| 摘要 | 第6-8页 |
| abstract | 第8-9页 |
| Chapter 1 Introduction | 第20-36页 |
| 1.1 Brief history of the magneto-electric (ME) effect | 第20-22页 |
| 1.2 Related work | 第22页 |
| 1.3 Literature review | 第22-28页 |
| 1.3.1 Symmetry breaking and ME effect in Cr2O3 single crystal | 第23-26页 |
| 1.3.2 Symmetry operations | 第26-27页 |
| 1.3.3 Higher order contributions | 第27-28页 |
| 1.4 Limitations of the ME applications | 第28-29页 |
| 1.4.1 Second breakthrough in the ME effect | 第29页 |
| 1.5 Diversion to composite materials | 第29-31页 |
| 1.5.1 Class of materials showing ME effect | 第30-31页 |
| 1.6 Importance in optical effects | 第31-32页 |
| 1.7 Overview of this work | 第32-36页 |
| Chapter 2 Magnetic uniaxial anisotropic magneto-electric media | 第36-58页 |
| 2.1 Introduction | 第36页 |
| 2.2 Representation of tensors | 第36-38页 |
| 2.3 Free energy expansion | 第38-40页 |
| 2.4 Essential exercise to work out the wave equation | 第40-43页 |
| 2.5 Definition of the linear magneto-electric effect | 第43页 |
| 2.6 Role of α in the tensorial magneto-electric media | 第43-44页 |
| 2.7 The uniaxial anisotropic media and the optical effects | 第44-45页 |
| 2.8 Theory of the tensorial magneto-electric effect in a magnetic uniaxial anisotropicmedium | 第45-48页 |
| 2.9 Equation form of the anisotropic magneto-electric medium | 第48-56页 |
| 2.10 Conclusion | 第56-58页 |
| Chapter 3 The double Jones birefringence and the D’yakonov surface wave | 第58-76页 |
| 3.1 Introduction | 第58页 |
| 3.2 Electromagnetic wave | 第58-59页 |
| 3.3 Important cases with additional constraints | 第59-73页 |
| 3.3.1 The trivial case when we assume no magneto-electric effect | 第60-61页 |
| 3.3.2 When the media has magnetic structure and the magneto-electric effect | 第61-63页 |
| 3.3.3 Surface wave in uniaxial anisotropic magneto-electric medium | 第63-64页 |
| 3.3.4 Media with the magneto-isotropic behavior and magneto-electric tensor | 第64-73页 |
| 3.4 A comparison with other published results | 第73-74页 |
| 3.5 Relationship with the AC and DC frequency | 第74-75页 |
| 3.6 Conclusion | 第75-76页 |
| Chapter 4 Electromagnetic wave through a vortex | 第76-88页 |
| 4.1 Introduction | 第76页 |
| 4.2 Maxwell’s equation as the starting point | 第76-77页 |
| 4.3 Defining the velocity of the vortex | 第77-86页 |
| 4.4 Conclusion | 第86-88页 |
| Chapter 5 Fluorite phase TiO2and its properties under pressure | 第88-104页 |
| 5.1 Introduction | 第88页 |
| 5.2 Software and the parameters used | 第88-89页 |
| 5.3 Structural properties | 第89-92页 |
| 5.3.1 Relaxed structure | 第89-90页 |
| 5.3.2 Density of states (DOS) | 第90-92页 |
| 5.4 Elastic and acoustic properties | 第92-96页 |
| 5.5 Optical properties | 第96-102页 |
| 5.6 Conclusion | 第102-104页 |
| Chapter 6 Structure designing for the photonic crystal fiber | 第104-116页 |
| 6.1 Introduction | 第104页 |
| 6.2 COMSOL Multiphysics | 第104-105页 |
| 6.3 Simple circular geometry | 第105-108页 |
| 6.3.1 Defining materials and observing the power flow | 第107-108页 |
| 6.4 Modified circular geometry | 第108-112页 |
| 6.5 Geometry comprising air holes | 第112-114页 |
| 6.5.1 Mode analysis for the air hole geometry | 第113-114页 |
| 6.6 Conclusion | 第114-116页 |
| Chapter 7 Conclusion | 第116-120页 |
| 7.1 Future work | 第117-120页 |
| Appendix A The calculations for the derivation of the matrix given in the Eq. (2.65) | 第120-130页 |
| Appendix B The special case when β' and τ' both are setequal to zero | 第130-138页 |
| Appendix C Setting the value of η equal to zero | 第138-142页 |
| Appendix D Media with the magneto-isotropic behavior and magneto-electric tensor | 第142-146页 |
| Appendix E Comparison with Hehl’s results | 第146-150页 |
| Bibliography | 第150-162页 |
| Acknowledgements | 第162-164页 |
| Publications | 第164-166页 |
| About the author | 第166页 |
