Academic literature on the topic 'Interactions spin-orbit'

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Journal articles on the topic "Interactions spin-orbit"

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JOHANNESSON, HENRIK, DAVID F. MROSS, and ERIK ERIKSSON. "TWO-IMPURITY KONDO MODEL: SPIN-ORBIT INTERACTIONS AND ENTANGLEMENT." Modern Physics Letters B 25, no. 12n13 (May 30, 2011): 1083–91. http://dx.doi.org/10.1142/s0217984911026796.

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Motivated by proposals to employ RKKY-coupled spins as building blocks in a solid-state quantum computer, we analyze how the RKKY interaction in a 2D electron gas is influenced by spin-orbit interactions. Using a two-impurity Kondo model with added Dresselhaus and Rashba spin-orbit interactions we find that spin-rotational invariance of the RKKY interaction — essential for a well-controllable two-qubit gate — is restored when tuning the Rashba coupling to have the same strength as the Dresselhaus coupling. We also discuss the critical properties of the two-impurity Kondo model in the presence of spin-orbit interactions, and extract the leading correction to the block entanglement scaling due to these interactions.
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Conzett, H. E. "Spin-orbit and spin-spin interactions in ΛNandNNscattering." Physical Review C 48, no. 2 (August 1, 1993): 924–25. http://dx.doi.org/10.1103/physrevc.48.924.

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Yildirim, T., A. B. Harris, O. Entin-Wohlman, and Amnon Aharony. "Symmetry, Spin-Orbit Interactions, and Spin Anisotropies." Physical Review Letters 73, no. 21 (November 21, 1994): 2919–22. http://dx.doi.org/10.1103/physrevlett.73.2919.

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Bliokh, K. Y., F. J. Rodríguez-Fortuño, F. Nori, and A. V. Zayats. "Spin–orbit interactions of light." Nature Photonics 9, no. 12 (November 27, 2015): 796–808. http://dx.doi.org/10.1038/nphoton.2015.201.

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Ovchinnikov, Yu N. "Superconductors with spin–orbit interactions." International Journal of Modern Physics B 30, no. 25 (September 28, 2016): 1650183. http://dx.doi.org/10.1142/s0217979216501836.

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The effect of spin-orbit (SO) interaction on the formation of the critical states in thin superconducting films in magnetic field oriented along the film is investigated. Hereby, the case of interband pairing is considered. It was found that eight branches exist in the plane of two parameters [Formula: see text] determined by the value of magnetic field and SO interaction. Six modes leads to inhomogeneous states with different values of the impulse [Formula: see text]. Each state is doubly degenerate over direction of impulse [Formula: see text]. The parameter values at critical point are found for all eight branches in explicit form for zero temperature. The optimal two branches are estimated, corresponding to largest critical magnetic field value for given SO interaction.
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Wei, Qun. "Investigation of the Spin-Hamiltonian Parameters and the Local Structure of Ni2+ Ions in CsMgX3 (X = Cl, Br, I) Crystals." Zeitschrift für Naturforschung A 63, no. 3-4 (April 1, 2008): 188–92. http://dx.doi.org/10.1515/zna-2008-3-412.

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Taking into account spin-spin (SS), spin-other-orbit (SOO), and orbit-orbit (OO) interactions in addition to general spin-orbit (SO) interactions, the local structures of Ni2+ in CsMgX3 (X = Cl, Br, I) are theoretically investigated by using the complete diagonalization method (CDM). On this basis, it is found that the local angles, at the Ni2+ centres are larger than those, at the hosts. The contributions to the spin-Hamiltonian parameters from spin triplets and slight magnetic interactions are discussed.
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Abramov, I. E., and A. V. Andreev. "Hyperfine structure of a hydrogen-like atom due to orbit-orbit, spin-orbit, and spin-spin interactions." Moscow University Physics Bulletin 62, no. 5 (October 2007): 283–86. http://dx.doi.org/10.3103/s0027134907050037.

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Yin, He, Wang Fan, and Chun Wa Wong. "Baryon-nucleon spin-orbit forces from symmetric quark-quark spin-orbit interactions." Nuclear Physics A 451, no. 4 (April 1986): 653–65. http://dx.doi.org/10.1016/0375-9474(86)90297-6.

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Bliokh, K. Y., F. J. Rodríguez-Fortuño, F. Nori, and A. V. Zayats. "Erratum: Spin–orbit interactions of light." Nature Photonics 11, no. 2 (February 2017): 137. http://dx.doi.org/10.1038/nphoton.2016.275.

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Hao, Ya-Fei. "Spin-orbit interactions in semiconductor superlattice." Physics Letters A 384, no. 4 (February 2020): 126092. http://dx.doi.org/10.1016/j.physleta.2019.126092.

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Dissertations / Theses on the topic "Interactions spin-orbit"

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Lenz, Lucia [Verfasser], and Hermann [Akademischer Betreuer] Grabert. "Spin orbit interactions in carbon based materials = Spin-Orbit Wechselwirkungen in Kohlenstoff basierten Materialien." Freiburg : Universität, 2013. http://d-nb.info/1123478147/34.

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Stano, Peter. "Controlling electron quantum dot qubits by spin-orbit interactions." [S.l.] : [s.n.], 2007. http://deposit.ddb.de/cgi-bin/dokserv?idn=983802254.

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Smirnov, Sergey. "Ratchet phenomena in quantum dissipative systems with spin-orbit interactions." kostenfrei, 2009. http://www.opus-bayern.de/uni-regensburg/volltexte/2009/1407/.

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Pham, Thaï Ha. "Spin-Orbit effect in ferrimagnetic thin film." Electronic Thesis or Diss., Université de Lorraine, 2020. http://www.theses.fr/2020LORR0051.

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Un fort intérêt se porte actuellement sur l'influence du couplage spin-orbite sur les propriétés de transport. Notamment la possibilité de retourner l’aimantation grâce au couple spin-orbite (SOT). Afin d’envisager l’utilisation du SOT pour des applications dans le domaine de l’électronique de spin il est nécessaire de réduire le courant critique nécessaire au retournement et diminuer ou éliminer le champ magnétique externe planaire appliqué. Mon travail de thèse concerne l’étude expérimentale de systèmes bicouches métaux lourds/ ferrimagnétique (W/ CoxTb1−x ou Pt / CoxTb1−x ). Dans les alliages ferrimagnétiques, l’aimantation du sous réseau du Cobalt est couplé antiparallèlement à l’aimantation du sous réseau de Terbium. Ces alliages sont particulièrement intéressants car pour une certaine concentration, il existe une température pour laquelle l’aimantation des deux sous réseaux sont égales et donc que l’aimantation résultante est nulle. Dans un premier temps j’ai caractérisé ces systèmes par magnétométrie et par mesures de résistance Hall anomale pour des températures allant de 10 à 350 K. Les expériences de renversement d’aimantation induite par le courant ont été effectuées dans une géométrie « couple Spin-orbite » (SOT) où les impulsions de courant sont injectées dans le plan et le retournement de l’aimantation est détectée par la mesure de la résistance de Hall. Le retournement complet de l'aimantation a été observée dans tous les échantillons. Le courant de retournement varie de façon continue avec la composition de l’alliage et nous n’avons pas observé une réduction de celui-ci au point de compensation malgré la forte augmentation de l’efficacité du SOT. Un modèle basé sur les équations de Landau-Lifschitz-Gilbert couplées montre que la densité du courant de retournement est proportionnelle à l’anisotropie perpendiculaire effective, qui ne diminue pas au point de compensation. Bien que le TbCo possède une forte anisotropie magnétique perpendiculaire, le retournement se produit pour un champ magnétique planaire faible. Nous avons pu montrer que le chauffage provoqué par le courant joue un rôle important. En effet le retournement semble se produire à une température de commutation caractéristique Tswitch induite par le chauffage Joule qui est supérieure aux températures de compensation magnétique et angulaire mais inférieure à sa température de Curie (TC). Tout se passe comme s’il fallait atteindre une température proche de TC pour que le retournement ait lieu
The influence of spin-orbit coupling on transport properties has been a topic of strong and growing interest in the last ten years. In order to use of spin-orbit torque for applications in the field of spin electronics, it is necessary to reduce the critical current necessary for the reversal and to decrease or eliminate the planar external magnetic field applied. My thesis work concerns the experimental study of heavy metal / ferrimagnetic bilayer model systems (W / CoxTb1-x or Pt / CoxTb1 - x). In such ferrimagnetic alloys, the magnetization of the Cobalt sub-lattice is coupled antiparallel to the magnetization of the Terbium sub-lattice. These alloys are particularly interesting because for certain concentration, there is a temperature for which the magnetization of the two sub-networks are equal resulting in zero magnetization. This is the magnetization compensation temperature. At first I characterized these systems using magnetometry and Hall cross measurements for temperatures ranging from 10 to 350 K. The experiments of magnetization reversal of magnetization induced by the current were carried out in a "Spin- orbit torque” (SOT) geometry where the current pulses are injected into the plane and the reversal of the magnetization is detected by measuring the Hall resistance. The complete magnetization reversal was observed in all the samples. The current reversal was found to vary continuously with the alloy composition and we did not observe any reduction at the compensation point despite the large increase in the SOT efficiency. A model based on the coupled Landau-Lifschitz-Gilbert equations shows that the reversal current density is proportional to the effective perpendicular anisotropy, which does not decrease at the compensation point. Although TbCo has a strong perpendicular magnetic anisotropy, the reversal occurs for a weak planar magnetic field. We were able to show that the heating caused by the current plays an important role in the switching. Indeed the reversal seems to occur at a characteristic switching temperature (Tswitch) induced by Joule heating. Tswitch is larger than the magnetic and angular compensation temperatures, but lower than the Curie temperature. Everything happens as if it was necessary to reach a temperature close to the order temperature for the reversal to take place
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Hernangomez, Perez Daniel. "Spin-orbit Coupling and Strong Interactions in the Quantum Hall Regime." Thesis, Grenoble, 2014. http://www.theses.fr/2014GRENY087.

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L'effet Hall quantique, qui apparaît dans les gaz d'électrons bidimensionnels soumis à un champ magnétique perpendiculaire et à basses températures, a été un sujet de recherche intense pendant les derniers trente ans, en particulier, à cause des manifestations spectaculaires de la mécanique quantique dans les propriétés de transport à l'échelle macroscopique. Dans cette thèse, on étend l'horizon de la recherche au niveau théorique sur ce sujet en considérant les effets du couplage spin-orbite et l'interaction électron-électron de façon analytique dans ce régime.Dans la première partie de ce manuscrit, on considère l'effet simultané du couplage spin-orbite de type Rashba et l'interaction Zeeman dans le régime de l'effet Hall quantique entier. Pour cela, on étend un formalisme de fonctions de Green basé sur des états de vortex cohérents avec l'objectif d'inclure le couplage entre les degrés de liberté orbitaux et de spin dans les états de dérive électroniques. Puis, comme première application, on montre comment obtenir analytiquement, nonperturbativement et de manière contrôlée des fonctionnelles quantiques (spectre et densité d'états locale) pour des potentiels électrostatiques arbitraires et localement plats. Les fonctionnelles sont ensuite analysées dans différents régimes de températures et comparées aux données expérimentales obtenues à partir des sondes de spectroscopie locales. Comme seconde mise en pratique du formalisme, on étudie en profondeur les propriétés de transport de charge et de spin dans un régime hydrodynamique d'équilibre local (ou quasi-équilibre) et dérive des expressions analytiques qui incorporent les caractères non-relativiste et relativiste des gaz d'électrons avec couplage spin-orbite de type Rashba.Dans la deuxième partie de cette thèse, on s'occupe du problème de traiter analytiquement les fortes interactions électron-électron dans le régime de l'effet Hall quantique fractionnaire. A cette fin, on étudie un problème à deux corps généralisé avec du désordre et des corrélations électroniques, en utilisant une nouvelle représentation d'états de vortex cohérents. Des corrélations à longue portée entre les particules sont incorporées de manière topologique à travers la présence d'une métrique non-Euclidienne. Subséquemment, on montre que ces états de vortex forment bien une base d'un espace de Hilbert élargi, puis on dérive l'équation du mouvement pour la fonction de Green. Enfin, on vérifie la consistance de notre théorie pour tout niveau de Landau de paire et on discute la nécessité d'aller au-delà de la limite semiclassique (à champ magnétique infinie) pour obtenir des gaps dans chaque niveau de énergie
The quantum Hall effect, appearing in disordered two-dimensional electron gases under strong perpendicular magnetic fields and low temperatures, has been a subject of intense research during the last thirty years due to its very spectacular macroscopic quantum transport properties. In this thesis, we expand the theoretical horizon by analytically considering the effects of spin-orbit coupling and strong electron-electron interaction in these systems.In the first part of the manuscript, we examine the simultaneous effect of Rashba spin-orbit and Zeeman interaction in the integer quantum Hall regime. Under these conditions, we extend a coherent-state vortex Green's function formalism to take into account the coupling between orbital and spin degrees of freedom within the electronic drift states. As a first application of this framework, we analytically compute controlled microscopic nonperturbative quantum functionals, such as the energy spectrum and the local density of states, in arbitrary locally flat electrostatic potential landscapes, which are then analyzed in detail in different temperature regimes and compared to scanning tunnelling experimental data. As a second application, we thoroughly study local equilibrium charge and spin transport properties and derive analytical useful formulas which incorporate the mixed non-relativistic and relativistic character of Rashba-coupled electron gases.In the second part of this thesis, we deal with the problem of analytically incorporating strong electron-electron interactions in the fractional quantum Hall regime. To this purpose, we consider a generalized two-body problem where both disorder and correlations are combined and introduce a new vortex coherent-state representation of the two-body states that naturally include long-range correlations between the electrons. The novelty of this theory is that correlations are topologically built in through the non-Euclidean metric of the Hilbert space. Next, we show that this kind of vortex states form a basis of an enlarged Hilbert space and derive the equation of motion for the Green's function in this representation. Finally, we check the consistency of our approach for any Landau level of the pair and discuss the necessity of going beyond the semiclassical (infinite magnetic field) approximation to obtain energy gaps within each energy level
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Bush, Matthew Peter. "Spin-dependent interactions in the three-body eikonal model." Thesis, University of Surrey, 1997. http://epubs.surrey.ac.uk/844619/.

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A derivation of the elastic scattering differential cross section, within a three-body eikonal model, that treats both central and spin-orbit interactions between the constituent projectile clusters and the target is presented. This formalism is then used in the theoretical study of the scattering of 8B from 12C at 40 MeV/nucleon. The proton halo candidate, 8B, is taken to consist of a single valence proton orbiting a 7Be core cluster. Calculation of the elastic scattering amplitude relies upon determining the phase shifts caused as the projectile passes through the region of interaction with the target. A form for the orbital angular momentum operator of each projectile cluster about the target is obtained that allows a relatively simple form for the spin-orbit phase shift functions, analogous to those for the central interactions, to be deduced. The study of the angular distribution of the elastic scattering differential cross section is carried out in two parts. Initially the effect of elastic break-up and recombination of the projectile during the scattering process, only taking into account central interactions, is studied. To gauge the magnitude of these effects, within the three-body model, the elastic scattering differential cross section, in the limit of no projectile break-up, is derived. Despite the very small binding energy of 8B it is shown that these effects are quite small. It is also shown, however, that these effects become more conspicuous as the valence proton becomes less localised about the core. Finally the effect of including spin-orbit interactions is studied. In the system under study these effects are shown to have an almost negligible effect on the angular distribution of the differential cross section. However, increasing the projectile kinetic energy to the region of hundreds of MeV/nucleon is seen to increase their significance. Future calculations hope to look at the angular distribution of the elastic scattering differential cross section and vector and tensor analysing powers of polarised beams of deuterons as these systems are expected to show more sensitivity to spin- orbit interactions. Furthermore, with the possibility of polarised beams of halo nuclei, the three-body Glauber model would be an ideal theoretical tool with which to study certain of their spin-related phenomena too.
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Sichau, Jonas [Verfasser], and Robert H. [Akademischer Betreuer] Blick. "Electron Spin Resonance Studies on Spin-Orbit Interactions in Graphene / Jonas Sichau ; Betreuer: Robert H. Blick." Hamburg : Staats- und Universitätsbibliothek Hamburg, 2019. http://d-nb.info/1198404183/34.

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Kato, Takashi, Yasuhito Ishikawa, Hiroyoshi Itoh, and Jun-ichiro Inoue. "Intrinsic anisotropic magnetoresistance in spin-polarized two-dimensional electron gas with Rashba spin-orbit interaction." American Physical Society, 2008. http://hdl.handle.net/2237/11252.

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Liu, Jia, and 刘佳. "Exact solutions for electron pairing models with spin-orbit interactions and Zeeman coupling." Thesis, The University of Hong Kong (Pokfulam, Hong Kong), 2013. http://hdl.handle.net/10722/196010.

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Although a number of methods with appropriate approximations, such as mean-field theory, local density approximation, and tight-binding method have been well developed and widely used in solid state physics, they possess strong limitations, and thus physicists never stop trying to find methods that could rigorously solve the models of condensed matter systems. This thesis presents several new exact solutions for electron pairing models with spin-orbit interactions and Zeeman coupling, which have not been studied before. First, a type of electron pairing model with spin-orbit interactions or Zeeman coupling is solved exactly in the framework of the Richardson’s previous work for 2D cases. Based on the exact solutions for the electron pairing model with spin-orbit interactions, it is shown rigorously that the pairing symmetry is of the p+ip wave and the ground state possesses time-reversal symmetry, which are expected by the meanfield theory. And the difference is that such peroration from our framework is valid for any strength of the pairing interactions. Intriguingly, how Majorana fermions can emerge is also elaborated in a ribbon system as well. Condensation energy and critical magnetic field are calculated in two systems with the exact solutions, and compared with the relevant results achieved by the mean-field theory, the differences between our results and the mean-field theory show the significance of the work for exact solutions. Secondly, we generalize our scenario to 3D cases. Several remarks of the 3D case are given following the significant results from the 2D cases. And an unconventional type of Fulde-Ferrel-Larkin-Ovchinnikov ground state is revealed exactly, in which the center-of-mass momentum of the fermion pair is proportional to the Zeeman field. As a by-product, a similar Fulde-Ferrel-Larkin-Ovchinnikov state is also disclosed when the magnetic field is in the same plane of k for 2D case. In addition, applying the transformative Richardson ansatz in bosonic system, we elaborate on the drifting effect of the Zeeman field on the spin-orbit-coupled Bose-Einstein condensed matter as well. Finally, we discuss the application of the exact solutions in quantum entanglement quantification. The entanglement monotone concurrence is calculated with exact solutions for two models. It is found to be a smooth function of pairing interactions, as expected.
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Katukuri, Vamshi Mohan. "Quantum chemical approach to spin-orbit excitations and magnetic interactions in iridium oxides." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-160735.

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In the recent years, interest in TM oxides with 5d valence electrons has grown immensely due to the realization of novel spin-orbit coupled ground states. In these compounds, e.g., iridates and osmates, the intriguing situation arises where the spin-orbit and electron-electron interactions meet on the same energy scale. This has created a new window of interest in these compounds since the interplay of crystal field effects, local multiplet physics, spin-orbit couplings, and intersite hopping can offer novel types of correlated ground states and excitations. In 5d5 iridates, a spin-orbit entangled j = 1/2 Mott insulating state has been realized recently. A remarkable feature of such a ground state is that it gives rise to anisotropic magnetic interactions. The 2D honeycomb-lattice 213 iridium oxides, A2IrO3 (A=Li,Na), have been put forward to host highly anisotropic bond-dependent spin-spin interactions that resemble the Kitaev spin model, which supports various types of topological phases relevant in quantum computing. The 2D square-lattice 214 iridates Sr2IrO4 and Ba2IrO4 are, on the other hand, appealing because of their perceived structural and magnetic simi- larity to La2CuO4, the mother compound of the cuprate high-Tc superconductors. This has promoted the latter iridium oxide compounds as novel platforms for the search of high-Tc superconductivity. To put such considerations on a firm footing, it is essential to quantify the different coupling strengths and energy scales, as they for instance appear in effective Hamiltonian descriptions of these correlated systems. Moreover, it is important to correctly describe their effects. In this thesis, the electronic structure and magnetic properties of 5d5 (mainly 214 and 213) iridates are studied using wave-function-based quantum chemistry methods. These methods are fully ab initio and are capable of accurately treating the electron-electron interactions without using any ad hoc parameters. The spin-orbit entangled j = 1/2 ground state in 214, 213 and other lower symmetry Sr3CuIrO6 and Na4Ir3O8 iridates is first analyzed in detail, by studying the local electronic structure of the 5d5 Ir4+ ion. We establish that the longer-range crystal anisotropy, i.e., low-symmetry fields related to ionic sites beyond the nearest neighbor oxygen cage, strongly influence the energies of Ir d levels. The ground state in all the compounds studied is j = 1/2 like with admixture from j ≃ 3/2 states ranging from 1 – 15 %. Further, the average j ≃ 1/2 → j ≃ 3/2 excitation energy we find is around 0.6 eV. The NN magnetic exchange interactions we computed for 214 iridates are predominantly isotropic Heisenberg-like with J ~ 60 meV, 3 – 4 times smaller than found in isostructural copper oxides. However, the anisotropic interactions are an order of magnitude larger than those in cuprates. Our estimates are in excellent agreement with those extracted from experiments, e.g., resonant inelastic x-ray scattering measurements. For the 213 honeycomb-lattice Na2IrO3 our calculations show that the relevant spin Hamiltonian contains further anisotropic terms beyond the Kitaev-Heisenberg model. Nevertheless, we predict that the largest energy scale is the Kitaev interaction, 10 to 20 meV, while the Heisenberg superexchange and off-diagonal symmetric anisotropic couplings are significantly weaker. In the sister compound Li2IrO3, we find that the structural inequivalence between the two types of Ir-Ir links has a striking influence on the effective spin Hamiltonian, leading in particular to two very different NN superexchange pathways, one weakly AF (~ 1 meV) and another strongly FM (−19 meV). The latter gives rise to rigid spin-1 triplets on a triangular lattice.
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Books on the topic "Interactions spin-orbit"

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Cao, Gang, and Lance DeLong. Physics of Spin-Orbit-Coupled Oxides. Oxford University Press, 2021. http://dx.doi.org/10.1093/oso/9780199602025.001.0001.

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Prior to 2010, most research on the physics and chemistry of transition metal oxides was dominated by compounds of the 3d-transition elements such as Cr, Mn, Fe, Co, Ni, and Cu. These materials exhibited novel, important phenomena that include giant magnetoresistance in manganites, as well as high-temperature superconductivity in doped La2CuO4 and related cuprates. The discovery in 1994 of an exotic superconducting state in Sr2RuO4 shifted some interest toward ruthenates. Moreover, the realization in 2008 that a novel variant of the classic Mott metal-insulator transition was at play in Sr2IrO4 provided the impetus for a burgeoning group of studies of the influence of strong spin-orbit interactions in “heavy” (4d- and 5d-) transition-element oxides. This book reviews recent experimental and theoretical evidence that the physical and structural properties of 4d- and 5d-oxides are decisively influenced by strong spin-orbit interactions that compete or collaborate with comparable Coulomb, magnetic exchange, and crystalline electric field interactions. The combined effect leads to unusual ground states and magnetic frustration that are unique to this class of materials. Novel couplings between the orbital/lattice and spin degrees of freedom, which lead to unusual types of magnetic order and other exotic phenomena, challenge current theoretical models. Of particular interest are recent investigations of iridates and ruthenates focusing on strong spin-orbit interactions that couple the lattice and spin degrees of freedom.
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Nitta, J. Spin generation and manipulation based on spin-orbit interaction in semiconductors. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0013.

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This chapter focuses on the electron spin degree of freedom in semiconductor spintronics. In particular, the electrostatic control of the spin degree of freedom is an advantageous technology over metal-based spintronics. Spin–orbit interaction (SOI), which gives rise to an effective magnetic field. The essence of SOI is that the moving electrons in an electric field feel an effective magnetic field even without any external magnetic field. Rashba spin–orbit interaction is important since the strength is controlled by the gate voltage on top of the semiconductor’s two-dimensional electron gas. By utilizing the effective magnetic field induced by the SOI, spin generation and manipulation are possible by electrostatic ways. The origin of spin-orbit interactions in semiconductors and the electrical generation and manipulation of spins by electrical means are discussed. Long spin coherence is achieved by special spin helix state where both strengths of Rashba and Dresselhaus SOI are equal.
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Kozlova, Svetlana G., and Svyatoslav P. Gabuda. Spin-Orbit Interactions in PtF6 and in Related Octahedral Molecules and Fluorocomplexes. Nova Science Publishers, Incorporated, 2010.

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Kavokin, Alexey V., Jeremy J. Baumberg, Guillaume Malpuech, and Fabrice P. Laussy. Quantum Fluids of Light. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198782995.003.0010.

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In this chapter, we deal with polaritons as a “quantum fluid of light”, described by variants of the Gross–Pitaevskii equation. We discuss how interactions between flowing polaritons and a defect allow to study their superfluid regime and generate topological defects. Including spin gives rise to an effective magnetic field (polariton spin-orbit coupling) that acts on the topological defects—half-solitons and half-vortices—behaving as effective magnetic monopoles. We describe various techniques to create periodic potentials, that can lead to the formation of polaritonic bands and gaps with a unique flexibility. Special focus is given to topologically nontrivial bands, leading to a polariton topological insulator, based on a polariton graphene analog.
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Manchon, A., and S. Zhang. Theory of Rashba Torques. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0024.

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This chapter focuses on the theory of current-driven Rashba torque, a special type of spin–orbit mediated spin torque that requires broken spatial-inversion symmetry. This specific form of spin-orbit interaction enables the electrical generation of a non-equilibrium spin density that yields both damping-like and field-like torques on the local magnetic moments. We review the recent results obtained in (ferromagnetic and antiferromagnetic) two-dimensional electron gases, bulk magnetic semiconductors, and at the surface of topological insulators. We conclude by summarizing recent experimental results that support the emergence of Rashba torques in magnets lacking inversion symmetry.
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Valenzuela, S. O. Introduction. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0011.

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This chapter begins with a definition of spin Hall effects, which are a group of phenomena that result from spin–orbit interaction. These phenomena link orbital motion to spin direction and act as a spin-dependent magnetic field. In its simplest form, an electrical current gives rise to a transverse spin current that induces spin accumulation at the boundaries of the sample, the direction of the spins being opposite at opposing boundaries. It can be intuitively understood by analogy with the Magnus effect, where a spinning ball in a fluid deviates from its straight path in a direction that depends on the sense of rotation. spin Hall effects can be associated with a variety of spin-orbit mechanisms, which can have intrinsic or extrinsic origin, and depend on the sample geometry, impurity band structure, and carrier density but do not require a magnetic field or any kind of magnetic order to occur.
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Nagaosa, N. Multiferroics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0010.

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This chapter delves into the physics of multiferroics, the recent developments of which are discussed here from the viewpoint of the spin current and “emergent electromagnetism” for constrained systems. It presents the three sources of U(1) gauge fields, namely, the Berry phase associated with the noncollinear spin structure, the spin-orbit interaction (SOI), and the usual electromagnetic field. The chapter reviews multiferroic phenomena in noncollinear magnets from this viewpoint and discusses theories of multiferroic behavior of cycloidal helimagnets in terms of the spin current or vector spin chirality. Relativistic SOI leads to a coupling between the spin current and the electric polarization, and hence the ferroelectric and dielectric responses are a new and important probe for the spin states and their dynamical properties. Microscopic theories of the ground state polarization for various electronic configurations, collective modes including the electromagnon, and some predictions including photoinduced chirality switching are discussed with comparison to experimental results.
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Morawetz, Klaus. Interacting Systems far from Equilibrium. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198797241.001.0001.

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In quantum statistics based on many-body Green’s functions, the effective medium is represented by the selfenergy. This book aims to discuss the selfenergy from this point of view. The knowledge of the exact selfenergy is equivalent to the knowledge of the exact correlation function from which one can evaluate any single-particle observable. Complete interpretations of the selfenergy are as rich as the properties of the many-body systems. It will be shown that classical features are helpful to understand the selfenergy, but in many cases we have to include additional aspects describing the internal dynamics of the interaction. The inductive presentation introduces the concept of Ludwig Boltzmann to describe correlations by the scattering of many particles from elementary principles up to refined approximations of many-body quantum systems. The ultimate goal is to contribute to the understanding of the time-dependent formation of correlations. Within this book an up-to-date most simple formalism of nonequilibrium Green’s functions is presented to cover different applications ranging from solid state physics (impurity scattering, semiconductor, superconductivity, Bose–Einstein condensation, spin-orbit coupled systems), plasma physics (screening, transport in magnetic fields), cold atoms in optical lattices up to nuclear reactions (heavy-ion collisions). Both possibilities are provided, to learn the quantum kinetic theory in terms of Green’s functions from the basics using experiences with phenomena, and experienced researchers can find a framework to develop and to apply the quantum many-body theory straight to versatile phenomena.
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Gariglio, S., M. S. Scheurer, J. Schmalian, A. M. R. V. L. Monteiro, S. Goswami, and A. D. Caviglia. Surface and Interface Superconductivity. Edited by A. V. Narlikar. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780198738169.013.7.

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This article focuses on surface and interface superconductivity, a pivotal area of mesoscopic superconductivity. It discusses theoretical ideas regarding superconductivity in the 2D limit; pairing symmetry in systems with broken inversion symmetry and in the presence of Rashba spin–orbit interaction; and coupling of substrate phonon modes to layer electronic states to induce or enhance the superconducting condensate. It also reviews the experimental ongoing efforts to fabricate, characterize, and measure these systems, with particular emphasis on oxide materials. Superconductivity in two dimensions, in ultra-thin metals on Si(111), and at the LaAlO3/SrTiO3 interface is examined. The article concludes with an analysis of theoretical propositions aimed at realizing and testing novel superconducting states occurring at the surfaces and interfaces.
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Book chapters on the topic "Interactions spin-orbit"

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Winter, Othon C., and Wagner Sessin. "Nebular Drag and Capture into Spin-Orbit Resonance." In Interactions Between Physics and Dynamics of Solar System Bodies, 329–39. Dordrecht: Springer Netherlands, 1993. http://dx.doi.org/10.1007/978-94-011-1902-3_27.

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Hauser, Andreas W., Gerald Auböck, and Wolfgang E. Ernst. "Jahn–Teller Effect and Spin-Orbit Coupling in Heavy Alkali Trimers." In Vibronic Interactions and the Jahn-Teller Effect, 301–16. Dordrecht: Springer Netherlands, 2011. http://dx.doi.org/10.1007/978-94-007-2384-9_16.

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Celletti, Alessandra. "Stability of the Synchronous Spin-Orbit Resonance by Construction of Librational Trapping Tori." In Interactions Between Physics and Dynamics of Solar System Bodies, 325–28. Dordrecht: Springer Netherlands, 1993. http://dx.doi.org/10.1007/978-94-011-1902-3_26.

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Aremua, I., E. Baloïtcha, and M. N. Hounkonnou. "Supersymmetric Vector Coherent States for Systems with Zeeman Coupling and Spin-Orbit Interactions." In Trends in Mathematics, 113–26. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-18212-4_7.

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Kastberg, Anders. "The Spin–Orbit Interaction." In Structure of Multielectron Atoms, 57–65. Cham: Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-36420-5_4.

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Tilson, Jeffrey L., and Walter C. Ermler. "Massively parallel spin–orbit configuration interaction." In Highlights in Theoretical Chemistry, 91–99. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-662-48148-6_8.

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Matsika, Spiridoula, and David R. Yarkony. "Conical Intersections and the Spin-Orbit Interaction." In Advances in Chemical Physics, 557–81. New York, USA: John Wiley & Sons, Inc., 2003. http://dx.doi.org/10.1002/0471433462.ch10.

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Condon, E. U., and H. Odabasi. "Spin-Orbit Interaction In Self-Consistent Fields." In Selected Scientific Papers of E.U. Condon, 604–20. New York, NY: Springer New York, 1991. http://dx.doi.org/10.1007/978-1-4613-9083-1_46.

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Korostil, A. M., and M. M. Krupa. "Magnetization in Nanostructures with Strong Spin–Orbit Interaction." In Springer Proceedings in Physics, 35–102. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-18543-9_4.

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Ambrosetti, A., F. Pederiva, E. Lipparini, and L. Mitas. "Quantum Monte Carlo in Presence of Spin-Orbit Interaction." In ACS Symposium Series, 119–30. Washington, DC: American Chemical Society, 2012. http://dx.doi.org/10.1021/bk-2012-1094.ch010.

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Conference papers on the topic "Interactions spin-orbit"

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Götte, Jörg B., and Mark R. Dennis. "Spin-orbit interactions in vortex singularimetry." In SPIE NanoScience + Engineering, edited by Henri-Jean Drouhin, Jean-Eric Wegrowe, and Manijeh Razeghi. SPIE, 2013. http://dx.doi.org/10.1117/12.2022760.

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Shiraishi, Masashi. "Gate-tuned spin-orbit interactions in solids." In Spintronics XIV, edited by Henri-Jean M. Drouhin, Jean-Eric Wegrowe, and Manijeh Razeghi. SPIE, 2021. http://dx.doi.org/10.1117/12.2597048.

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Panda, Gaurab, Ryan S. Aridi, Haozhi Dong, Virginia M. Ayres, and Harry C. Shaw. "Coupled Spin-Orbit Interactions in Flying Qubit Architectures." In 2021 IEEE 21st International Conference on Nanotechnology (NANO). IEEE, 2021. http://dx.doi.org/10.1109/nano51122.2021.9514285.

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Forbes, Kayn A., and David L. Andrews. "Optical spin-orbit interactions in molecular scattering of twisted light." In Complex Light and Optical Forces XIII, edited by David L. Andrews, Enrique J. Galvez, and Jesper Glückstad. SPIE, 2019. http://dx.doi.org/10.1117/12.2509390.

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Bliokh, Konstantin Y., Miguel A. Alonso, and Elena A. Ostrovskaya. "Angular momentum of light revisited: spin-orbit interactions in free space." In SPIE OPTO, edited by David L. Andrews, Enrique J. Galvez, and Jesper Glückstad. SPIE, 2011. http://dx.doi.org/10.1117/12.873818.

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Lee, Gun-Yeal, Jangwoon Sung, and Byoungho Lee. "Dielectric metasurfaces for arbitrary engineering of multi-channel spin-orbit interactions." In Photonic Fiber and Crystal Devices: Advances in Materials and Innovations in Device Applications XIV, edited by Shizhuo Yin and Ruyan Guo. SPIE, 2020. http://dx.doi.org/10.1117/12.2568381.

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Kunihashi, Y., H. Sanada, H. Gotoh, K. Onomitsu, M. Kohda, J. Nitta, and T. Sogawa. "Anisotropic spin dynamics of drifting electrons with coexistence of Rashba and Dresselhaus spin-orbit interactions." In 2014 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2014. http://dx.doi.org/10.7567/ssdm.2014.m-2-2.

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Rodriguez Fortuno, Francisco J. "Spin-orbit interactions of light: Fundamentals and experimental works in spin-momentum locking of evanescent waves." In 2016 Progress in Electromagnetic Research Symposium (PIERS). IEEE, 2016. http://dx.doi.org/10.1109/piers.2016.7734546.

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Yasui, Shigehiro, Chandrasekhar Chatterjee, and Muneto Nitta. "Effects of Strong Magnetic Fields on Neutron 3P2 Superfluidity with Spin–Orbit Interactions." In Proceedings of the 8th International Conference on Quarks and Nuclear Physics (QNP2018). Journal of the Physical Society of Japan, 2019. http://dx.doi.org/10.7566/jpscp.26.024022.

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Bhandari, Ramesh. "Spin Orbit and Contact Interactions in Orbital Angular Momentum Modes in a Fiber." In Frontiers in Optics. Washington, D.C.: OSA, 2019. http://dx.doi.org/10.1364/fio.2019.jw4a.122.

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Reports on the topic "Interactions spin-orbit"

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Lu, Tzu-Ming, Leon Maurer, Ezra Bussmann, Charles Thomas Harris, Lisa A. Tracy, and Keshab Raj Sapkota. Engineering Spin-Orbit Interaction in Silicon. Office of Scientific and Technical Information (OSTI), September 2018. http://dx.doi.org/10.2172/1475504.

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Das, Tanmoy. Interaction induced staggered spin-orbit order in two-dimensional electron gas. Office of Scientific and Technical Information (OSTI), June 2012. http://dx.doi.org/10.2172/1043015.

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Danilov, V., V. Ptitsyn, and T. Gorlov. Creating intense polarized electron beam via laser stripping and spin-orbit interaction. Office of Scientific and Technical Information (OSTI), December 2010. http://dx.doi.org/10.2172/1013524.

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Agassi, D. Y., and J. B. Restorff. Pseudopotential Band Calculations along a High-Symmetry Axis. Part 2. Spin-Orbit Interaction and the (111) Direction. Fort Belvoir, VA: Defense Technical Information Center, July 1991. http://dx.doi.org/10.21236/ada252397.

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Polarization Possibilities of Small Spin-Orbit Interaction in Strained-Superlattice Photocathodes. Office of Scientific and Technical Information (OSTI), August 2010. http://dx.doi.org/10.2172/992984.

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