| Molybdenum disulfide(MoS2),a typical transition-metal dichalcogenide(TMD),has attracted extensive interest in recent years due to its unique physical properties and wide applications in electronic transistors,optoelectronic devices,and sensors.Combined with the excellent electronic and optical properties of intrinsic monolayer MoS2,the realization of tunable magnetic properties in monolayer MoS2 is important for expanding the application in spintronic devices,and magneto-optical nanodevices,etc.Therefore,the exploration of experimentally feasible magnetic modulation of monolayer MoS2 has attracted great attention.At present,monolayer MoS2 can be successfully fabricated by various experi-mental methods,such as mechanical exfoliation,molecular beam epitaxy,and vapor deposition.However,there are different density vacancies(VS)on the monolayer MoS2 surface,which provide the opportunity to induce localized magnetism by dop-ing in MoS2.The experimental progress of MoS2 based van der Waals heterojunctions also provides the possibility to realize long-range ordered magnetism.In this work,we have studied the tunable magnetic properties of monolayer MoS2 by doping and by van der Waals vertical heterojunction using first-priciples calculations.Our main works are listed as follows:(1)Tunable magnetic properties of monolayer MoS2 by doping.Firstly,magntic properties of monolayer MoS2 doped with light atoms of IIIA,IVA and VA have been studied.The results show that Al-,N-,P-atoms doping can induce magnetic moments in intrinsic materials,while Si-,Ge-,and As-atoms doped monolayer MoS2 systems are non-magnetic.Moreover,the magnetic moments can be switched on and off in the range of strain from-12%to 10%.Secondly,we have studied the electronic properties of monolayer MoS2 doped with gas molecules CO,NO,H2O,O2,N2,NH3,and CH4and it is found that NO and N2 doping can induce magnetic moments in MoS2.Meanwhile,all gas molecules doped systems can realize the light absorption in the infrared region.These results indicate that doping can tune the magnetic properties of monolayer MoS2 effectively,which is helpful for the fabrication of low dimensional spin devices and magnetic switches.(2)Tunable magnetic properties of monolayer MoS2 by co-doping.Firstly,we have studied Ge(Si)-As co-doping effects in MoS2.The results shown that Ge(Si)-As co-doping can induce magnetism in monolayer MoS2,and the magnetic moment gradually disappears with the increase of the co-doping diatomic distance.And we found that the magnetic property is dependent on the interaction between the co-doped atoms.The magnetic moment decreases from 1μB to 0μB gradually as the distance between the co-doped atoms increases due to the weakening of defect-defect interaction.Secondly,Si-X co-doping causes the polarization charge of the system to transfer from the vicinity of X atom to Si atom.The results show that the interaction between Si-X weakens the orbital hybridization of X atom and the intrinsic material,and enhances the hybridization strength of the Si atom’s spin-splitting state around the Fermi level.Moreover,the biaxial strain causes the phenomenon of magnetic moment transition in the Si-X co-doped system due to the interaction between defects.Our studies not only prove that co-doping is an effective means for magnetic regulation,but also discover a new mechanism for modulating magnetic properties by the de-fect-defect interaction.(3)Non-local magnetic regulation of g-C4N3/MoS2 vertical heterojunction by electric field.The results show that g-C4N3/MoS2 is semi-metallic,and the magnetism is mainly concentrated in the g-C4N3 layer.When a positive vertical electric field is applied to g-C4N3/MoS2,the layer spacing decreases with the increase of the forward electric field.At the same time,under the action of light excitation,the g-C4N3 layer and MoS2 layer have the non-local electron transition in the spin up(spin down)channel,which realizes the new phenomenon of spin separation in g-C4N3/MoS2 het-erojunction,and then realizes the non-local magnetic regulation in monolayer MoS2. |