Livres : « Spin effect »

1

Teana, Francesco La. La nascita dello spin. Napoli : Bibliopolis, 2005.

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2

Wolf, Michael Johannes. Spin Transport and Proximity Effect in Nanoscale Superconductor Hybrid Structures. [S.l : s.n.], 2013.

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3

Buchachenko, A. L. Magnetic isotope effect in chemistry and biochemistry. Hauppauge, NY : Nova Science Publishers, 2009.

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4

Allsworth, Max Daniel. The effect of spin-polarised electrons on superconductivity in a ferromagnet superconductor bilayer. Birmingham : University of Birmingham, 2002.

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5

Salikhov, K. M. Magnetic isotope effect in radical reactions : An introduction. Wien : Springer, 1996.

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6

Magnetic Compton scattering : An application to spin-dependent momentum distribution in RFe₂ compounds. Białystok [Poland] : Dział Wydawnictw Filii Uniwersytetu Warszawskiego w Białymstoku, 1996.

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7

Takayama, Akari. High-Resolution Spin-Resolved Photoemission Spectrometer and the Rashba Effect in Bismuth Thin Films. Tokyo : Springer Japan, 2015. http://dx.doi.org/10.1007/978-4-431-55028-0.

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8

Free radicals : Biology and detection by spin trapping. New York : Oxford University Press, 1999.

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9

Stough, H. Paul. Flight investigation of the effect of tail configuration on stall, spin, and recovery characteristics of a low-wing general aviation research airplane. Hampton, Va : Langley Research Center, 1987.

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10

Stough, H. Paul. Flight investigation of the effect of tail configuration on stal, spin, and recovery characteristics of a low-wing general aviation research airplane. [Washington, DC] : National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1987.

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11

Stough, H. Paul. Flight investigation of the effect of tail configuration on stal, spin, and recovery characteristics of a low-wing general aviation research airplane. [Washington, DC] : National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1987.

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12

Peter, Blümel, et Ranke Michael B, dir. Growth hormone over the human life span. Heidelberg : Barth, 1998.

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13

Winkler, Roland. Spin--Orbit Coupling Effects in Two-Dimensional Electron and Hole Systems. Berlin, Heidelberg : Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/b13586.

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14

Winkler, Roland. Spin-orbit coupling effects in two-dimensional electron and hole systems. Berlin : Springer, 2003.

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15

1946-, Maekawa S., et Shinjō Teruya 1938-, dir. Spin dependent transport in magnetic nanostructures. Boca Raton : CRC Press, 2002.

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16

RCNP International Symposium on Nuclear Responses and Medium Effects (2nd 1998 Osaka, Japan). Nuclear responses and medium effects : Proceedings of the RCNP International Symposium on Nuclear Responses and Medium Effects, Osaka, Japan, November 26-28, 1998. Tokyo, Japan : Universal Academy Press, 1999.

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17

Hawkes, C. V. The effect of spine pre-heating on hot melt binding. [Leatherhead] : Pira,Printing & InformationTechnology Division, 1988.

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18

Spin-pumping effects in ferromagnetic thin film heterostructures measured through ferromagnetic resonance. [New York, N.Y.?] : [publisher not identified], 2022.

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19

B, Sheridan Thomas, et Ames Research Center, dir. Effect of time span and task load on pilot mental workload. Cambridge, Mass : Man-Machine Systems Laboratory, Dept. of Mechanical Engineering, Massachusetts Institute of Technology, 1985.

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20

S, Maekawa, et Shinjo Teruya 1938-, dir. Spin dependent transport in magnetic nanostructures. London : Taylor & Francis, 2002.

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21

Thompson, Roy C. Life-span effects of ionizing radiation in the beagle dog. [Oak Ridge, Tenn.] : Office of Scientific and Technical Information, U.S. Dept. of Energy, 1989.

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22

Marek, Szpalski, et Gunzburg Robert, dir. The failed spine. Philadelphia : Lippincott Williams & Willkins, 2005.

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23

Introduction to dynamic spin chemistry : Magnetic field effects on chemical and biochemical reactions. Singapore : World Scientific, 2004.

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24

Amnon, Kohen, et Limbach Hans-Heinrich, dir. Isotope effects in chemistry and biology. Boca Raton : Taylor & Francis, 2006.

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25

Takahashi, S., et S. Maekawa. Spin Hall Effect. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0012.

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This chapter discusses the spin Hall effect that occurs during spin injection from a ferromagnet to a nonmagnetic conductor in nanostructured devices. This provides a new opportunity for investigating AHE in nonmagnetic conductors. In ferromagnetic materials, the electrical current is carried by up-spin and downspin electrons, with the flow of up-spin electrons being slightly deflected in a transverse direction while that of down-spin electrons being deflected in the opposite direction; this results in an electron flow in the direction perpendicular to both the applied electric field and the magnetization directions. Since up-spin and downspin electrons are strongly imbalanced in ferromagnets, both spin and charge currents are generated in the transverse direction by AHE, the latter of which are observed as the electrical Hall voltage.

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26

Uchida, K., R. Ramos et E. Saitoh. Spin Seebeck effect. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0018.

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Chapter 18 This chapter discusses the spin Seebeck effect (SSE), which stands for the generation of a spin current, a flow of spinangular momentum, as a result of a temperature gradient in magnetic materials. In spintronics and spin caloritronics, the SSE is of crucial importance because it enables simple and versatile generation of a spin current from heat. Since the SSE is driven by thermally excited magnon dynaimcs, the thermal spin current can be generated not only from ferromagnetic conductors but also from insulators. Therefore, the SSE is applicable to “insulator-based thermoelectric conversion” which was impossible if only conventional thermoelectric technologies were used. In this chapter, after introducing basic characteristics and mechanisms of the SSE, important experimental progresses, such as the high-magnetic-field response of the SSE and the enhancement of the SSE in multilayer systems, are reviewed.

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27

Wunderlich, J., K. Olejník, L. P. Zârbo, V. P. Amin, J. Sinova et T. Jungwirth. Spin-injection Hall effect. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0016.

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This chapter discusses the Spin-injection Hall effect (SiHE), another member of the spin-dependent Hall effects that is closely related to the anomalous Hall effect (AHE), the spin Hall effect (SHE), and the inverse spin Hall effect (iSHE). The microscopic origins responsible for the appearance of spin-dependent Hall effects are due to the spin-orbit (SO) coupling-related asymmetrical deflections of spin carriers. Depending on the relative strength of the SO coupling compared to the energy-level broadening of the quasi-particle states due to disorder scattering, scattering-related extrinsic mechanisms or intrinsic band structure-related deflection dominate the spin-dependent Hall response. Both the iSHE and the SiHE require spin injection into a nonmagnetic system. Similar to the AHE, a spin-polarized charge current flows in the case of the SiHE and the SO coupling generates the spin-dependent Hall signal.

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28

Saitoh, E., et K. Ando. Experimental observation of the spin Hall effect using spin dynamics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0015.

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This chapter describes an experiment on the inverse spin Hall effect (ISHE) induced by spin pumping. Spin pumping is the generation of spin currents as a result of magnetization M(t) precession; in a ferromagnetic/paramagnetic bilayer system, a conduction-electron spin current is pumped out of the ferromagnetic layer into the paramagnetic conduction layer in a ferromagnetic resonance condition. The sample used in the experiment is a Ni81Fe19/Pt bilayer film comprising a 10-nm-thick ferromagnetic Ni81Fe19layer and a 10-nm-thick paramagnetic Pt layer. For the measurement, the sample system is placed near the centre of a TE011 microwave cavity at which the magnetic-field component of the microwave mode is maximized while the electric-field component is minimized.

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29

Murakami, S., et T. Yokoyama. Quantum spin Hall effect and topological insulators. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0017.

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This chapter begins with a description of quantum spin Hall systems, or topological insulators, which embody a new quantum state of matter theoretically proposed in 2005 and experimentally observed later on using various methods. Topological insulators can be realized in both two dimensions (2D) and in three dimensions (3D), and are nonmagnetic insulators in the bulk that possess gapless edge states (2D) or surface states (3D). These edge/surface states carry pure spin current and are sometimes called helical. The novel property for these edge/surface states is that they originate from bulk topological order, and are robust against nonmagnetic disorder. The following sections then explain how topological insulators are related to other spin-transport phenomena.

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30

Brataas, A., Y. Tserkovnyak, G. E. W. Bauer et P. J. Kelly. Spin pumping and spin transfer. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0008.

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This chapter discusses the interaction between currents and magnetization, which can cause undesirable effects such as enhanced magnetic noise in read heads made from magnetic multilayers. While most research has been carried out on metallic structures, current-induced magnetization dynamics in semiconductors or even insulators has been pursued as well. These issues have attracted many physicists because, on top of the practical aspects, the underlying phenomena are fascinating. Berger and Slonczewski are acknowledged to have started the field in general through their introduction of the concept of current-induced magnetization dynamics by the transfer of spin. The reciprocal effect, i.e., spin pumping, was expected long ago, but it took some time before Tserkovnyak et al. developed a rigorous theory of spin pumping for magnetic multilayers, including the associated increased magnetization damping.

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31

Angle And Spin Resolved Auger Emission Theory And Applications To Atoms And Molecules. Springer, 2008.

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32

Valenzuela, S. O., et T. Kimura. Experimental observation of the spin Hall effect using electronic nonlocal detection. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0014.

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This chapter shows how the spin Hall effect (SHE) has been described as a source of spin-polarized electrons for electronic applications without the need for ferromagnets or optical injection. Because spin accumulation does not produce an obvious measurable electrical signal, electronic detection of the SHE proved to be elusive and was preceded by optical demonstrations. Several experimental schemes for the electronic detection of the SHE had been originally proposed, including the use of ferromagnetic electrodes to determine the spin accumulation at the edges of the sample. However, the difficulty of sample fabrication and the presence of spin-related phenomena such as anisotropic magnetoresistance or the anomalous Hall effect in the ferromagnetic electrodes could mask or even mimic the SHE signal in the sample layouts.

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33

Takanashi, K., et Y. Sakuraba. Spin polarization in magnets. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0005.

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This chapter explains how the exchange splitting between up- and down-spin bands in ferromagnets unexceptionally generates spin-polarized electronic states at the Fermi energy. The quantity of spin polarization P in ferromagnets is one of the important parameters for application in spintronics, since a ferromagnet having a higher P is able to generate larger various spin-dependent effects such as the magnetoresistance effect, spin transfer torque, spin accumulation, and so on. However, the spin polarizations of general 3d transition metals or alloys generally limit the size of spin-dependent effects. Thus,“‘half-metals” attract much interest as an ideal source of spin current and spin-dependent scattering because they possess perfectly spin-polarized conduction electrons due to the energy band gap in either the up- or down-spin channel at the Fermi level.

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34

Lohmann, Bernd. Angle and Spin Resolved Auger Emission : Theory and Applications to Atoms and Molecules. Springer Berlin / Heidelberg, 2010.

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35

Lohmann, Bernd. Angle and Spin Resolved Auger Emission : Theory and Applications to Atoms and Molecules. Springer London, Limited, 2008.

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36

Maekawa, Sadamichi, Sergio O. Valenzuela, Eiji Saitoh et Takashi Kimura, dir. Spin Current. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.001.0001.

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Since the discovery of the giant magnetoresistance effect in magnetic multilayers in 1988, a new branch of physics and technology, called spin-electronics or spintronics, has emerged, where the flow of electrical charge as well as the flow of electron spin, the so-called “spin current,” are manipulated and controlled together. The physics of magnetism and the application of spin current have progressed in tandem with the nanofabrication technology of magnets and the engineering of interfaces and thin films. This book aims to provide an introduction and guide to the new physics and applications of spin current, with an emphasis on the interaction between spin and charge currents in magnetic nanostructures.

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37

Kimura, T. Introduction of spin torques. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0019.

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This chapter discusses the spin-transfer effect, which is described as the transfer of the spin angular momentum between the conduction electrons and the magnetization of the ferromagnet that occurs due to the conservation of the spin angular momentum. L. Berger, who introduced the concept in 1984, considered the exchange interaction between the conduction electron and the localized magnetic moment, and predicted that a magnetic domain wall can be moved by flowing the spin current. The spin-transfer effect was brought into the limelight by the progress in microfabrication techniques and the discovery of the giant magnetoresistance effect in magnetic multilayers. Berger, at the same time, separately studied the spin-transfer torque in a system similar to Slonczewski’s magnetic multilayered system and predicted spontaneous magnetization precession.

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38

Glazov, M. M. Spin Systems in Semiconductor Nanostructures. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0002.

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This chapter is an introduction to a rich variety of effects taking place in the interacting system of electrons and nuclei in semiconductors. It includes also the basics of electronic properties of nanostructures and of spin physics, an overview of fundamental interactions in the electron and nuclear spin systems, the selection rules at optical transitions in semiconductors, spin resonance effect, as well as optical orientation, and dynamical nuclear polarization. In this chapter an analysis of particular features of spin dynamics arising in the structures with localized electrons such as quantum dots, which are studied further in the book, are addressed. The aim of this chapter is to provide basic minimum of information needed to read the remaining chapters.

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39

Sun, Kenneth Cheung-Ping. Synthesis and low-temperature Mossbauer effect investigation of intermediate-spin halobis (N,N'-dialkyldithiocarbamato) iron (III) complexes. 1985.

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40

Sun, Kenneth Cheung-Ping. Synthesis and low-temperature Mossbauer effect investigation of intermediate-spin halobis (N,N'-dialkyldithiocarbamato) iron (III) complexes. 1985.

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41

Cardona, M., et G. Güntherodt. Light Scattering in Solids IV : Electronic Scattering, Spin Effects, SERS, and Morphic Effects. Springer London, Limited, 2014.

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42

Glazov, M. M. Electron Spin Relaxation Beyond the Hyperfine Interaction. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0008.

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Here, some prospects for future studies in the field of electron and nuclear spin dynamics are outlined. In contrast to previous chapters where the electron interaction with multitude of nuclei was discussed, in Chapter 8 particular emphasis is put on a situation where hyperfine interaction is so strong that it leads to a qualitative rear rangement of the energy spectrum resulting in coherent excitation transfer between electron and nucleus. The strong coupling between the spin of the charge carrier and of the nucleus is realized; e.g., in the case of deep impurity centers in semiconductors or in isotopically purified systems. We also discuss the effect of the nuclear spin polaron; that is, the ordered state, where the carrier spin orientation results in alignment of spins of the nucleus interacting with the electron or hole. Such problems have been briefly discussed in the literature but, in our opinion, call for in-depth investigation.

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43

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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44

Takayama, Akari. High-Resolution Spin-Resolved Photoemission Spectrometer and the Rashba Effect in Bismuth Thin Films. Springer, 2014.

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45

Takayama, Akari. High-Resolution Spin-Resolved Photoemission Spectrometer and the Rashba Effect in Bismuth Thin Films. Springer, 2016.

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46

Takayama, Akari. High-Resolution Spin-Resolved Photoemission Spectrometer and the Rashba Effect in Bismuth Thin Films. Springer Japan, 2014.

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47

Glazov, M. M. Dynamical Nuclear Polarization. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0005.

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The transfer of nonequilibrium spin polarization between the electron and nuclear subsystems is studied in detail. Usually, a thermal orientation of nuclei in magnetic field is negligible due to their small magnetic moments, but if electron spins are optically oriented, efficient nuclear spin polarization can occur. The microscopic approach to the dynamical nuclear polarization effect based on the kinetic equation method, along with a phenomenological but very powerful description of dynamical nuclear polarization in terms of the nuclear spin temperature concept is given. In this way, one can account for the interaction between neighbouring nuclei without solving a complex many-body problem. The hyperfine interaction also induces the feedback of polarized nuclei on the electron spin system giving rise to a number of nonlinear effects: bistability of nuclear spin polarization and anomalous Hanle effect, dragging and locking of optical resonances in quantum dots. Theory is illustrated by experimental data on dynamical nuclear polarization.

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48

Glazov, M. M. Strong Coupling of Electron and Nuclear Spins : Outlook and Prospects. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0011.

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In this chapter, some prospects in the field of electron and nuclear spin dynamics are outlined. Particular emphasis is put ona situation where the hyperfine interaction is so strong that it leads to a qualitative rearrangement of the energy spectrum resulting in the coherent excitation transfer between the electron and nucleus. The strong coupling between the spin of the charge carrier and of the nucleus is realized, for example in the case of deep impurity centers in semiconductors or in isotopically purified systems. We also discuss the effect of the nuclear spin polaron, that is ordered state, formation at low enough temperatures of nuclear spins, where the orientation of the carrier spin results in alignment of the spins of nucleus interacting with the electron or hole.

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49

Cao, Gang, et 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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50

Nikolic, Branislav K., Liviu P. Zarbo et Satofumi Souma. Spin currents in semiconductor nanostructures : A non-equilibrium Green-function approach. Sous la direction de A. V. Narlikar et Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533046.013.24.

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This article examines spin currents and spin densities in realistic open semiconductor nanostructures using different tools of quantum-transport theory based on the non-equilibrium Green function (NEGF) approach. It begins with an introduction to the essential theoretical formalism and practical computational techniques before explaining what pure spin current is and how pure spin currents can be generated and detected. It then considers the spin-Hall effect (SHE), and especially the mesoscopic SHE, along with spin-orbit couplings in low-dimensional semiconductors. It also describes spin-current operator, spindensity, and spin accumulation in the presence of intrinsic spin-orbit couplings, as well as the NEGF approach to spin transport in multiterminal spin-orbit-coupled nanostructures. The article concludes by reviewing formal developments with examples drawn from the field of the mesoscopic SHE in low-dimensional spin-orbit-coupled semiconductor nanostructures.

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