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Journal articles on the topic 'Spin effect'

Author: Grafiati

Published: 9 March 2023

Last updated: 31 July 2025

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1

DYAKONOV, M. I. "SPIN HALL EFFECT." International Journal of Modern Physics B 23, no. 12n13 (2009): 2556–65. http://dx.doi.org/10.1142/s0217979209061986.

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A review of the phenomenology of the Spin Hall Effect and related phenomena originating from the coupling between spin and charge currents by spin-orbit interaction is presented. The physical origin of various effects in spin-dependent scattering is demonstrated. A previously unknown feature of spin transport, the swapping of spin currents, is discussed.

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2

GANICHEV, S. D. "SPIN-GALVANIC EFFECT AND SPIN ORIENTATION BY CURRENT IN NON-MAGNETIC SEMICONDUCTORS." International Journal of Modern Physics B 22, no. 01n02 (2008): 113–14. http://dx.doi.org/10.1142/s0217979208046177.

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Lately, there is much interest in the use of the spin of carriers in semiconductor quantum well (QW) structures together with their charge to realize novel concepts like spintronics. The necessary conditions to develop spintronic devices are high spin polarizations in QWs and a large spin-splitting of subbands in k-space. The latter is important for the ability to control spins with an external electric field by the Rashba effect. Significant progress has been achieved recently in generating large spin polarizations, in demonstrating the Rashba splitting and also in using the splitting for man

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3

Takahashi, Saburo, and Sadamichi Maekawa. "Spin current, spin accumulation and spin Hall effect." Science and Technology of Advanced Materials 9, no. 1 (2008): 014105. http://dx.doi.org/10.1088/1468-6996/9/1/014105.

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4

Hirsch, J. E. "Spin Hall Effect." Physical Review Letters 83, no. 9 (1999): 1834–37. http://dx.doi.org/10.1103/physrevlett.83.1834.

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5

Ganichev, S. D., E. L. Ivchenko, V. V. Bel'kov, et al. "Spin-galvanic effect." Nature 417, no. 6885 (2002): 153–56. http://dx.doi.org/10.1038/417153a.

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6

Won, Rachel. "Metasurface spin effect." Nature Photonics 7, no. 11 (2013): 849. http://dx.doi.org/10.1038/nphoton.2013.302.

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7

Lee, W. "Spin Holstein effect." Physica B: Condensed Matter 194-196 (February 1994): 1537–38. http://dx.doi.org/10.1016/0921-4526(94)91268-8.

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8

SCHLIEMANN, JOHN. "SPIN HALL EFFECT." International Journal of Modern Physics B 20, no. 09 (2006): 1015–36. http://dx.doi.org/10.1142/s021797920603370x.

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The intrinsic spin Hall effect in semiconductors has developed to a remarkably lively and rapidly growing branch of research in the field of semiconductor spintronics. In this article we give a pedagogical overview on both theoretical and experimental accomplishments and challenges. Emphasis is put on the the description of the intrinsic mechanisms of spin Hall transport in III-V zinc-blende semiconductors and on the effects of dissipation.

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9

Liu, S. Y., Norman J. M. Horing, and X. L. Lei. "Inverse spin Hall effect by spin injection." Applied Physics Letters 91, no. 12 (2007): 122508. http://dx.doi.org/10.1063/1.2783254.

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10

Ignatjev V.K. "Reciprocity relations for mechanically induced spin currents in metals in a nonlinear regime." Technical Physics 68, no. 5 (2023): 656. http://dx.doi.org/10.21883/tp.2023.05.56073.258-22.

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In the Markov relaxation and locally quasi-equilibrium distribution approximation, analogues of Onzager's relations for the response functions of the spin current in the nonlinear by intense mechanical and thermodynamic effects regime were obtained by the Kubo method. Keywords: locally quasi-equilibrium distribution, spin Hamiltonian, spin current, nonlinearity, reciprocity, streintronics, spin caloritronics, Peltier spin effect, Zeebeck spin effect.

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11

Niu, Zhi Ping. "Thermoelectric effects in spin field-effect transistors." Physics Letters A 375, no. 36 (2011): 3218–22. http://dx.doi.org/10.1016/j.physleta.2011.07.018.

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12

Iguchi, R., K. Ando, E. Saitoh, and T. Sato. "Spin current study of spin glass AgMn using spin pumping effect." Journal of Physics: Conference Series 266 (January 1, 2011): 012089. http://dx.doi.org/10.1088/1742-6596/266/1/012089.

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13

VALENZUELA, SERGIO O. "NONLOCAL ELECTRONIC SPIN DETECTION, SPIN ACCUMULATION AND THE SPIN HALL EFFECT." International Journal of Modern Physics B 23, no. 11 (2009): 2413–38. http://dx.doi.org/10.1142/s021797920905290x.

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In recent years, electrical spin injection and detection has grown into a lively area of research in the field of spintronics. Spin injection into a paramagnetic material is usually achieved by means of a ferromagnetic source, whereas the induced spin accumulation or associated spin currents are detected by means of a second ferromagnet or the reciprocal spin Hall effect, respectively. This article reviews the current status of this subject, describing both recent progress and well-established results. The emphasis is on experimental techniques and accomplishments that brought about important

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14

Fedorov, Dmitry V., Martin Gradhand, Katarina Tauber, Gerrit E. W. Bauer, and Ingrid Mertig. "Seebeck effect in nanomagnets." Journal of Physics: Condensed Matter 34, no. 8 (2021): 085801. http://dx.doi.org/10.1088/1361-648x/ac3b26.

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Abstract We present a theory of the Seebeck effect in nanomagnets with dimensions smaller than the spin diffusion length, showing that the spin accumulation generated by a temperature gradient strongly affects the thermopower. We also identify a correction arising from the transverse temperature gradient induced by the anomalous Ettingshausen effect and an induced spin-heat accumulation gradient. The relevance of these effects for nanoscale magnets is illustrated by ab initio calculations on dilute magnetic alloys.

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15

Lyapilin, I. I. "Spin Hall Effect Induced by Sound." Solid State Phenomena 190 (June 2012): 117–20. http://dx.doi.org/10.4028/www.scientific.net/ssp.190.117.

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Transport of electronic spins in low-dimensional and nanoscale systems is the subject of thenovel and quickly developing eld of spintronics. The possibility of coherent spin manipulationrepresents an ultimate goal of this eld. Typically, spin transport is strongly aected by couplingof spin and orbital degrees of freedom. The inuence of the spin orbit interaction is twofold.The momentum relaxation due to the scattering of carriers, inevitably leads to spin relaxationand destroys the spin coherence. On the other hand, the controlled orbital motion of carrierscan result in a coherent motion of th

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16

Hong, Seokmin, Shehrin Sayed, and Supriyo Datta. "Spin Circuit Representation for the Spin Hall Effect." IEEE Transactions on Nanotechnology 15, no. 2 (2016): 225–36. http://dx.doi.org/10.1109/tnano.2016.2514410.

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17

Basu, B., and P. Bandyopadhyay. "Spin–orbit gauge and quantum spin Hall effect." Physics Letters A 373, no. 1 (2008): 148–51. http://dx.doi.org/10.1016/j.physleta.2008.10.077.

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18

Huh, Seon-Gu, Hyun Cheol Koo, Jonghwa Eom, Hyunjung Yi, Joonyeon Chang, and Suk-Hee Han. "Unbalanced spin accumulation induced by spin Hall effect." Journal of Magnetism and Magnetic Materials 310, no. 2 (2007): e705-e707. http://dx.doi.org/10.1016/j.jmmm.2006.10.1013.

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19

Marinescu, D. C. "Spin back-flow effect in spin-polarized transport." Journal of Physics: Condensed Matter 15, no. 22 (2003): 3759–65. http://dx.doi.org/10.1088/0953-8984/15/22/310.

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20

Chowdhury, Debashree, and B. Basu. "Effect of spin rotation coupling on spin transport." Annals of Physics 339 (December 2013): 358–70. http://dx.doi.org/10.1016/j.aop.2013.09.011.

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21

YANG, JUN, KAI-MING JIANG, WEN YUAN WU, and YAN CHUN GONG. "MAGNETIC SWITCHING EFFECT IN SPIN FIELD-EFFECT TRANSISTORS." International Journal of Modern Physics B 24, no. 23 (2010): 4501–7. http://dx.doi.org/10.1142/s0217979210056190.

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Taking account the presence of external magnetic field, we study the conductance properties in spin field-effect transistors (SFET). It is shown that the conductance of the SFET exhibits an excellent magnetic switching characteristic for high potential barriers, and it is more and more pronounced with the potential barrier strength increasing. According to the effect, we can switch the SFET on or off by tuning the strength of the magnetic field. We also study how the conductance of the SFET is manipulated by spin–orbit coupling strength and spin polarization in source and drain.

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22

GANICHEV, S. D. "MAGNETO-GYROTROPIC PHOTOGALVANIC EFFECTS IN SEMICONDUCTOR QUANTUM WELLS." International Journal of Modern Physics B 22, no. 01n02 (2008): 115–16. http://dx.doi.org/10.1142/s0217979208046189.

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The spin-orbit coupling provides a versatile tool to generate and to manipulate the spin degree of freedom in low-dimensional semiconductor structures. The spin Hall effect, where an electric current drives a transverse spin current and causes a nonequilibrium spin accumulation near the sample boundary,1,2 the spin-galvanic effect, where a nonequilibrium spin polarization drives an electric current3,4 or the reverse process, in which an electrical current generates a non-equilibrium spin-polarization,5–9 are all consequences of spin-orbit coupling. In order to observe a spin Hall effect a bias

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23

SHENG, L., and C. S. TING. "INTRINSIC SPIN HALL EFFECT IN MESOSCOPIC SYSTEMS." International Journal of Modern Physics B 20, no. 17 (2006): 2339–58. http://dx.doi.org/10.1142/s0217979206034613.

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The intrinsic spin Hall effect has been attracting increasing theoretical and experimental interest since its discovery about two years ago. In this article, we review the main achievements in the theoretical aspect of both dissipative and nondissipative spin Hall effects in mesoscopic systems. The Landauer–Büttiker formula and Green's function approach based numerical method for the spin Hall effect is also introduced.

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24

CHEN, KUO-CHIN, and CHING-RAY CHANG. "GEOMETRICAL EFFECT ON SPIN TRANSPORT." SPIN 03, no. 03 (2013): 1340006. http://dx.doi.org/10.1142/s2010324713400067.

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This review paper shows some methods to study electrons with spin transport properties. We focus on spin precession patterns with the influence of the spin orbital interaction (SOI) by different way to discuss the spin transport on curved system. This paper can be divided into three parts. The first part is studying the spin precession patterns in the U-shaped 1D wire by introducing a confined potential. In the second part, we introduce a non-Abelian spin–orbital gauge field to study electrons transport on a curved surface. The third part is a generalized form of part one, we study exact Hamil

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25

Ellsworth, David, Lei Lu, Jin Lan, et al. "Photo-spin-voltaic effect." Nature Physics 12, no. 9 (2016): 861–66. http://dx.doi.org/10.1038/nphys3738.

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26

Wunderlich, J., B. G. Park, A. C. Irvine, et al. "Spin Hall Effect Transistor." Science 330, no. 6012 (2010): 1801–4. http://dx.doi.org/10.1126/science.1195816.

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27

Bass, S. D., and A. W. Thomas. "The EMC spin effect." Journal of Physics G: Nuclear and Particle Physics 19, no. 7 (1993): 925–55. http://dx.doi.org/10.1088/0954-3899/19/7/005.

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28

Yanson, I. K., Yu G. Naidyuk, V. V. Fisun, et al. "Surface Spin-Valve Effect." Nano Letters 7, no. 4 (2007): 927–31. http://dx.doi.org/10.1021/nl0628192.

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29

Gurzhi, R. N., A. N. Kalinenko, A. I. Kopeliovich, and A. V. Yanovskiĭ. "Nanocontact spin-electric effect." Low Temperature Physics 34, no. 7 (2008): 535–37. http://dx.doi.org/10.1063/1.2957005.

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30

Jungwirth, Tomas, Jörg Wunderlich, and Kamil Olejník. "Spin Hall effect devices." Nature Materials 11, no. 5 (2012): 382–90. http://dx.doi.org/10.1038/nmat3279.

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31

Kawada, Takuya, Masashi Kawaguchi, Takumi Funato, Hiroshi Kohno, and Masamitsu Hayashi. "Acoustic spin Hall effect in strong spin-orbit metals." Science Advances 7, no. 2 (2021): eabd9697. http://dx.doi.org/10.1126/sciadv.abd9697.

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We report on the observation of the acoustic spin Hall effect that facilitates lattice motion–induced spin current via spin-orbit interaction (SOI). Under excitation of surface acoustic wave (SAW), we find that a spin current flows orthogonal to the SAW propagation in nonmagnetic metals (NMs). The acoustic spin Hall effect manifests itself in a field-dependent acoustic voltage in NM/ferromagnetic metal bilayers. The acoustic voltage takes a maximum when the NM layer thickness is close to its spin diffusion length, vanishes for NM layers with weak SOI, and increases linearly with the SAW freque

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32

Panda, S. N., S. Mondal, J. Sinha, S. Choudhury та A. Barman. "All-optical detection of interfacial spin transparency from spin pumping in β-Ta/CoFeB thin films". Science Advances 5, № 4 (2019): eaav7200. http://dx.doi.org/10.1126/sciadv.aav7200.

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Generation and utilization of pure spin current have revolutionized energy-efficient spintronic devices. Spin pumping effect generates pure spin current, and for its increased efficiency, spin-mixing conductance and interfacial spin transparency are imperative. The plethora of reports available on generation of spin current with giant magnitude overlook the interfacial spin transparency. Here, we investigate spin pumping in β-Ta/CoFeB thin films by an all-optical time-resolved magneto-optical Kerr effect technique. From variation of Gilbert damping with Ta and CoFeB thicknesses, we extract the

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33

Ustinov, V. V., I. A. Yasyulevich, and N. G. Bebenin. "The Chiral Spin-Orbitronics of a Helimagnet–Normal Metal Heterojunction." Физика металлов и металловедение 124, no. 2 (2023): 204–13. http://dx.doi.org/10.31857/s001532302260174x.

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A theory of spin and charge transport in bounded metallic magnets has been constructed, which takes into account the effects of spin-orbit scattering of conduction electrons by crystal lattice defects. The theory can be used to describe the spin Hall effect and the anomalous Hall effect and can serve as a basis for describing the phenomena of spin-orbitronics. Phenomenological boundary conditions for the charge and spin fluxes at the interface between two different metals have been formulated, on the basis of which the injec-tion of a pure spin current into a helimagnet, which arises in a norm

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34

Dvoreckaia E. V., Sidorov V. L., Koplak O. V., et al. "Magnetocaloric effect in amorphous-crystalline microcircuits PrDyFeCoB." Physics of the Solid State 64, no. 8 (2022): 989. http://dx.doi.org/10.21883/pss.2022.08.54615.373.

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In amorphous-crystalline PrDyFeCoB microconductors obtained by ultrafast melt cooling, a negative magnetocaloric effect was detected at 200-250 K (with heat release when the magnetic field is turned on), as well as a positive magnetocaloric effect in the temperature range of 300-340 K (with heat absorption when the magnetic field is turned on). It is established that there are no phase transitions of the first kind in the studied temperature range, which indicates that both of the detected effects are associated with a change in the magnetic part of the entropy. The transition at 200-250 K is

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35

Shan, Shu-Ping. "Temperature effect and Rashba effect of polaron in a parabolic quantum well." Low Temperature Physics 50, no. 2 (2024): 171–75. http://dx.doi.org/10.1063/10.0024330.

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Using Tokuda’s improved linear combination operator method and variational technique, the expression of the polaron effective mass in an parabolic quantum well is derived. Due to the spin-orbit interaction, the effective mass of polaron splits into two branches. The dependence of effective mass on temperature and mean number phonons is discussed by numerical calculation. The effective mass of polaron is an increasing function of temperature and mean number phonons. The absolute value of total spin splitting effective mass increases with the increase in temperature and spin-orbit coupling param

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36

Hattori, Kiminori. "Spin-Current-Driven Spin Pumping in Rashba Spin–Orbit Coupled Systems: A Spin Torque Effect." Journal of the Physical Society of Japan 78, no. 8 (2009): 084703. http://dx.doi.org/10.1143/jpsj.78.084703.

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37

B S, Athira, Mandira Pal, Sounak Mukherjee, et al. "Towards the development of new generation spin-orbit photonic techniques." Journal of Optics 24, no. 5 (2022): 054006. http://dx.doi.org/10.1088/2040-8986/ac5cd8.

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Abstract Spin–orbit interaction deals with the interaction and coupling of spin and orbital angular momentum degrees of freedom of spinning particles, which manifests in diverse fields of physics, ranging from atomic, condensed matter to optical systems. In classical light beams, this has led to a number of non-trivial optical phenomena like spin and orbital Hall effect of light, optical Rashba effect, photonic Aharonov–Bohm effect, rotational Doppler effect, transverse spin, Belinfante’s spin-momentum and spin-momentum locking etc. These have been observed in diverse micro- and nano-scale opt

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38

Wang, Zhenyu, Weiwei Bao, Yunshan Cao, and Peng Yan. "All-magnonic Stern–Gerlach effect in antiferromagnets." Applied Physics Letters 120, no. 24 (2022): 242403. http://dx.doi.org/10.1063/5.0096968.

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The Stern–Gerlach (SG) effect is well known as the spin-dependent splitting of a beam of atoms carrying magnetic moments by a magnetic-field gradient, leading to the concept of electron spin. Antiferromagnets can accommodate two magnon modes with opposite spin polarizations, which is equivalent to the spin property of electrons. Here, we propose an all-magnonic SG effect in an antiferromagnetic magnonic system, where a linearly polarized spin-wave beam is deflected by a straight Dzyaloshinskii–Moriya interaction (DMI) interface into two opposite polarized spin-wave beams propagating in two dis

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39

Lan, Shun-Yi, and Xiang-Cun Meng. "The Effect of Irradiation on the Spin of Millisecond Pulsars." Astrophysical Journal Letters 956, no. 1 (2023): L24. http://dx.doi.org/10.3847/2041-8213/acfedf.

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Abstract A millisecond pulsar (MSP) is an old neutron star (NS) that has accreted material from its companion star, causing it to spin up, which is known as the recycling scenario. During the mass transfer phase, the system manifests itself as an X-ray binary. PSR J1402+13 is an MSP with a spin period of 5.89 ms and a spin period derivative of log P ̇ spin = − 16.32 . These properties make it a notable object within the pulsar population, as MSPs typically exhibit low spin period derivatives. In this paper, we aim to explain how an MSP can possess a high spin period derivative by binary evolut

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40

Pournaghavi, Nezhat, Mahdi Esmaeilzadeh, Adib Abrishamifar, and Somaieh Ahmadi. "Extrinsic Rashba spin–orbit coupling effect on silicene spin polarized field effect transistors." Journal of Physics: Condensed Matter 29, no. 14 (2017): 145501. http://dx.doi.org/10.1088/1361-648x/aa5b06.

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41

Bhardwaj, Ravindra G., Paul C. Lou, and Sandeep Kumar. "Spin Seebeck effect and thermal spin galvanic effect in Ni80Fe20/p-Si bilayers." Applied Physics Letters 112, no. 4 (2018): 042404. http://dx.doi.org/10.1063/1.5003008.

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42

Zhao Junqian, 赵军倩, 周新星 Zhou Xinxing, and 罗海陆 Luo Hailu. "Spin Angle Splitting in Spin Hall Effect of Light." Acta Optica Sinica 33, no. 5 (2013): 0526003. http://dx.doi.org/10.3788/aos201333.0526003.

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43

Lee, Kyung-Jin, and Seo-Won Lee. "Effect of Spin Memory Loss on Spin-Transfer Torque." Journal of the Korean Physical Society 55, no. 4 (2009): 1501–8. http://dx.doi.org/10.3938/jkps.55.1501.

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44

Balinskiy, Michael, Howard Chiang, David Gutierrez, and Alexander Khitun. "Spin wave interference detection via inverse spin Hall effect." Applied Physics Letters 118, no. 24 (2021): 242402. http://dx.doi.org/10.1063/5.0055402.

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45

Manchon, A., and K. J. Lee. "Spin Hall effect-driven spin torque in magnetic textures." Applied Physics Letters 99, no. 2 (2011): 022504. http://dx.doi.org/10.1063/1.3609236.

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46

Bellucci, S., F. Corrente, and P. Onorato. "Spin Hall effect and spin filtering in ballistic nanojunctions." Journal of Physics: Condensed Matter 19, no. 39 (2007): 395019. http://dx.doi.org/10.1088/0953-8984/19/39/395019.

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47

Kim, Kitae, Woo Young Shim, and Sug-Bong Choe. "Huge self-spin swapping effect with asymmetric spin-sink structures." NPG Asia Materials 17, no. 1 (2025). https://doi.org/10.1038/s41427-025-00597-5.

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Abstract The spin swapping effect is a promising phenomenon that provides a symmetry-breaking component for deterministic field-free switching, essential for the all-electric control of spintronic devices. Without the need for additional magnetic layers in the original proposal, this effect can occur with a single magnetic layer by reinjecting spin current back into itself, known as the self-spin swapping effect. Here, we experimentally demonstrate that the self-spin swapping effect is significant and even surpasses other dominant phenomena such as the spin Hall effect. This observation became

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48

Zeng, Wen, and Rui Shen. "Anomalous spin Josephson effect in spin superconductors." Chinese Physics B, December 29, 2023. http://dx.doi.org/10.1088/1674-1056/ad1982.

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Abstract The spin superconductor state is the spin-polarized triplet exciton condensate, which can be viewed as a counterpart of the charge superconductor state. As an analogy of the charge Josephson effect, the spin Josephson effect can be generated in the spin superconductor/normal metal/spin superconductor junctions. Here we study the spin supercurrent in the Josephson junctions consisting of two spin superconductors with noncollinear spin polarizations. For the Josephson junctions with out-of-plane spin polarizations, the possible π-state spin supercurrent appears due to the Fermi momentum

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49

Kumar, Gaurav, and Anurag Srivastava. "Silicene Nanoribbon Based Spin-Field Effect Transistor With Spin Filtering and Spin Seebeck Effects." IEEE Transactions on Nanotechnology, 2022, 1–8. http://dx.doi.org/10.1109/tnano.2022.3220031.

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50

Qi, Yunong, Zhi-Gang Yu, and Michael E. Flatté. "Spin Gunn Effect." Physical Review Letters 96, no. 2 (2006). http://dx.doi.org/10.1103/physrevlett.96.026602.

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