# Spinon

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{{Short description|Quasiparticle in an extremely cold solid}}
'''Spinons''' are one of three [quasiparticle](/source/quasiparticle)s, along with [holon](/source/holon_(physics))s and [orbiton](/source/orbiton)s, that [electron](/source/electron)s in solids are able to split into during the process of [spin–charge separation](/source/spin%E2%80%93charge_separation), when extremely tightly confined at temperatures close to [absolute zero](/source/absolute_zero).<ref>
{{cite web
 | title = Discovery About Behavior Of Building Block Of Nature Could Lead To Computer Revolution
 | url = https://www.sciencedaily.com/releases/2009/07/090730141607.htm
 | date = 31 July 2009
 | work = [ScienceDaily](/source/ScienceDaily)
 | accessdate = 2009-08-01
}}</ref> The electron can always be theoretically considered as a [bound state](/source/bound_state) of the three, with the spinon carrying the [spin](/source/Spin_(physics)) of the electron, the [orbiton](/source/orbiton) carrying the [orbital location](/source/Atomic_orbital) and the [holon](/source/Holon_(physics)) carrying the [charge](/source/Electric_charge), but in certain conditions they can behave as independent [quasiparticle](/source/quasiparticle)s.

The term spinon is frequently used in discussions of experimental facts within the framework of both [quantum spin liquid](/source/quantum_spin_liquid) and [strongly correlated quantum spin liquid](/source/strongly_correlated_quantum_spin_liquid).<ref>{{cite book | author=Amusia, M., Popov, K., Shaginyan, V., Stephanovich, V. | title=Theory of Heavy-Fermion Compounds - Theory of Strongly Correlated Fermi-Systems | volume=182 | publisher=Springer | year=2014 | isbn=978-3-319-10825-4| doi=10.1007/978-3-319-10825-4 | series=Springer Series in Solid-State Sciences }}</ref>

==Overview==
Electrons, being of like charge, repel each other. As a result, in order to move past each other in an extremely crowded environment, they are forced to modify their behavior. Research published in July 2009 by the [University of Cambridge](/source/University_of_Cambridge) and the [University of Birmingham](/source/University_of_Birmingham) in [England](/source/England) showed that electrons could jump from the surface of the metal onto a closely located [quantum wire](/source/quantum_wire) by [quantum tunneling](/source/quantum_tunneling), and upon doing so, will separate into two [quasiparticle](/source/quasiparticle)s, named spinons and holons by the researchers.<ref>
{{cite journal
 | author = Y. Jompol| year = 2009
 | title = Probing Spin-Charge Separation in a Tomonaga-Luttinger Liquid
 | journal = [Science](/source/Science_(journal))
 | volume = 325 | issue = 5940 | pages = 597–601
 | doi = 10.1126/science.1171769
 | pmid = 19644117
|bibcode = 2009Sci...325..597J |arxiv = 1002.2782 | s2cid = 206193
 |display-authors=etal}}</ref>

The orbiton was predicted theoretically by [van den Brink](/source/Jeroen_van_den_Brink),  [Khomskii](/source/Daniel_I._Khomskii) and Sawatzky in 1997–1998.<ref>
{{cite journal
 | author = H.F. Pen, J. van den Brink, D. I. Khomskii and G.A. Sawatzky
 | year = 1997
 | title = Orbitally ordered, triangular spin singlet phase in LiVO2
 | journal = Physical Review Letters
 | volume = 78  | issue = 7
 | pages = 1323–1326
  |bibcode = 1997PhRvL..78.1323P |doi = 10.1103/PhysRevLett.78.1323 | s2cid = 120734299
 }}</ref><ref>{{cite journal
 | author = J. van den Brink, W. Stekelenburg, D.I. Khomskii, G.A. Sawatzky and K.I. Kugel
 | year = 1998
 | title = Spin and orbital excitations in magnetic insulators with Jahn-Teller ions
 | journal = Physical Review B
 | volume = 58  | issue = 16
 | pages = 10276–10282
  |bibcode = 1998PhRvB..5810276V |doi = 10.1103/PhysRevB.58.10276 | s2cid = 55650675
 }}</ref>
Its experimental observation as a separate quasiparticle was reported in paper sent to publishers in September 2011.<ref>{{cite journal
 |title=Spin–orbital separation in the quasi-one-dimensional Mott insulator Sr2CuO3
 |date=18 April 2012
 |doi=10.1038/nature10974
 |arxiv = 1205.1954 |bibcode = 2012Natur.485...82S
 |pmid=22522933
 |volume=485
 |issue=7396
 |journal=Nature
 |pages=82–5|last1=Schlappa
 |first1=J
 |last2=Wohlfeld
 |first2=K
 |last3=Zhou
 |first3=K. J
 |last4=Mourigal
 |first4=M
 |last5=Haverkort
 |first5=M. W
 |last6=Strocov
 |first6=V. N
 |last7=Hozoi
 |first7=L
 |last8=Monney
 |first8=C
 |last9=Nishimoto
 |first9=S
 |last10=Singh
 |first10=S
 |last11=Revcolevschi
 |first11=A
 |last12=Caux
 |first12=J. S
 |last13=Patthey
 |first13=L
 |last14=Rønnow
 |first14=H. M
 |last15=Van Den Brink
 |first15=J
 |last16=Schmitt
 |first16=T
 |s2cid=205228324
 }}</ref><ref>{{cite journal
 |title=Not-quite-so elementary, my dear electron
 |date=18 April 2012
 |doi=10.1038/nature.2012.10471
 |url=http://www.nature.com/news/not-quite-so-elementary-my-dear-electron-1.10471
 |last1=Merali
 |first1=Zeeya
 |journal=Nature
 }}</ref>
The research states that by firing a beam of [X-ray](/source/X-ray) [photon](/source/photon)s at a single electron in a one-dimensional sample of strontium [cuprate](/source/cuprate), this will excite the electron to a higher orbital, causing the beam to lose a fraction of its energy in the process. In doing so, the electron will be separated into a spinon and an orbiton. This can be traced by observing the energy and momentum of the X-rays before and after the collision.

==See also==
*[Condensed matter physics](/source/Condensed_matter_physics)
*[Tomonaga–Luttinger liquid](/source/Tomonaga%E2%80%93Luttinger_liquid)

==References==
{{reflist}}

Category:Quasiparticles

{{particle-stub}}

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Adapted from the Wikipedia article [Spinon](https://en.wikipedia.org/wiki/Spinon) by Wikipedia contributors ([contributor history](https://en.wikipedia.org/wiki/Spinon?action=history)). Available under [Creative Commons Attribution-ShareAlike 4.0 International](https://creativecommons.org/licenses/by-sa/4.0/). Changes may have been made.
