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Books on the topic 'Spin polarised'

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Published: 4 June 2021
Last updated: 31 January 2023

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1

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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2

Evans, Myron W. Electron spin and nuclear magnetic resonance in the presence of a circularly polarised laser: Angular momentum of radiation. Ithaca, N.Y: Cornell Theory Center, Cornell University, 1991.

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3

Samarin, Sergey, Oleg Artamonov, and Jim Williams. Spin-Polarized Two-Electron Spectroscopy of Surfaces. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-030-00657-0.

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4

Crabb, D. G. (Don G.), ed. Spin physics: 18th International Spin Physics Symposium, Charlottesville, Virginia, 6-11 October 2008. Melville, N.Y: American Institute of Physics, 2009.

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5

International Spin Physics Symposium (14th 2000 Osaka, Japan). SPIN 2000: 14th International Spin Physics Symposium, Osaka, Japan, 16-21 October 2000. Edited by Hatanaka K and American Institute of Physics. Melville, N.Y: American Institute of Physics, 2001.

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6

P, Derenchuk Vladimir, and Von Przewoski Barbara, eds. Proceedings of the Ninth International Workshop Polarized Sources and Targets: Nashville, Indiana, USA, 30 September-4 October 2001. River Edge, N.J: World Scientific, 2002.

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7

Conference on Spin Polarized Quantum Systems (1988 Torino, Italy). Spin polarized quantum systems: June 20-24, 1988, Villa Gualino, Torino. Edited by Stingari S, Institute for Scientific Interchange, and Università degli studi di Trento. Dipartimento di fisica. Singapore: World Scientific, 1989.

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8

F, Bradamante, and Workshop on Polarized Electron Sources and Polarimeters (2004 : Trieste, Italy), eds. SPIN 2004: Proceedings of the 16th International Spin Physics Symposium and Workshop on Polarized Electron Sources and Polarimeters, Trieste, Italy, 10-16 October 2004. Hackensack, N.J: World Scientific, 2005.

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9

International Workshop on Polarized Ion Sources, Targets and Polarimetry (13th 2009 Ferrara, Italy). Polarized sources, targets and polarimetry: Proceedings of the 13th International Workshop, Ferrara, Italy, 7 - 11 September 2009. New Jersey: World Scientific, 2011.

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10

International, Spin Physics Symposium (15th 2002 Upton N. Y. ). Spin 2002: 15th International Spin Physics Symposium, Upton, New York, 9-14 September 2002 and, Workshop on Polarized Electron Sources and Polarimeters, Danvers, Massachusetts 4-6 September 2002. Melville, N.Y: American Institute Of Physics, 2003.

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11

International Workshop on the Spin Structure of the Proton and Polarized Collider Physics (2001 Trento, Italy). The spin structure of the proton and polarized collider physics: Proceedings of the International Workshop on the Spin Structure of the Proton and Polarized Collider Physics : Trento, Italy, 23-28 July 2001. [Amsterdam]: North-Holland, 2002.

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12

Japan) International Spin Physics Symposium (17th 2006 Kyoto. Proceedings of the 17th International Spin Physics Symposium, Kyoto, Japan, 2-7 October 2006. Edited by Imai Kenʼichi 1946-. Melville, N.Y: American Institute of Physics, 2007.

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13

G, Crabb D., Day Donal B, and Chen J. P, eds. Testing QCD through spin observables in nuclear targets: University of Virginia, USA : April 18-20, 2002. River Edge, N.J: World Scientific, 2003.

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14

International Symposium on High Energy Spin Physics (10th 1992 Nagoya, Japan). Frontiers of high energy spin physics: Proceedings of the 10th International Symposium on High Energy Spin Physics (Yamada Conference XXXV), November 9-14, 1992, Nagoya, Japan. Tokyo, Japan: Universal Academy Press, 1993.

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15

Y, Onel, Paver N, Penzo A, Unesco, International Centre for Theoretical Physics., and International Atomic Energy Agency, eds. Proceedings of the Adriatico Research Conference on trends in collider spin physics: ICTP, Trieste, Italy 5-8 December 1995. Singapore: World Scientific, 1997.

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16

de, Jager C. W., ed. SPIN96: Proceedings : 12th International Symposium on High-Energy Spin Physics, September 10-14, 1996, Amsterdam, The Netherlands. Singapore: River Edge, N.J., 1997.

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17

Nakamura, Katsuro. Longitudinal Double-Spin Asymmetry of Electrons from Heavy Flavor Decays in Polarized p + p Collisions at √s = 200 GeV. Tokyo: Springer Japan, 2014. http://dx.doi.org/10.1007/978-4-431-54616-0.

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18

Dee, Philip R. A study of the spin dependency of elastic scattering of [polarized] [superior 6]Li on [superior 58]Ni at 70.5MeV. Birmingham: University of Birmingham, 1993.

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19

Smith, Timothy John. The application of spin polarised neutron scattering to superconductors. 1999.

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20

Kavokin, Alexey V., Jeremy J. Baumberg, Guillaume Malpuech, and Fabrice P. Laussy. Spin and polarisation. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198782995.003.0009.

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In this chapter we consider a complex set of optical phenomena linked to the spin dynamics of exciton-polaritons in semiconductor microcavities. We review a few important experiments that reveal the main mechanisms of the exciton-polariton spin dynamics and present the theoretical model of polariton spin relaxation based on the density matrix formalism. We also discuss the polarisation properties of the condensate and the superfluid phase transitions for polarised exciton-polaritons. We briefly address the polarization multistability and switching in polariton lasers. Finally, the optical spin-Hall and spin-Meissner effects are described.
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21

McClintock, P. V. E., A. M. Goldman, M. Springford, and Meyerovich. Spin-Polarized Qntm Systms. University of Cambridge ESOL Examinations, 1999.

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22

Suzuki, Y. Spin torque in uniform magnetization. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0020.

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This chapter discusses the effects of a spin current injected into a uniformly magnetized ferromagnetic cell. The junction consists of two ferromagnetic layers separated by a nonmagnetic metal interlayer or insulating barrier layer. With a nonmagnetic metal interlayer, the junction is called a giant magnetoresistive nanopillar, and with an insulating barrier layer a magnetic-tunnel junction. When charge current is passed through this device, the electrons are first spin polarized by the fixed layer and spin-polarized current is then injected into the free layer through the nonmagnetic interlayer. This spin current interacts with the spins in the host material by an exchange interaction and exerts a torque. If the exerted torque is large enough, magnetization in the free layer is reversed or continuous precession is excited.
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23

Hirohata, A., and J. Y. Kim. Optically Induced and Detected Spin Current. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0006.

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This chapter presents an alternative method of injecting spin-polarized electrons into a nonmagnetic semiconductor through photoexcitation. This method uses circularly-polarized light, whose energy needs to be the same as, or slightly larger than, the semiconductor band-gap, to excite spin-polarized electrons. This process will introduce a spin-polarized electron-hole pair, which can be detected as electrical signals. Such an optically induced spin-polarized current can only be generated in a direct band-gap semiconductor due to the selection rule described in the following sections. This introduction of circularly polarized light can also be used for spin-polarized scanning tunnelling microscopy.
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24

Glazov, M. M. Interaction of Spins with Light. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0006.

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This chapter presents the details of the optical manipulation of electron spin states. It also addresses manifestations of the electron and nuclear spin dynamics in optical response of semiconductor nanostructures via spin-Faraday and -Kerr effects. Coupling of spins with light provides the most efficient method of nonmagnetic spin manipulation. The main aim of this chapter is to provide the theoretical grounds for optical spin injection, ultrafast spin control, and readout of spin states by means of circularly and linearly polarized light pulses. The Faraday and Kerr effects induced by the electron and nuclear spin polarization are analyzed both by means of a macroscopic, semi-phenomenological approach and by using the microscopic quantum mechanical model. Theoretical analysis is supported by experimental data.
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25

(Editor), Kichiji Hatanaka, Takashi Nakano (Editor), Kenichi Imai (Editor), and Hiroyasu Ejiri (Editor), eds. Spin 2000. American Institute of Physics, 2001.

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26

Samarin, Sergey, Oleg Artamonov, and Jim Williams. Spin-Polarized Two-Electron Spectroscopy of Surfaces. Springer, 2019.

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27

Samarin, Sergey, Oleg Artamonov, and Jim Williams. Spin-Polarized Two-Electron Spectroscopy of Surfaces. Springer, 2018.

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28

Kimura, T., and Y. Otani. Magnetization switching due to nonlocal spin injection. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0021.

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This chapter discusses and presents a schematic illustration of nonlocal spin injection. In this case, the spin-polarized electrons are injected from the ferromagnet and are extracted from the left-hand side of the nonmagnet. This results in the accumulation of nonequilibrium spins in the vicinity of the F/N junctions. Since the electrochemical potential on the left-hand side is lower than that underneath the F/N junction, the electron flows by the electric field. On the right-hand side, although there is no electric field, the diffusion process from the nonequilibrium into the equilibrium state induces the motion of the electrons. Since the excess up-spin electrons exist underneath the F/N junction, the up-spin electrons diffuse into the right-hand side. On the other hand, the deficiency of the down-spin electrons induces the incoming flow of the down-spin electrons opposite to the motion of the up-spin electron.
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29

Takanashi, K., and 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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30

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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31

(Editor), Vladimir P. Derenchuk, and Barbara Von Przewoski (Editor), eds. Polarized Sources and Targets. World Scientific Publishing Company, 2002.

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32

Aulenbacher, Kurt, Italy) Spin 200 (2004 Trieste, and Workshop on Polarized Electron Sources A. Spin 2004: 16th International Spin Physics Symposium; Workshop On Polerized Electron Sources and Polarimeters. World Scientific Publishing Company, 2005.

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33

(Editor), Tomohiro Uesaka, Hideyuki Sakai (Editor), Akihiro Yoshimi (Editor), and Koichiro Asahi (Editor), eds. Polarized Sources and Targets: Proceedings of the 11th International Workshop. World Scientific Publishing Company, 2007.

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34

Glazov, M. M. Electron Spin Precession Mode Locking and Nuclei-Induced Frequency Focusing. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0009.

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This chapter addresses a rich variety of effects in spin dynamics arising under the conditions of pump-probe experiments. Here we consider the case where the electron spin is injected by a periodic train of circularly polarized pump pulses and precesses between the pulses in an external magnetic field. Nontrivial effects such as resonant spin amplification and spin coherence mode-locking take place due to commensurability of the repetition period of pump pulses and the charge carrier spin precession period. Theoretical approaches to describing the electron and nuclear spin coherence and experimental manifestations of these unusual regimes of spin dynamics are discussed in detail.
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35

Spin Polarized Quantum Systems: June 20-24, 1988, Villa Gualino, Torino. World Scientific Pub Co Inc, 1989.

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36

Ansermet, J. Ph. Spintronics with metallic nanowires. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533060.013.3.

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This article focuses on spintronics with metallic nanowires. It begins with a review of the highlights of spintronics research, paying attention to the very important developments accomplished with tunnel junctions. It then considers the effect of current on magnetization before discussing spin diffusion and especially spin-dependent conductivities, spin-diffusion lengths, and spin accumulation. It also examines models for spin-polarized currents acting on magnetization, current-induced magnetization switching, and current-driven magnetic excitations. It concludes with an overview of resonant-current excitations, with emphasis on spin-valves and tunnel junctions as well as resonant excitation of spin-waves, domain walls and vortices. In addition, the article reflects on the future of spintronics, citing in particular the potential of the spin Hall effect as the method of generating spin accumulation, free of charge accumulation.
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37

Highenergy Nuclear Optics Of Polarized Particles. World Scientific Publishing Company, 2012.

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38

Wunderlich, J., K. Olejník, L. P. Zârbo, V. P. Amin, J. Sinova, and 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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39

Valenzuela, S. O., and 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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40

(Editor), Yousef I. Makdisi, Alfredo U. Luccio (Editor), and William W. MacKay (Editor), eds. SPIN 2002: 15th International Spin Physics Symposium and Workshop on Polarized Electron Sources and Polarimeters, Upton, NY, 9-14 September 2002 (AIP Conference Proceedings / High Energy Physics). American Institute of Physics, 2003.

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41

L, Berger Edmond, and Fermi National Accelerator Laboratory, eds. Proceedings of the Symposium on Future Polarization at Fermilab: Fermi National Accelerator Laboratory, Batavia, Illinois, June 13-14, 1988. Batavia, Ill: The Laboratory, 1988.

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42

(Editor), D. G. Crabb, Donald B. Day (Editor), and J. P. Chen (Editor), eds. Testing QDC Through Spin Observables in Nuclear Targets: University of Virginia, USA April 18-20, 2002. World Scientific Pub Co Inc, 2003.

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43

Meot, François, Haixin Huang, Vadim Ptitsyn, and Fanglei Lin. Polarized Beam Dynamics and Instrumentation in Particle Accelerators: USPAS Summer 2021 Spin Class Lectures. Springer International Publishing AG, 2022.

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44

Meot, François, Haixin Huang, Vadim Ptitsyn, and Fanglei Lin. Polarized Beam Dynamics and Instrumentation in Particle Accelerators: USPAS Summer 2021 Spin Class Lectures. Springer International Publishing AG, 2022.

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45

Burton, J. D., and E. Y. Tsymbal. Magnetoresistive phenomena in nanoscale magnetic contacts. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533046.013.18.

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This article examines magnetoresistive phenomena in nano- and atomic-size ferromagnetic metal contacts. In particular, it considers how magnetization affects the flow of electrical current in ferromagnetic materials by focusing on two major categories of magnetoresistive phenomena: the ‘spin-valve’, where the flow of spin-polarized electrical current is affected by an inhomogeneous magnetization profile, and anisotropic magnetoresistance (AMR), which involves the anisotropy of electrical transport properties with respect to the orientation of the magnetization. The article first provides an overview of ballistic transport and conductance quantization before discussing domain-wall magnetoresistance at the nanoscale. It also describes AMR in magnetic nanocontacts as well as tunnelling anisotropic magnetoresistance in broken contacts.
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46

H, Althoff K., and International Symposium on High Energy Spin Physics (9th : 1990 : Bonn, Germany), eds. High energy spin physics: Proceedings of the 9th International Symposium, held at Bonn, 10-15 September 1990. Berlin: Springer-Verlag., 1991.

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47

Classical and Quantic Periodic Motions of Multiply Polarized Spin-Particles (Research Notes in Mathematics Series). Chapman & Hall/CRC, 1997.

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48

Fromme, Bärbel. D-D Excitations in Transition-Metal Oxides: A Spin-Polarized Electron Energy-Loss Spectroscopy Study. Springer, 2007.

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49

Jager, C. W. De, J. E. J. Oberski, and P. J. Mulders. Proceedings of the 12th International Symposium on High Energy Spin Physics. World Scientific Pub Co Inc, 1997.

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50

Steffens, E., and W. Meyer. High Energy Spin Physics: Workshops : Proceedings of the 9th International Symposium Held at Bonn, Frg, 6-15 September 1990. Springer, 1991.

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