The First Principle Study for Magnetic Properties of d0 Nano-materials
- Abstract
- It is common knowledge that the magnetism is originated from narrowing d-band in 3d transition metals. This can be accounted from band and Stoner's theory. Narrow d-band causes the high density of states at Fermi level and then, this leads the spontaneous spin polarized state in materials. For example, Fe, Ni, and Co have the ground state for ferromagnetic state. However, late transition metals, such as 4d and 5d metal, do not show ferromagnetic state. This can be well understood from Stoner's theory.
As mention above, one can observe magnetism only Fe, Ni, and Co in bulk structure, except 4f materials. However, many experimental researches have reported that pure oxide materials show magnetic signal in recent. HfO2 is the most representative material showing the magnetic state without any 3d transition metal dopant. Of course, magnetism can be observed in other pure oxide materials, such ZnO, TiO2, and CaO. The origin of pure oxide material is considered as cation vacancy defect, and many results have been reported. These phenomena also observed in surface state, and we have called this to d0 magnetism.
In this thesis, we have investigated the origin of d0 magnetism in 2p materials with nano-structure. We have used the art-of-state full potential linearized augmented plane wave (FLAPW) method. The d0 magnetism have two origin, atomic vacancy defect and surface effect.
In section 5.1 and 5.2, we have consider atomic defect in TiO2 and ZnO bulk systems. We have obtained that both TiO2 and ZnO show magnetic state with O and Zn atomic defect, respectively. Also, we can observe that the lattice distortion is very important factor, because both materials do not show magnetic state if we do not consider lattice distortion. From this, we can assume that the atomic vacancy defect causes lattice distortion and lattice distortion bring magnetism in TiO2 and ZnO.
To study the effect of surface, we have calculated MgO(001) surface in section 5.3. We observed that the Mg vacancy defect can induced a spin polarization in oxygen atoms around the Mg vacancy site whereas the O vacancy defect has no influence on the magnetic state. We have obtained that the total magnetic moment per unit cell increases as the Mg vacancy defect moves to the surface layer.
Previous studies show that vacancy defect induced magnetic state around O atom, and the p-orbital is essential role. Thus, other 2p materials, such C and N, can show magnetic signals. To proof this, we have calculated carbon doped ZnO in section 5.4. Also, Ultrathin N and C films on MgO(001) surface have been investigated in section 5.5. MgN and MgC films on MgO(001) surface show ferromagnetic and half metallic features. One can see the details in section 5.6.
In section 5.7 and 5.8, magnetic properties of 5d and 4d transition metal is calculated. In nature, 4d and 5d transition metal is nonmagnetic materials, but these materials can be induced magnetic state by forming nano-structure or surface (ultrathin films). We have find that ultrathin 4d and 5d metal on NiAl(001) surface have giant perpendicular magnetic anisotropy energy.
- Author(s)
- 김동유
- Issued Date
- 2012
- Awarded Date
- 2012. 8
- Type
- Dissertation
- Publisher
- 부경대학교
- URI
- https://repository.pknu.ac.kr:8443/handle/2021.oak/25114
http://pknu.dcollection.net/jsp/common/DcLoOrgPer.jsp?sItemId=000001964999
- Alternative Author(s)
- Dongyoo Kim
- Affiliation
- 부경대학교 대학원
- Department
- 대학원 물리학과
- Advisor
- 홍지상
- Table Of Contents
- 1.Introduction 1
2.Density Functional Theory 7
2.1.Born-Oppenheimer Approximation 7
2.2.Hartree-Fock Approximation 9
2.3.Hohenberg-Kohn and Kohn-Sham Equation (Density Functional Theory) 11
2.4.Spin Density Functional Theory 18
2.5.Approximations of The Exchange-correlation Term Exc 20
3.The FLAPW Method 24
3.1.Augmented Plane-wave Method 24
3.2.Linearized Augmented Plane-wave Method 26
3.3.The Full-potential LAPW Method 30
3.4.FLAPW Method for Film Calculation 31
4.Theory of Itinerant Electrons Magnetism 35
4.1.Band Theory for Ferromagnetism 36
4.2.Magnetic anisotropy energy 40
4.2.1.Origin of the magnetic anisotropy 41
4.2.2.Magnetic dipolar anisotropy (Shape Anisotropy) 42
4.2.3.Magnetocrystalline Anisotropy 43
4.2.4.Computational Method to Determine Magnetic Anisotropy 45
4.3.X-ray Magnetic Circular Dichroism (XMCD) 48
5.The Magnetic Properties of d0 Nanomaterials 50
5.1.The Origine of Oxygen Vacancy Induced Ferromagnetism in Undoped TiO2 50
5.1.1.Introduction 50
5.1.2.Computational Method 51
5.1.3.Computational Results and Discussion 52
5.1.4.Experimental Method 57
5.1.5.Experimental Results 57
5.1.6.Conclusion 59
5.2.Ferromagnetism Induced by Zn Vacancy Defect and Lattice Distortion in ZnO 61
5.2.1.Introduction 61
5.2.2.Computational Method 63
5.2.3.Computational Results 63
5.2.4.Conclusion 74
5.3.Mg Vacancy Defect Induced Half Metallic MgO(001) Film 76
5.3.1.Introduction 76
5.3.2.Numerical Method 77
5.3.3.Results and Discussions 78
5.3.4.Conclusion 85
5.4.Magnetic Property of Carbon doped ZnO and X-ray Magnetic Circular Dichroism 86
5.4.1.Introduction 86
5.4.2.Computational Method 87
5.4.3.Results and Discussions 88
5.4.4.Summary 98
5.5.Ultrathin Half Metallic N and Antiferromagnetic Semiconducting C Layers on MgO(001) 99
5.5.1.Introduction 99
5.5.2.Numerical Method 100
5.5.3.Results and Discussions 101
5.5.4.Summary 110
5.6.Half Metallic MgN and Ferromagnetic MgC Films on MgO(001) Surface 111
5.6.1.ntroduction 111
5.6.2.Numerical Method 112
5.6.3.Results and Discussions 113
5.6.4.ummary 124
5.7.Giant Perpendicular Magnetic Anisotropy of An Ir Monolayer on A NiAl(001) Surface 125
5.7.1.Introduction 125
5.7.2.Numerical Method 126
5.7.3.Results and Discussion 127
5.7.4.Summary 135
5.8.Large Perpendicular Magnetic Anisotropy of Ultrathin Ru and Rh Films on NiAl(001) Surface 136
5.8.1.Introduction 136
5.8.2.Numerical Method 138
5.8.3.Results and Discussions 139
5.8.4.Summary 152
6.Conclusions 153
7.References 158
8.Publications 167
- Degree
- Doctor
-
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