Publications (19)56.56 Total impact

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ABSTRACT: The temperature ($T$) dependence of the optical conductivity spectra $\sigma(\omega)$ of a single crystal SrRuO$_3$ thin film is studied over a $T$ range from 5 to 450 K. We observed significant $T$ dependence of the spectral weights of the charge transfer and interband $d$$d$ transitions across the ferromagnetic Curie temperature ($T_c$ ~ 150 K). Such $T$ dependence was attributed to the increase in the Ru spin moment, which is consistent with the results of density functional theory calculations. $T$ scans of $\sigma(\Omega, T)$ at fixed frequencies $\Omega$ reveal a clear $T^2$ dependence below $T_c$, demonstrating that the Stoner mechanism is involved in the evolution of the electronic structure. In addition, $\sigma(\Omega, T)$ continues to evolve at temperatures above $T_c$, indicating that the local spin moment persists in the paramagnetic state. This suggests that SrRuO$_3$ is an intriguing oxide system with itinerant ferromagnetism.Physical Review Letters 09/2013; 110(24). DOI:10.1103/PhysRevLett.110.247202 · 7.73 Impact Factor 
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ABSTRACT: We report on a fundamental thickness limit of the itinerant ferromagnetic oxide SrRuO3 that might arise from the orbitalselective quantum confinement effects. Experimentally, SrRuO3 films remain metallic even for a thickness of 2 unit cells (uc), but the Curie temperature TC starts to decrease at 4 uc and becomes zero at 2 uc. Using the Stoner model, we attributed the TC decrease to a decrease in the density of states (No). Namely, in the thin film geometry, the hybridized Ru dyz,zx orbitals are terminated by top and bottom interfaces, resulting in quantum confinement and reduction of No. 
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ABSTRACT: We present an effective tightbinding Hamiltonian for Li2IrO3 based on maximally localized Wannier functions for states near the Fermi level as obtained from firstprinciples electronic structure calculations. The majority of the Wannier orbitals are positioned on the center site with dominant jeff=1/2 character, while relatively small jeff=3/2 tails lie on the three nearestneighbor sites. Interestingly, the spin quantization axis of the jeff=1/2 components deviates from the local octahedral axis and points toward the nearestneighbor Ir direction. In our tightbinding model, there are relatively strong nextnearest and the thirdnearestneighbor hopping terms within the twodimensional Ir honeycomb lattice in addition to the relatively small but significant interlayer hopping terms. The ratio between the nearestneighbor and the thirdnearestneighbor hoppings, which can be controlled by the lattice strain, plays a critical role in determinating the Z2invariant character of Li2IrO3. From our tightbinding model, we also derive an effective Hamiltonian and its parameters for the magnetic exchange interactions. Due to the complex spindependent nextnearestneighbor hopping terms, our pseudospin Hamiltonian includes significant nextnearestneighbor antiferromagnetic Kitaev terms as well as DzyaloshinskiiMoriya and Heisenberg interactions. From our model Hamiltonian we estimate classical energies of collinear magnetic configurations as functions of the Hund's coupling of the Ir atom, from which zigzagtype magnetic order gives the lowest energy.Physical review. B, Condensed matter 04/2013; 87(16). DOI:10.1103/PhysRevB.87.165117 
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ABSTRACT: We performed angleresolved photoemission studies on Cu(111) and Au(111) surface states with circularly polarized light to investigate local orbital angular momentum (OAM) structures. Existence of OAM is confirmed, as predicted, to exist in systems with an inversion symmetry breaking. Cu(111) surface state bands are found to have chiral OAM in spite of very small spinorbit coupling, consistent with the theoretical prediction. As for Au(111), we observe split bands for which OAM for the inner and outer bands are parallel, unlike the Bi2Se3 case. We also performed firstprinciples calculations and the results are found to be consistent with experimental results. Moreover, the majority of OAM is found to have dorbital origin while a small contribution comes from porbitals. An effective Hamiltonian that incorporates the role of OAM is derived and is used to extract the spin and OAM structures. We discuss the evolution of angular momentum structures from a pure OAM system to a strongly spinorbitentangled state. 
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ABSTRACT: The phenomenon of Rashba spinorbit coupling is examined theoretically for an ultrathin magnetic layer in contact with a nonmagnetic heavymetal layer. From a firstprinciples calculation, a large Rashba parameter of order 1 eV Å is obtained, which makes the Rashba interaction a powerful tool for enhancing the spintransfer torque. Interestingly, the magnitude and sign of the parameter vary from energy band to energy band, which we attribute to bandspecific chiral ordering of the orbital angular momentum. We argue that the band dependence of the Rashba parameter provides a natural explanation for a host of recent experiments and may enhance the potential for device application of the Rashbaactive magnetic layer.Physical review. B, Condensed matter 01/2013; 87(4). DOI:10.1103/PhysRevB.87.041301 
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ABSTRACT: Theory of Rashba spinorbit coupling in magnetic metals is worked out from microscopic Hamiltonian describing dorbitals. When structural inversion symmetry is broken, electron hopping between $d$orbitals generates chiral ordering of orbital angular momentum, which combines with atomic spinorbit coupling to result in the Rashba interaction. Rashba parameter characterizing the interaction is bandspecific, even reversing its sign from band to band. Large enhancement of the Rashba parameter found in recent experiments is attributed to the orbital mixing of 3d magnetic atoms with nonmagnetic heavy elements as we demonstrate by firstprinciples and tightbinding calculations. 
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ABSTRACT: We performed angleresolved photoemission studies on Cu(111) and Au(111) surface states with circularly polarized light to investigate local orbital angular momentum (OAM) structures. Existence of OAM is confirmed, as predicted, to exist in systems with an inversion symmetry breaking. Cu(111) surface state bands are found to have chiral OAM in spite of very small spinorbit coupling, consistent with the theoretical prediction. As for Au(111), we observe split bands for which OAM for the inner and outer bands are parallel, unlike the Bi2Se3 case. We also performed firstprinciples calculations and the results are found to be consistent with experimental results. Moreover, the majority of OAM is found to have dorbital origin while a small contribution comes from p orbitals. An effective Hamiltonian that incorporates the role of OAM is derived and is used to extract the spin and OAM structures. We discuss the evolution of angular momentum structures from a pure OAM system to a strongly spinorbitentangled state. We predict that the transition occurs through a reversal of the OAM direction at a k point in the inner band if the system has a proper spinorbit coupling strength.Physical Review B 05/2012; 85(19). DOI:10.1103/PhysRevB.85.195402 · 3.66 Impact Factor 
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ABSTRACT: We show, by way of tightbinding and firstprinciples calculations, that a onetoone correspondence between an electron's crystal momentum k and nonzero orbital angular momentum (OAM) is a generic feature of surface bands. The OAM forms a chiral structure in momentum space much as its spin counterpart in Rashba model does, as a consequence of the inherent inversion symmetry breaking at the surface but not of spinorbit interaction. This is the orbital counterpart of conventional Rashba effect and may be called the “orbital Rashba effect.” The circular dichroism (CD) angleresolved photoemission (ARPES) method is an efficient way to detect this new order, and we derive formulas explicitly relating the CDARPES signal to the existence of OAM in the band structure. The cases of degenerate p and dorbital bands are considered.Physical review. B, Condensed matter 05/2012; 85(19). DOI:10.1103/PhysRevB.85.195401 
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ABSTRACT: We predict a quantum phase transition from normal to topological insulators in the 5d transition metal oxide Na2IrO3, where the transition can be driven by the change of the longrange hopping and trigonal crystal field terms. From the firstprinciplesderived tightbinding Hamiltonian, we determine the phase boundary through the parity analysis. In addition, our firstprinciples calculations for Na2IrO3 model structures show that the interlayer distance can be an important parameter for the existence of a threedimensional strong topological insulator phase. Na2IrO3 is suggested to be a candidate material which can have both a nontrivial topology of bands and strong electron correlations.Physical Review Letters 03/2012; 108(10):106401. DOI:10.1103/PhysRevLett.108.106401 · 7.73 Impact Factor 
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ABSTRACT: We demonstrate that the chiral orbital angular momentum (OAM) structure can emerge as a result of broken inversion symmetry especially at the metal surfaces. The surfacenormal electric field is responsible for chiral OAM states even if spinorbit interaction is negligible. Such chiral OAM structure can be measured by a circular dichroism (CD) in angleresolved photoemission spectroscopy (ARPES). To confirm the existence of OAM and its detection by CDARPES, we perform simulation of CDARPES for Cu surface states by firstprinciples calculation and the results agree well with our CDARPES experiment. Addition of the spinorbit interaction to the chiral OAM structure produces a chiral spin angular momentum (SAM) pattern and the corresponding Rashbatype band splitting. We assert that OAM polarization should be a more widespread feature than the chiral spin structure which requires strong spinorbit coupling. 
Article: Topological quantum phase transitions driven by external electric fields in Sb2Te3 thin films
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ABSTRACT: Using firstprinciples calculations, we show that topological quantum phase transitions are driven by external electric fields in thin films of Sb(2)Te(3). The film, as the applied electric field normal to its surface increases, is transformed from a normal insulator to a topological insulator or vice versa depending on the film thickness. We identify the band topology by directly calculating the Z(2) invariant from electronic wave functions. The dispersion of edge states is also found to be consistent with the bulk band topology in view of the bulkboundary correspondence. We present possible applications of the topological phase transition as an on/off switch of the topologically protected edge states in nanoscale devices.Proceedings of the National Academy of Sciences 12/2011; 109(3):6714. DOI:10.1073/pnas.1119010109 · 9.81 Impact Factor 
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ABSTRACT: We show, by way of tightbinding and firstprinciples calculations, that a onetoone correspondence between electron's crystal momentum k and nonzero orbital angular momentum (OAM) is a generic feature of surface bands. The OAM forms a chiral structure in momentum space much as its spin counterpart in Rashba model does, as a consequence of the inherent inversion symmetry breaking at the surface but not of spinorbit interaction. Circular dichroism (CD) angleresolved photoemission (ARPES) experiment is an efficient way to detect this new order, and we derive formulas explicitly relating the CDARPES signal to the existence of OAM in the band structure. The cases of degenerate p and dorbital bands are considered. 
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ABSTRACT: We propose that the existence of local orbital angular momentum (OAM) on the surfaces of highZ materials plays a crucial role in the formation of Rashbatype surface band splitting. Local OAM state in a Bloch wave function produces an asymmetric charge distribution (electric dipole). The surfacenormal electric field then aligns the electric dipole and results in chiral OAM states and the relevant Rashbatype splitting. Therefore, the band splitting originates from electric dipole interaction, not from the relativistic Zeeman splitting as proposed in the original Rashba picture. The characteristic spin chiral structure of Rashba states is formed through the spinorbit coupling and thus is a secondary effect to the chiral OAM. Results from firstprinciples calculations on a single Bi layer under an external electric field verify the key predictions of the new model.Physical Review Letters 10/2011; 107(15):156803. DOI:10.1103/PhysRevLett.107.156803 · 7.73 Impact Factor 
Article: Emergence of Orbital Angular Momentum by Inversion Symmetry Breaking and Its Detection by ARPES
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ABSTRACT: Rashbasplit surface band is characterized by a onetoone correspondence between the electron's momentum k and its spin orientation. Here we show that a similar correspondence between momentum and orbital angular momentum (OAM) must exist on surface bands once the inversion symmetry is broken. The correspondence is valid even when there is no spinorbit interaction. Tightbinding and firstprinciples calculations are presented to support our claim. As a method to detect such OAMmomentum correspondence, we propose the circular dichroism (CD) experiment using the angleresolved photoemission (ARPES) setup. CDARPES experiment performed on Cu surface confirms the existence of chiral OAM. A new concept of "orbital Galvanic effect" is proposed. 
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ABSTRACT: Recently defect induced ferroelectricity in SrTiO3 has been reported at room temperature. Strontiumoxygen vacancies were suggested as a possible source of electric polarization regarding to the existence of midgap states. To understand the detailed electronic structures induced by defects and their formation energies, we carried out densityfunctionaltheory calculations for various defects such as Sr, Ti, O, SrO, SrO O vacancies. We employed the LDA+U method as implemented in the VASP code to describe the dorbital occupation at the Ti site due to the presence of oxygen vacancy. A complex of SrOO vacancies is found to contribute to the localized electronic states in the band gap and its formation energy is small enough to form easily under the poor oxygen limit. We conclude that the vacancycomplex defects play a crucial role in determination of the physical properties of SrTiO3 thin films. 
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ABSTRACT: We have investigated the electronic structure of double perovskites, Ba(2)FeReO(6) (metallic) and Ca(2)FeReO(6) (insulating) using optical and xray absorption spectroscopy. By comparing the experimental results with the density functional theory calculations, we found that the electronic structure of Ba(2)FeReO(6) could be determined from the interaction of the electron correlation and spinorbit coupling. On the other hand, for Ca(2)FeReO(6), the lattice distortion and electron correlation are important in determining the electronic structure. Additionally, the insulating gap in Ca(2)FeReO(6) is realized by the spinorbit coupling. Our work shows that the subtle interplay of the spinorbit interaction, electron correlation, and lattice distortion should be taken into account to understand the electronic structure of the 5d transition metal oxides.Journal of Physics Condensed Matter 09/2010; 22(34):345602. DOI:10.1088/09538984/22/34/345602 · 2.22 Impact Factor 
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ABSTRACT: We report on a fundamental thickness limit of the itinerant ferromagnetic oxide SrRuO$_3$ that might arise from the orbitalselective quantum confinement effects. Experimentally, SrRuO$_3$ films remain metallic even for a thickness of 2 unit cells (uc), but the Curie temperature, T$_C$, starts to decrease at 4 uc and becomes zero at 2 uc. Using the Stoner model, we attributed the T$_C$ decrease to a decrease in the density of states (N$_o$). Namely, in the thin film geometry, the hybridized Rud$_yz,zx$ orbitals are terminated by top and bottom interfaces, resulting in quantum confinement and reduction of N$_o$.Physical Review Letters 07/2009; 103:057201. DOI:10.1103/PhysRevLett.103.057201 · 7.73 Impact Factor 
Article: Mott Insulating Ground State and its Proximity to SpinOrbit Insulators in Na$_{2}$IrO$_{3}$
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ABSTRACT: We present an antiferromagnetically ordered ground state of Na$_{2}$IrO$_{3}$ based on densityfunctionaltheory calculations including both spinorbit coupling and onsite Coulomb interaction $U$. We show that the splitting of $e_{g}'$ doublet states by the strong spinorbit coupling is mainly responsible for the intriguing nature of its insulating gap and magnetic ground state. Due to its proximity to the spinorbit insulator phase, the magnetic ordering as obtained with finite $U$ is found to exhibit a strong inplane anisotropy. The phase diagram of Na$_{2}$IrO$_{3}$ suggests a possible interplay between spinorbit insulator and Mott antiferromagnetic insulator phases. Comment: 5 pages, 4 figures 
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ABSTRACT: We present an extension of the local moment approach to the Anderson impurity model with spindependent hybridization. By employing the twoselfenergy description, as originally proposed by Logan and coworkers, we applied the symmetry restoration condition for the case with spindependent hybridization. Selfconsistent ground states were determined through variational minimization of the ground state energy. The results obtained with our spindependent local moment approach applied to a quantum dot system coupled to ferromagnetic leads are in good agreement with those obtained from previous work using numerical renormalization group calculations.Journal of Physics Condensed Matter 09/2007; 19(45). DOI:10.1088/09538984/19/45/456203 · 2.22 Impact Factor
Publication Stats
150  Citations  
56.56  Total Impact Points  
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Institutions

2007–2013

Seoul National University
 Department of Physics and Astronomy
Sŏul, Seoul, South Korea
