the Mn atom,which is slightly higher than that of Mn-Ni(100) c(2×2) surface alloy(3.41 eV) due to the higher magnetic moment.A large magnetic moment for the Mn atom is predicted to be 3.81μB.We suggest the ferromagnetic order of the Mn moments and the ferromagnetic coupling to the Ni substrate,which confirms the experimental results.The magnetism of Mn is identified as the driving force of the large buckling and the work-function change.The comparison with the other magnetic surface alloys is also presented and some trends are predicted.
Using first-principles total energy method, we study the structural, the electronic and the magnetic properties of the MnNi (110) c (2x2) surface alloy. Paramagnetic, ferromagnetic, and antiferromagnetic surfaces in the top layer and the second layer are considered. Turns out that the substitutional alloy in the outermost layer with ferromagnetic surface is the most stable in all cases. Buckling of the Mn-Ni (110) c (2x2) surface alloy in the top layer is as large as 0.26 A (1 A = 0.1 nm) and the weak rippling is 0.038 A in the third layer, in excellent agreement with experimental results. It is proved that the magnetism of Mn can stabilize this surface alloy. Electronic structures show a large magnetic splitting for the Mn atom, which is slightly higher than that of Mn-Ni (100) c (2 × 2) surface alloy (3.41 eV) due to the higher magnetic moment. A large magnetic moment for the Mn atom is predicted to be 3.81 μB .We suggest the ferromagnetic order of the Mn moments and the ferromagnetic coupling to t he Ni substrate, which confirms the experimental results. the magnetism of Mn is identified as the driving force of the large buckling and the work-function change. the comparison with the other magnetic surface alloys is also presented and some trends are predicted.