Skill Mion
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In solid-state physics, skill Mion [1] (British: with skyrmion [ˈskɜːrmi.ɒn], scar Mion [2]) means the model of the topologically unusual vortex to occur in the consecutive places. Because each behaves like a particle, I can see this whirlpool with quasiparticle with limited mass [3]. For 1,962 years, was devised by Tony スカーム () to explain quantum stack alignment and a resonance state of the baryon [note 1]; [4]. It was foretold from atomic nucleus properties of matter [5]. This model is like higher mathematics and is non-linear by a mathematical request explicitly. Originally it is started from high energy physics, but it is applied in solid physics now and collects interest from the field of information technology. Skill Mion of Bose = Einstein condensation body [6], superconductor [7], magnetic film [8], カイラルネマティック liquid crystal [9] is reported, but is not the thing which I got of the conclusive evidence conclusively [the source required].
Table of contents
Summary
The skill Mion model models fermion (nucleon) as special soliton arising from the boson ground (non-linear classic ground to explain strong interaction by the exchange of the mesotron); [10] [11] [12] [13]. In the early 1980s, I was proposed with work of Edward Witten and the famous bag model (I refer to the item of Kenneth, Andrew Johnson ) independently and I connected it with quantum Hall effect and was argued. Skill Mion in the surface, interface magnetism system is discovered now [14]; [15].
In the field of solid-state physics particularly the development remarkable spintronics technology, spin placement non-self-evident topologically called magnetic skill Mion attracts attention. It is the spin placement that is provided when two-dimensional magnetic skill Mion performs, for example, stereo projection of three-dimensional spin "hedgehog (hedgehog)" [note 2]. In other words, have downward South Pole spin with ascending North Pole spin in the center point of Japanese yen in the fringe domain of Japanese yen; is distributed [16].
When a magnetic field placed a chiral magnetic body under it, a thing of the size of around several thousand electronic spins is known to produce magnetic skill Mion. Because can move the microbest solid freely, and the possibility that can control it was shown without hardly starting a Joule heat, application as the nonvolatile memory to realize low power consumption and high density implementation is expected [17]; [18].
Mathematical definition
In the field theory, skill Mion is the classic solution which is non-self-evident for homoTopy for the non-linear sigma model of the non-self-evident target manifold topology. Therefore, skill Mion is topologic soliton. Examples include chiral model () [note 3] of the mesotron. In this case the target manifold is homogeneous space of the next structure group.
Here SU(N)L and SU(N)R of the SU(N) line is the left part and the right part each, and SU(N)diag is opposite angle subgroup ().
When space-time has topological S3 X R, the classic placement is classified in integer number of revolutions [note 4]. This is homoTopy group of Miyoshi
But, this is because it is equivalent with the ring of the integer. Here, the equal sign means the phase same model.
A topologic clause may be added to chiral raglan sleeves diAnn, and the integral calculus depends only on homoTopy then. As a result, a super choice sector occurs in the quantized model. Skill Mion can be similar as soliton of the signature ゴルドン equation (). With mass, it becomes the fermion interacting according to a schilling model () when I quantize it by the Bethe temporary construction () others.
Magnetic body, data recording medium
In the chiral magnetic body which Diallo since key, Moriya interaction () plays an important role in, magnetic skill Mion is known to appear without having an inversion symmetry. The size of this skill Mion is 1,200nm [the source required] degree from 1nm (example in case of iron on Ir (111)) [19]. As a result of study, I can read and write skill Mion by a scanning tunnel microscope [20]. From littleness of magnetic skill Mion and lower energy consumption, the future application to the data recording medium of the form representing "1" and "0" of the bit and other spintronics devices is expected by topology Cal charge representing the living-in-absence of skill Mion [21]; [22] [23]. There is the report of stable skill Mion in room temperature [24]; [25].
Outside link
- "Developments in Magnetic Skyrmions Come in Bunches" (English). IEEE Spectrum (2015). September 24, 2016 reading.
- Christian Schüller. "Ultraschnelle Exzitonendynamik am Quanten-Hall-Ferromagneten." (German). Regensburg University (). It archives it than an original as of October 6, 2007. September 27, 2016 reading.
- "Skyrmionen im Spingitter" (German). Pro-Physik (February 13, 2009). September 27, 2016 reading.
- FDTD Skyrmion simulation in calculating pixel space - YouTube
Footnote
- The model who was connected with a mesotron appeared afterwards ^.
- Singular point of homoTopy 1 called the ブロッホ point of number +1 coating in ^ micro magnetics
- A verge between the left skill and the right skill is emphasized with the ^ chiral model.
- A classification like ^ fulfills an effective spin "hedgehog singular point". As for the upper spin, the lower spin sets out for the South Pole at the North Pole. I refer to Döring (1968).
Source
- ^ "skill Mion." Technology term information. Technology promotion mechanism. September 28, 2016 reading.
- ^ Ezawa Masahiko. "Topology Cal structure in a magnetic body". Tokyo University. September 28, 2016 reading.
- ^ "Feldknoten als Teilchen" (German). Spektrum der Wissenschaft (4): 11. (2009).
- ^ Wong, Stephen (2002). It is arXiv:hep-ph/0202250 [hep/ph]. "What exactly is a Skyrmion?"
- ^ M.r. khoshbin-e-khoshnazar (2002). "Correlated quasiskyrmions as alpha-particles" (English). Eur. Phys. J. A 14 (2): 207–209. doi: 10.1140/epja/i2001-10198-.
- ^ Al Khawaja, Usama; Stoof, Henk (2001). "Skyrmions in a ferromagnetic Bose–Einstein condensate." Nature 411 (6840): 918–20. Bibcode 2001Natur.411..918A. doi: 10.1038/35082010. PMID 11418849.
- ^ Baskaran, G. (2011). It is arXiv: "Possibility of Skyrmion Superconductivity in Doped Antiferromagnet K2Fe4Se5" 1108.3562 [cond-mat.supr-con].
- ^ Kiselev, N. S.; Bogdanov, A. N.; Schäfer, R.; Rößler, U. K. (2011). "Chiral skyrmions in thin magnetic films: New objects for magnetic storage technologies?." Journal of Physics D: Applied Physics 44 (39): 392001. arXiv: 1102.2726. Bibcode 2011JPhD...44M2001K. doi: 10.1088/0022-3727/44/39/392001.
- ^ Fukuda, J.-I.; Žumer, S. (2011). "Quasi-two-dimensional Skyrmion lattices in a chiral nematic liquid crystal." Nature Communications 2:246. Bibcode 2011NatCo...2E.246F. doi: 10.1038/ncomms1250. PMID 21427717.
- ^ Skyrme, T. H. R. (1958). "A Non-Linear Theory of Strong Interactions". Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences 247 (1249): 260–278. doi: 10.1098/rspa.1958.0183. ISSN 0080-4630.
- ^ Skyrme, T. H. R. (1959). "A Unified Model of K- and \pi -mesons". Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences 252 (1269): 236–245. doi: 10.1098/rspa.1959.0149. ISSN 0080-4630.
- ^ Skyrme, T. H. R. (1961). "A Non-Linear Field Theory". Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences 260 (1300): 127–138. doi: 10.1098/rspa.1961.0018. ISSN 0080-4630.
- ^ Skyrme, T. H. R. (1961). "Particle States of a Quantized Meson Field". Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences 262 (1309): 237–245. doi: 10.1098/rspa.1961.0115. ISSN 0080-4630.
- ^ Stefan Blügel. "From Rashba effect to topologically protected spin textures at metal surfaces" (PDF). Universität Regensburg. It archives it than an original as of October 14, 2013. September 26, 2016 reading. .
- ^ Christian Pfleiderer (2010). "Magnetismus mit Drehsinn" (German). Physik Journal (11): 25.
Christian Pfleiderer (2013). "Wirbel um Spinwirbel" (German). Physik Journal (10): 20–21. - ^ Döring, W. (1968). "Point Singularities in Micromagnetism". Journal of Applied Physics 39 (2): 1006–1007. doi: 10.1063/1.165614.
- It is "greatly reading for electron it is a microelectric current in whirlpool "skill Mion" of spinning realization of the magnetism spin control technology at the low current density of a one-100,000th of drive - before ^ on progress -" (press release), Institute of Physical and Chemical Research, (August 8, 2012)/ September 24, 2016.
- In ^ "a very small magnetic whirlpool storage cell." The Nihon Keizai Shimbun: p. 17. (March 8, 2015)
- ^ Heinze, Stefan; Von Bergmann, Kirsten; Menzel, Matthias; Brede, Jens; Kubetzka, André; Wiesendanger, Roland; Bihlmayer, Gustav; Blügel, Stefan (2011). "Spontaneous atomic-scale magnetic skyrmion lattice in two dimensions." Nature Physics 7 (9): 713–718. Bibcode 2011NatPh...7..713H. doi: 10.1038/NPHYS2045 (Jul 31, 2011).
- ^ Romming, N.; Hanneken, C.; Menzel, M.; Bickel, J. E.; Wolter, B.; Von Bergmann, K.; Kubetzka, A.; Wiesendanger, R. (2013). "Writing and Deleting Single Magnetic Skyrmions." Science 341 (6146): 636–9. Bibcode 2013Sci...341..636R. doi: 10.1126/science.1240573. PMID 23929977 (Aug 8, 2013).
- ^ A. Fert; V. Cros; J. Sampaio (2013). "Skyrmions on the track." It is 152–156. Nature Nanotechnology 8 Bibcode 2013NatNa...8..152F. doi: 10.1038/nnano.2013.29.
- ^ Y. Zhou, E. Iacocca, A.A. Awad, R.K. Dumas, F.C. Zhang, H.B. Braun and J. Akerman (2015). "Dynamically stabilized magnetic skyrmions." Nature Communications 6:8,193. Bibcode 2015NatCo...6E8193Z. doi: 10.1038/ncomms9193.
- ^ X.C. Zhang; M. Ezawa; Y. Zhou (2014). "Magnetic skyrmion logic gates: conversion, duplication and merging of skyrmions." It is arXiv: Scientific Reports 5:9,400 1410.3086. Bibcode 2015NatSR...5E9400Z. doi: 10.1038/srep09400.
- ^ Jiang, Wanjun; Upadhyaya, Pramey; Zhang, Wei; Yu, Guoqiang; Jungfleisch, M. Benjamin; Fradin, Frank Y.; Pearson, John E.; Tserkovnyak, Yaroslav et al. (2015-07-17). "Blowing magnetic skyrmion bubbles". Science 349 (6245): 283–286. arXiv: 1502.08028. Bibcode 2015Sci...349..283J. doi: 10.1126/science.aaa1442. ISSN 0036-8075. PMID 26067256.
- ^ Gilbert, Dustin A.; Maranville, Brian B.; Balk, Andrew L.; Kirby, Brian J.; Fischer, Peter; Pierce, Daniel T.; Unguris, John; Borchers, Julie A. et al. (2015-10-08). "Realization of ground-state artificial skyrmion lattices at room temperature". Nature Communications 6. Bibcode 2015NatCo...6E8462G. doi: 10.1038/ncomms946.
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