TY - JOUR
T1 - Electronic and magnetic properties of 4d series transition metal substituted graphene
T2 - A first-principles study
AU - Sun, Minglei
AU - Ren, Qingqiang
AU - Zhao, Yiming
AU - Chou, Jyh Pin
AU - Yu, Jin
AU - Tang, Wencheng
N1 - Publisher Copyright:
© 2017 Elsevier Ltd
PY - 2017/8
Y1 - 2017/8
N2 - We implement a theoretical study of the geometry parameters, binding energies, electronic and magnetic properties of 4d series transition metals substituted graphene. Based on a hybridization model, the variations of binding energies and magnetic moments size can be well understood. According to the occupation of different vacancy-metal hybridized electronic states, the substituted systems can be divided into three types: (i) for Y and Zr, all the bonding states are completely occupied, and the magnetic moment is zero; (ii) for Nb, Mo and Tc, nonbonding states become occupied, which induce a strong localized magnetic moment with d character of 1 μB, 2 μB and 1 μB, respectively; (iii) for Ru, Rh and Pd, the magnetic moment oscillates between 0 and 1 μB as the antibonding state become occupied. In addition, we found that the Y- and Rh-substituted graphene exhibit metallic behavior, and the semiconducting natures were found in Zr-, Ru- and Pd-substituted systems. More interestingly, half-metallic state were predicted in Nb- and Tc-substituted graphene, while spin-polarized semiconducting state is realized in Mo-substituted system. The Curie temperature of about 83, 354 and 36 K was estimated for Nb-, Mo- and Tc-substituted systems in the mean-field approximation at impurity concentration 3.125%.
AB - We implement a theoretical study of the geometry parameters, binding energies, electronic and magnetic properties of 4d series transition metals substituted graphene. Based on a hybridization model, the variations of binding energies and magnetic moments size can be well understood. According to the occupation of different vacancy-metal hybridized electronic states, the substituted systems can be divided into three types: (i) for Y and Zr, all the bonding states are completely occupied, and the magnetic moment is zero; (ii) for Nb, Mo and Tc, nonbonding states become occupied, which induce a strong localized magnetic moment with d character of 1 μB, 2 μB and 1 μB, respectively; (iii) for Ru, Rh and Pd, the magnetic moment oscillates between 0 and 1 μB as the antibonding state become occupied. In addition, we found that the Y- and Rh-substituted graphene exhibit metallic behavior, and the semiconducting natures were found in Zr-, Ru- and Pd-substituted systems. More interestingly, half-metallic state were predicted in Nb- and Tc-substituted graphene, while spin-polarized semiconducting state is realized in Mo-substituted system. The Curie temperature of about 83, 354 and 36 K was estimated for Nb-, Mo- and Tc-substituted systems in the mean-field approximation at impurity concentration 3.125%.
UR - http://www.scopus.com/inward/record.url?scp=85019490481&partnerID=8YFLogxK
U2 - 10.1016/j.carbon.2017.04.060
DO - 10.1016/j.carbon.2017.04.060
M3 - Article
AN - SCOPUS:85019490481
SN - 0008-6223
VL - 120
SP - 265
EP - 273
JO - Carbon
JF - Carbon
ER -