Topological Physics – Phenomena in physics controlled by the topology (often: the homotopy theory) of the physical system.
General theory:
In metamaterials:
topological phononics (sound waves?)
For quantum computation:
In quantum physics, braid group statistics or anyon statistics (sometimes: plektons) refers to an exotic phenomenon where the braiding of the worldlines of certain effective particles (“anyons”) in an effectively 2+1-dimensional spacetime has the effect of transforming the quantum state of the total quantum system by unitary operators which constitute a linear representation of the braid group – a braid representation.
Often this is motivated as a generalization of the boson- or fermion-“statistics” which enters the spin-statistics theorem, see below.
But the actual mathematical nature of anyons must be different from that of elements of boson/fermion-Fock spaces and often remains somewhat vague in existing discussions. One may recognize two different more concrete conceptualizations of anyons in the literature:
anyonic quanta much like boson/fermion quanta but subject to an additional global interaction by Aharonov-Bohm phases due to a flat fictitious gauge field which is sourced by and coupled to each of the quanta;
(this goes back to Arovas, Schrieffer, Wilczek & Zee 1985, further developed in Chen, Wilczek, Witten & Halperin 1989, see below)
anyonic defects like vortices or other solitons, whose position is a classical parameter to the quantum system, the adiabatic movement of which acts by Berry phases on the quantum ground state.
(e.g. Avros, Schrieffer & Wilczek 1984, see further below)
The concept of anyons is particularly well motivated in solid state physics, where effectively 2-dimensional quantum materials are common place (eg. graphene) or where particles may otherwise be constrained to move in a plane, such as in the quantum Hall effect. There is a multitude of models in condensed matter theory (mostly lattice models, such as string-net models) which theoretically realize anyon braid group statistics, and there are some first experimental indications of anyonic phenomena in actual materials (see the references under Experimental Realization) below.
Specifically, in the context of topological phases of matter, the (potential) presence of anyons has come to be known as the case of topological order, see there for more.
Besides general curiosity, much of the interest in anyonic braid group statistics lies in the fact that these braid representations are imagined to potentially serve as quantum gates in topological quantum computers. See there for more.
In quantum field theory, one speaks of the “statistics” of a particle species when referring to the linear representation that $n$-particle wavefunctions form under the the symmetric group $Sym(n)$ which permutes the $n$ particles.
While there is a rich representation theory of the symmetric group, the spin-statistics theorem says, when it applies, that for field quanta only the simplest two possibilities may occur:
bosons (such as photons) transform under the trivial representation of $Sym(n)$,
fermions (such as electrons) transform under the sign representation of $Sym(n)$.
(see also at Slater determinant)
Now, the braid group on $n$ strands covers the symmetric group
which allows one to regard any linear representation of the symmetric group also as a particular braid group representation. But by its definition, the braid group may be understood as the group of isotopy-classes of disjoint timelike worldlines in an effectively 2+1 dimensional spacetime, with the group operation being concatenation of worldlines.
In this sense, one may imagine that any braid group representations may generalize the boson/fermion statistics in 2+1 dimensions. Texts typically suggest that this applies to quasiparticles.
The term anyon (due to Wilczek 1982b) is a pun on this state of affairs that any statistics “in between” boson- and fermion-statistics may be allowed.
On the other hand, anyonic braiding is conceptually different from boson/fermion statistics – if it were on the same footing then the spin-statistics theorem would rule out anyonic braiding. This is acknowledged by Chen, Wilczek, Witten & Halperin 1989, p. 352 (cf. also Wilczek 1990, §I.2, pp. 11):
Once the permutation group is replaced by the braid group, the simple construction of passing from the solution to the one-particle problems to the solution of many-particle problems, familiar from the free bosons and free fermions, does not work anymore.
A concrete model for anyonic quanta via otherwise free fermions in 2d interacting through a flat “fictitious gauge field” was proposed in Arovas, Schrieffer, Wilczek & Zee 1985 and developed in Chen, Wilczek, Witten & Halperin 1989 (the model has been advertized in early reviews, e.g. Wilczek 1990, §I.3 and Wilczek 1991, but seems not to have been developed much since):
The model regards anyons as a priori free fermions, but equipped now with a non-local mutual interaction via a “fictitious gauge field” (CWWH89, §2), in that each of the particles is modeled as the singular source of a flat circle connection (a vector potential with vanishing field strength), which hence exerts no Lorentz force but has the effect that globally each particle is subject to the same Aharonov-Bohm effect as would be caused by a tuple of infinite solenoids piercing through each of the other particle’s positions.
For emphasis, from CWWH89, p. 359:
Here the particles are to be regarded (in the absence of interactions) as fermions; the interaction then makes them anyons with statistical parameter $\theta = \pi(1 - 1/n)$.
It follows (Wu 1984, Imbo, Imbo & Sudarshan 1990) that (quoting from Fröhlich, Gabbiani & Marchetti 1990, p. 20):
If $\theta \in\!\!\!\!\!/ \frac{1}{2}\mathbb{Z}$ the Hilbert space of anyon wave functions must be chosen to be a space of multi-valued functions with half-monodromies given by the phase factors $exp(2 \pi \mathrm{i} \theta)$. Such wave functions can be viewed as single-valued functions on the universal cover $\widetilde M_n$ of $M_n$ $[$the configuration space of points$]$.
Further discussion of anyon-wavefunctions as multi-valued functions on a configuration space of points, hence equivariant functions on its universal cover: BCMS93, §1, Mund & Schrader 1995, DFT97, §1 Myrheim 1999, DMV03, Murthy & Shankar 2009
Incidentally, the quasi-particle-excitations of (or in) a gas of such Aharonov-Bohm phased anyons are argued to be vortices (CWWH89, p. 457):
we are led to conclude that in anyon superconductivity, charged quasi-particles and vortices do not constitute two separate sorts of elementary excitations - they are one and the same.
This seamlessly leads over to:
In practice, many (most?) incarnations of the concept of anyons are anyonic defects – non-perturbative solitonic defects (of codimension=2), akin to vortices in fluids:
Anyonic particles are best viewed as a kind of topological defects that reveal non-trivial properties of the ground state. $[$Kitaev 2006, p. 4$]$
Anyons can arise in two ways: as localised excitations of an interacting quantum Hamiltonian or as defects in an ordered system. $[$Das Sarma, Freedman & Nayak 2015, p. 1$]$
(Compare also the original discussions in Goldin, Menikoff & Sharp 1981, §III, Wilczek 1982a & Wilczek 1990, p. 5, which offer a quantum particle “bound” to a classical & infinite solenoid – hence a 2d magnetic monopole defect – as a decent model for an anyon.)
But defects are a kind of boundary conditions, hence external parameters or background fields for the actual quantum field.
Concretely, a widely appreciated proposal (Moore & Read 1991, Read & Rezayi 1999) identifies anyonic ground state wavefunctions with conformal blocks of a 2d CFT – hence with Chern-Simons theory states – with prescribed poles at the location of the anyons.
Now the quantum adiabatic theorem says that the sufficiently slow motion of such external parameters transforms the quantum ground state by unitary operators (“Berry phases”, see also at adiabatic quantum computation). This suggests (Avros, Schrieffer & Wilczek 1984, p. 1, Freedman, Kitaev, Larsen & Wang 2003, pp. 6, Nayak, Simon, Stern & Freedman 2008, §II.A.2 (p. 6), Cheng, Galitski & Das Sarma 2011, p. 1) that:
(adiabatic defect braiding)
Anyon braiding statistics is the braid group representation on a quantum ground state induced by adiabatic braiding of topological codimension=2 defects in their configuration space.
Here
for point-defects the “configuration space” is the configuration space of points in a surface (as briefly touched upon already in Leinaas & Myrheim 1977, pp. 22, Wilczek 1982b, p. 959), such as in the plane, in which case its fundamental group is the braid group;
“topological” is meant as in topological quantum field theory: The induced adiabatic unitary transformation is demanded/assumed to depend only on the isotopy-class of the defect-worldlines, hence only on the underlying braid-pattern.
This notion of anyon “statistics” is at least tacitly implicit in much of the literature on anyons in topological quantum computation, such as in the popular graphics depicting anyon worldlines as the Wilson lines in Chern-Simons theory. (see the graphics below).
Indeed, the effects of adiabatic braiding of defects in quantum materials has been understood and discussed before and in parallel to the term “anyon” becoming established: Mermin 1979, Lo & Preskill 1993.
A concrete realistic example of defect anyons are vortex anyons see below. But the notion of codimension=2 defects subsumes situations that are quite different from the quasiparticle-excitations imagined in traditional texts on anyons, such as:
Specifically, vortex anyons are realized in Bose-Einstein condensates (MPSS19, following PFCZ01) and in (other) superfluids (MMN21).
In fact, defect-type vortex anyons generically appear in condensates of non-defect anyons (CDLR19):
A theoretical model of vortex anyons in a Higgs field coupled to Chern-Simons theory is discussed in Fröhlich & Marchetti 1988. An instructive lattice model of vortex anyons is analyzed in detail in Kitaev 2006.
Much attention in current efforts towards realizing topological quantum computation is being paid to anyons realized as Majorana zero modes bound to vortices (Das Sarma, Freedman & Nayak 2015, cf. MMBDRSC19).
This situation may generalize to parafermion-su(2)-anyons, where
each (anti)soliton carries parafermion zero mode which supplies it with the non-Abelian statistics $[$Tsvelik 2014a, p. 2, cf. Borcherding 2018, pp. 3. $]$
Braiding of nodal points in momentum space (graphics from MMBDRSC19, Fig. 1):
Around 2020 the view has been emerging that also defects “in momentum/reciprocal space” may behave as anyonic defects under braiding in momentum space. This applies concretely to nodal points (where electron bands touch or cross) in the momentum space Brillouin torus of topological semi-metals:
here are band crossing points, henceforth called vortices $[$Ahnm Park & Yang 2019$]$
a new type non-Abelian “braiding” of nodal-line rings inside the momentum space $[$Tiwari & Bzdušek 2020$]$
(graphics from SS22)
Curiously, these reciprocal/momemtum space anyons lend themselves to tractable laboratory manipulation in a way that has remained notoriously elusive for “position space” anyons:
Our work opens up routes to readily manipulate Weyl nodes using only slight external parameter changes, paving the way for the practical realization of reciprocal space braiding $[$CBSM22$]$,
specifically
it is possible to controllably braid Kagome band nodes in monolayer $\mathrm{Si}_2 \mathrm{O}_3$ using strain and/or an external electric field $[$PBMS22$]$,
leading to:
new opportunities for exploring non-Abelian braiding of band crossing points (nodes) in reciprocal space, providing an alternative to the real space braiding exploited by other strategies.
Real space braiding is practically constrained to boundary states, which has made experimental observation and manipulation difficult; instead, reciprocal space braiding occurs in the bulk states of the band structures and we demonstrate in this work that this provides a straightforward platform for non-Abelian braiding. $[$PBSM22$]$.
In string theory, defect branes are D-branes or M-branes of codimension=2, such as D7-branes in type IIB string theory or M5-brane-intersections on “M3-branes” in M-theory.
It has been suggest in deBoer & Shigemori 2012, p. 65 that these could behave like anyons. This is further substantiated in SS22. See there for more.
The concept of anyons satisfying braid group statistics originated independently in:
Jon Magne Leinaas, Jan Myrheim, On the theory of identical particles, К теории тождествениых частиц, Nuovo Cim B 37, 1–23 (1977) (doi:10.1007/BF02727953)
G. A. Goldin, R. Menikoff, D. H. Sharp, Representations of a local current algebra in nonsimply connected space and the Aharonov–Bohm effect, J. Math. Phys. 22 1664 (1981) $[$doi:10.1063/1.525110$]$
Frank Wilczek, Magnetic Flux, Angular Momentum, and Statistics, Phys. Rev. Lett. 48 (1982) 1144 (reprinted in Wilczek 1990, p. 163-165) $[$doi:10.1103/PhysRevLett.48.1144$]$
The term anyon was introduced in:
Identification of anyon phases (specifically in the quantum Hall effect) as Berry phases of an adiabatic transport of anyon positions:
The “fictitious gauge field”-method for modelling anyons:
Daniel P. Arovas, Robert Schrieffer, Frank Wilczek, Anthony Zee, Statistical mechanics of anyons, Nuclear Physics B 251 (1985) 117-126 (reprinted in Wilczek 1990, p. 173-182) $[$doi:10.1016/0550-3213(85)90252-4$]$
Yi-Hong Chen, Frank Wilczek, Edward Witten, Bertrand Halperin, On Anyon Superconductivity, International Journal of Modern Physics B 03 07 (1989) 1001-1067 (reprinted in Wilczek 1990, p. 342-408) $[$doi:10.1142/S0217979289000725, pdf$]$
Frank Wilczek, States of Anyon Matter, International Journal of Modern Physics B 05 09 (1991) 1273-1312 $[$doi:10.1142/S0217979291000626$]$
The suggestion that the anyonic ground state-wavefunctions are essentially conformal blocks of 2d CFT (notably for su(2)-anyons):
Gregory Moore, Nicholas Read, Nonabelions in the fractional quantum hall effect, Nuclear Physics B 360 2–3 (1991) 362-396 $[$doi:10.1016/0550-3213(91)90407-O, pdf$]$
Nicholas Read, Edward Rezayi, Beyond paired quantum Hall states: Parafermions and incompressible states in the first excited Landau level, Phys. Rev. B 59 (1999) 8084 $[$doi:10.1103/PhysRevB.59.8084$]$
More comprehensive accounts of anyons:
Frank Wilczek, Fractional Statistics and Anyon Superconductivity, World Scientific (1990) $[$doi:10.1142/0961$]$
Alexei Kitaev, Anyons in an exactly solved model and beyond, Annals of Physics 321 1 (2006) 2-111 $[$doi:10.1016/j.aop.2005.10.005$]$
Rigorous discussion in terms of superselection sectors in algebraic quantum field theory:
Jürg Fröhlich, Pieralberto Marchetti, Quantum field theory of anyons, Lett. Math. Phys. 16 (1988) 347–358 (reprinted in Wilczek 1990, p. 202-213) $[$doi:10.1007/BF00402043$]$
Jürg Fröhlich, Fabrizio Gabbiani, Braid statistics in local quantum theory, Reviews in Mathematical Physics, 2 03 (1990) 251-353 $[$doi:10.1142/S0129055X90000107$]$
Jürg Fröhlich, Fabrizio Gabbiani, Pieralberto Marchetti, Braid statistics in three-dimensional local quantum field theory, in: H.C. Lee (ed.) Physics, Geometry and Topology NATO ASI Series, 238 Springer (1990) $[$doi:10.1007/978-1-4615-3802-8_2, pdf$]$
Klaus Fredenhagen, Karl-Henning Rehren, Bert Schroer, Superselection sectors with braid group statistics and exchange algebras – I: General theory, Comm. Math. Phys. Volume 125, Number 2 (1989), 201-226. (euclid:cmp/1104179464)
Klaus Fredenhagen, Karl-Henning Rehren, Bert Schroer, Superselection sectors with braid group statistics and exchange algebras – II: Geometric aspects and conformal covariance, Reviews in Mathematical PhysicsVol. 04, No. spec01, pp. 113-157 (1992) (doi:10.1142/S0129055X92000170 pdf)
Discussion of anyon-wavefunctions as multi-valued functions on a configuration space of points:
Yong-Shi Wu, Multiparticle Quantum Mechanics Obeying Fractional Statistics, Phys. Rev. Lett. 53 (1984) 111 $[$doi:10.1103/PhysRevLett.53.111, pdf$]$
Tom Imbo, Chandni Shah Imbo, E. C. G. Sudarshan, Identical particles, exotic statistics and braid groups, Physics Letters B 234 1–2, (1990) 103-107 $[$doi:10.1016/0370-2693(90)92010-G, pdf$]$
Garth A. Baker, Geoff S. Canright, Shashikant B. Mulay, Carl Sundberg, On the spectral problem for anyons, Communications in Mathematical Physics 153 (1993) 277–295 $[$doi:10.1007/BF02096644$]$
J. Mund, Robert Schrader, Hilbert Spaces for Nonrelativistic and Relativistic “Free” Plektons (Particles with Braid Group Statistics), in Advances in dynamical systems and quantum physics (Capri, 1993), World Sci. (1995) 235–259 $[$arXiv:hep-th/9310054$]$
followed up by:
Klaus Fredenhagen, Matthias Gaberdiel and Stefan M. Rüger, Scattering states of plektons (particles with braid group statistics) in 2+1 dimensional quantum field theory, Communications in Mathematical Physics 175 (1996) 319–335 $[$doi:10.1007/BF02102411$]$
Gianfausto Dell’Antonio, Rodolfo Figari & Alessandro Teta, Statistics in Space Dimension Two, Letters in Mathematical Physics 40 (1997) 235–256 $[$doi:10.1023/A:1007361832622$]$
Jan Myrheim, Anyons, p. 265-414 in: Topological aspects of low dimensional systems, Les Houches LXIX, Springer (1999) $[$doi:10.1007/3-540-46637-1, pdf$]$
M.V.N. Murthy, Ramamurti Shankar, Exclusion Statistics: From Pauli to Haldane (1999, 2009) $[$dspace:123456789/334, pdf, pdf$]$
G. Date, M.V.N. Murthy, Radhika Vathsan, Classical and Quantum Mechanics of Anyons $[$arXiv:cond-mat/0302019$]$
In condensed matter theory it is folklore that species of anyonic topological order correspond to braided unitary fusion categories/modular tensor categories.
The origin of the claim may be:
Early accounts re-stating this claim (without attribution):
Chetan Nayak, Steven H. Simon, Ady Stern, Michael Freedman, Sankar Das Sarma, pp. 28 of: Non-Abelian Anyons and Topological Quantum Computation, Rev. Mod. Phys. 80 1083 (2008) $[$arXiv:0707.1888, doi:10.1103/RevModPhys.80.1083$]$
Zhenghan Wang, Section 6.3 of: Topological Quantum Computation, CBMS Regional Conference Series in Mathematics 112, AMS (2010) $[$ISBN-13: 978-0-8218-4930-9, pdf$]$
Further discussion (all without attribution):
Eric C. Rowell, Zhenghan Wang, Mathematics of Topological Quantum Computing, Bull. Amer. Math. Soc. 55 (2018), 183-238 (arXiv:1705.06206, doi:10.1090/bull/1605)
Tian Lan, A Classification of (2+1)D Topological Phases with Symmetries $[$arXiv:1801.01210$]$
From categories to anyons: a travelogue $[$arXiv:1811.06670$]$
Colleen Delaney, A categorical perspective on symmetry, topological order, and quantum information (2019) $[$pdf, uc:5z384290$]$
Colleen Delaney, Lecture notes on modular tensor categories and braid group representations (2019) $[$pdf, pdf$]$
Liang Wang, Zhenghan Wang, In and around Abelian anyon models, J. Phys. A: Math. Theor. 53 505203 (2020) $[$doi:10.1088/1751-8121/abc6c0$]$
Parsa Bonderson, Measuring Topological Order, Phys. Rev. Research 3, 033110 (2021) $[$arXiv:2102.05677, doi:10.1103/PhysRevResearch.3.033110$]$
Zhuan Li, Roger S.K. Mong, Detecting topological order from modular transformations of ground states on the torus $[$arXiv:2203.04329$]$
Emphasis that the expected description of anyons by braided fusion categories had remained folklore, together with a list of minimal assumptions that would need to be shown:
Exposition and review:
An argument that the statement at least for SU(2)-anyons does follow from an enhancement of the K-theory classification of topological phases of matter to interacting topological order:
References on anyon-excitations (satisfying braid group statistics) in the quantum Hall effect (for more on the application to topological quantum computation see the references there):
The prediction of abelian anyon-excitations in the quantum Hall effect (i.e. satisfying braid group statistics in 1-dimensional linear representations of the braid group):
B. I. Halperin, Statistics of Quasiparticles and the Hierarchy of Fractional Quantized Hall States, Phys. Rev. Lett. 52, 1583 (1984) (doi:10.1103/PhysRevLett.52.1583)
Erratum Phys. Rev. Lett. 52, 2390 (1984) (doi:10.1103/PhysRevLett.52.2390.4)
Daniel Arovas, J. R. Schrieffer, Frank Wilczek, Fractional Statistics and the Quantum Hall Effect, Phys. Rev. Lett. 53, 722 (1984) $[$doi:10.1103/PhysRevLett.53.722$]$
The original discussion of non-abelian anyon-excitations in the quantum Hall effect (i.e. satisfying braid group statistics in higher dimensional linear representations of the braid group, related to modular tensor categories):
Review:
On anyon-excitations in topological superconductors.
via Majorana zero modes:
Original proposal:
Review:
Sankar Das Sarma, Michael Freedman, Chetan Nayak, Majorana Zero Modes and Topological Quantum Computation, npj Quantum Information 1, 15001 (2015) (nature:npjqi20151)
Nur R. Ayukaryana, Mohammad H. Fauzi, Eddwi H. Hasdeo, The quest and hope of Majorana zero modes in topological superconductor for fault-tolerant quantum computing: an introductory overview (arXiv:2009.07764)
Further development:
via Majorana zero modes restricted to edges of topological insulators:
While the occurrence of anyon-excitations in the quantum Hall effect is a robust theoretical prediction (see the references above), and while the quantum Hall effect itself has long been established in experiment, the actual observation of anyons in these systems is subtle:
An early claim of the observation of non-abelian anyons seems to remain unconfirmed:
The claimed observation of abelian anyons is apparently more securely established:
H. Bartolomei, M. Kumar, R. Bisognin, A. Marguerite, J.-M. Berroir, E. Bocquillon, B. Plaçais, A. Cavanna, Q. Dong, U. Gennser, Y. Jin, G. Fève:
Fractional statistics in anyon collisions, Science 368, 173-177 (2020) (arXiv:2006.13157)
James Nakamura, Shuang Liang, Geoffrey C. Gardner, Michael J. Manfra, Direct observation of anyonic braiding statistics, Nat. Phys. 16, 931–936 (2020). (arXiv:2006.14115, doi:10.1038/s41567-020-1019-1)
Bob Yirka, Best evidence yet for existence of anyons, PhysOrg News July 10, 2020 (phys.org/news/2020-07)
Often the concept of anyons is introduced as if a generalization of perturbative quanta like fundamental bosons and fermions. But many (concepts of) types of anyons are really solitonic$\;$defects such as vortices.
The general concept of braiding of defects in solid state physics:
N. David Mermin, The topological theory of defects in ordered media, Rev. Mod. Phys. 51 (1979) 591 $[$doi:10.1103/RevModPhys.51.591$]$
(including a review of basic homotopy theory)
and more specifically for vortices:
Explicit discussion in terms of anyons:
Alexei Kitaev, Anyons in an exactly solved model and beyond, Annals of Physics 321 1 (2006) 2-111 $[$doi:10.1016/j.aop.2005.10.005$]$
Anyonic particles are best viewed as a kind of topological defects that reveal nontrivial properties of the ground state. $[$p. 4$]$
Concrete vortex$\;$anyons in Bose-Einstein condensates:
B. Paredes, P. Fedichev, J. I. Cirac, P. Zoller 1/2-Anyons in small atomic Bose-Einstein condensates, Phys. Rev. Lett. 87 (2001) 010402 $[$arXiv:cond-mat/0103251, doi:10.1103/PhysRevLett.87.010402$]$
Julien Garaud, Jin Dai, Antti J. Niemi, Vortex precession and exchange in a Bose-Einstein condensate, J. High Energ. Phys. 2021 157 (2021) $[$arXiv:2010.04549$]$
Thomas Mawson, Timothy Petersen, Joost Slingerland, Tapio Simula, Braiding and fusion of non-Abelian vortex anyons, Phys. Rev. Lett. 123 (2019) 140404 $[$doi:10.1103/PhysRevLett.123.140404$]$
and in (other) superfluids:
and in condensates of non-defect anyons:
See also Ahn, Park & Yang 19 who refer to the band nodes in the Brillouin torus of a semi-metal as “vortices in momentum space”.
And see at defect brane.
On non-trivial braiding of modal points in the Brillouin torus of semi-metals (“braiding in momentum space”):
Junyeong Ahn, Sungjoon Park, Bohm-Jung Yang, Failure of Nielsen-Ninomiya theorem and fragile topology in two-dimensional systems with space-time inversion symmetry: application to twisted bilayer graphene at magic angle, Phys. Rev. X 9 (2019) 021013 $[$doi:10.1103/PhysRevX.9.021013, arXiv:1808.05375$]$
here are band crossing points, henceforth called vortices
QuanSheng Wu, Alexey A. Soluyanov, Tomáš Bzdušek, Non-Abelian band topology in noninteracting metals, Science 365 (2019) 1273-1277 (arXiv:1808.07469 ,doi:10.1126/science.aau8740)
Apoorv Tiwari, Tomáš Bzdušek, Non-Abelian topology of nodal-line rings in PT-symmetric systems, Phys. Rev. B 101 (2020) 195130 (doi:10.1103/PhysRevB.101.195130)
a new type non-Abelian “braiding” of nodal-line rings inside the momentum space
Here we report that Weyl points in three-dimensional (3D) systems with $\mathcal{C}_2\mathcal{T}$ symmetry carry non-Abelian topological charges. These charges are transformed via non-trivial phase factors that arise upon braiding the nodes inside the reciprocal momentum space.
Braiding of Dirac points in twisted bilayer graphene:
Jian Kang, Oskar Vafek, Non-Abelian Dirac node braiding and near-degeneracy of correlated phases at odd integer filling in magic angle twisted bilayer graphene, Phys. Rev. B 102 (2020) 035161 $[$arXiv:2002.10360, doi:10.1103/PhysRevB.102.035161$]$
Bin Jiang, Adrien Bouhon, Zhi-Kang Lin, Xiaoxi Zhou, Bo Hou, Feng Li, Robert-Jan Slager, Jian-Hua Jiang Experimental observation of non-Abelian topological acoustic semimetals and their phase transitions, Nature Physics 17 (2021) 1239-1246 $[$arXiv:2104.13397, doi:10.1038/s41567-021-01340-x$]$
(analog realization in phononic crystals)
Here, we consider an exotic type of topological phases beyond the above paradigms that, instead, depend on topological charge conversion processes when band nodes are braided with respect to each other in momentum space or recombined over the Brillouin zone. The braiding of band nodes is in some sense the reciprocal space analog of the non-Abelian braiding of particles in real space.
$[$…$]$
we experimentally observe non-Abelian topological semimetals and their evolutions using acoustic Bloch bands in kagome acoustic metamaterials. By tuning the geometry of the metamaterials, we experimentally confirm the creation, annihilation, moving, merging and splitting of the topological band nodes in multiple bandgaps and the associated non-Abelian topological phase transitions
Haedong Park, Stephan Wong, Xiao Zhang, and Sang Soon Oh, Non-Abelian Charged Nodal Links in a Dielectric Photonic Crystal, ACS Photonics 8 (2021) 2746–2754 [doi:10.1021/acsphotonics.1c00876]
Siyu Chen, Adrien Bouhon, Robert-Jan Slager, Bartomeu Monserrat, Non-Abelian braiding of Weyl nodes via symmetry-constrained phase transitions (formerly: Manipulation and braiding of Weyl nodes using symmetry-constrained phase transitions), Phys. Rev. B 105 (2022) L081117 $[$arXiv:2108.10330, doi:10.1103/PhysRevB.105.L081117$]$
Our work opens up routes to readily manipulate Weyl nodes using only slight external parameter changes, paving the way for the practical realization of reciprocal space braiding.
Bo Peng, Adrien Bouhon, Robert-Jan Slager, Bartomeu Monserrat, Multi-gap topology and non-Abelian braiding of phonons from first principles, Phys. Rev. B 105 (2022) 085115 (arXiv:2111.05872, doi:10.1103/PhysRevB.105.085115)
(analog realization in phononic crystals)
new opportunities for exploring non-Abelian braiding of band crossing points (nodes) in reciprocal space, providing an alternative to the real space braiding exploited by other strategies.
Real space braiding is practically constrained to boundary states, which has made experimental observation and manipulation difficult; instead, reciprocal space braiding occurs in the bulk states of the band structures and we demonstrate in this work that this provides a straightforward platform for non-Abelian braiding.
Bo Peng, Adrien Bouhon, Bartomeu Monserrat, Robert-Jan Slager,Phonons as a platform for non-Abelian braiding and its manifestation in layered silicates, Nature Communications volume 13, Article number: 423 (2022) (doi:10.1038/s41467-022-28046-9)
(analog realization in phononic crystals)
it is possible to controllably braid Kagome band nodes in monolayer $\mathrm{Si}_2 \mathrm{O}_3$ using strain and/or an external electric field.
Haedong Park, Wenlong Gao, Xiao Zhang, Sang Soon Oh, Nodal lines in momentum space: topological invariants and recent realizations in photonic and other systems, Nanophotonics 11 11 (2022) 2779–2801 $[$doi:10.1515/nanoph-2021-0692$]$
(analog realization in photonic crystals)
Adrien Bouhon, Robert-Jan Slager, Multi-gap topological conversion of Euler class via band-node braiding: minimal models, PT-linked nodal rings, and chiral heirs $[$arXiv:2203.16741$]$
See also:
Incidentally, references indicating that the required toroidal (or yet higher genus) geometry for anyonic topological order in position space is dubious (as opposed to the evident toroidal geometry of the momentum-space Brillouin torus): Lan 19, p. 1, ….
The idea of topological quantum computation via the Chern-Simons theory of anyons (e.g. in the quantum Hall effect) is due to:
Alexei Kitaev, Fault-tolerant quantum computation by anyons, Annals Phys. 303 (2003) 2-30 (arXiv:quant-ph/9707021, doi:10.1016/S0003-4916(02)00018-0)
Michael Freedman, Alexei Kitaev, Michael Larsen, Zhenghan Wang, Topological quantum computation, Bull. Amer. Math. Soc. 40 (2003), 31-38 (arXiv:quant-ph/0101025, doi:10.1090/S0273-0979-02-00964-3, pdf)
Michael Freedman, Michael Larsen, Zhenghan Wang, A modular functor which is universal for quantum computation, Communications in Mathematical Physics. 227 3 (2002) 605-622 $[$arXiv:quant-ph/0001108, doi:10.1007/s002200200645$]$
(specifically via su(2)-anyons)
D. Melnikov, A. Mironov, S. Mironov, A. Morozov, An. Morozov, Towards topological quantum computer, Nucl. Phys. B926 (2018) 491-508 (arXiv:1703.00431, doi:10.1016/j.nuclphysb.2017.11.016)
Textbook accounts:
Zhenghan Wang, Topological Quantum Computation, CBMS Regional Conference Series in Mathematics 112, AMS 2010 (ISBN-13: 978-0-8218-4930-9, pdf)
Jiannis K. Pachos, Introduction to Topological Quantum Computation, Cambridge University Press (2012) $[$doi:10.1017/CBO9780511792908$]$
Tudor D. Stanescu, Part IV of: Introduction to Topological Quantum Matter & Quantum Computation, CRC Press 2020 (ISBN:9780367574116)
Steven H. Simon, Topological Quantum, 2021 $[$pdf, webpage$]$
Review:
Chetan Nayak, Steven H. Simon, Ady Stern, Michael Freedman, Sankar Das Sarma, Non-Abelian Anyons and Topological Quantum Computation, Rev. Mod. Phys. 80 1083 (2008) $[$arXiv:0707.1888, doi:10.1103/RevModPhys.80.1083$]$
Ady Stern, Netanel H. Lindner, Topological Quantum Computation – From Basic Concepts to First Experiments, Science 339 6124 (2013) 1179-1184 (doi:10.1126/science.1231473)
Eric C. Rowell, An Invitation to the Mathematics of Topological Quantum Computation, J. Phys.: Conf. Ser. 698 (2016) 012012 (doi:10.1088/1742-6596/698/1/012012)
Ville Lahtinen, Jiannis K. Pachos, A Short Introduction to Topological Quantum Computation, SciPost Phys. 3 021 (2017) (arXiv:1705.04103)
Eric C. Rowell, Zhenghan Wang, Mathematics of Topological Quantum Computing, Bull. Amer. Math. Soc. 55 (2018), 183-238 (arXiv:1705.06206, doi:10.1090/bull/1605)
Bernard Field, Tapio Simula, Introduction to topological quantum computation with non-Abelian anyons, Quantum Science and Technology 3 (2018) 045004 (arXiv:1802.06176, doi:10.1088/2058-9565/aacad2)
Muhammad Ilyas, Quantum Field Theories, Topological Materials, and Topological Quantum Computing $[$arXiv:2208.09707$]$
Eric C. Rowell, Braids, Motions and Topological Quantum Computing $[$arXiv:2208.11762$]$
Focus on abelian anyons:
Jiannis K. Pachos, Quantum computation with abelian anyons on the honeycomb lattice, International Journal of Quantum Information 4 6 (2006) 947-954 (arXiv:quant-ph/0511273)
James Robin Wootton, Dissecting Topological Quantum Computation, 2010 (pdf, pdf)
“non-Abelian anyons are usually assumed to be better suited to the task. Here we challenge this view, demonstrating that Abelian anyon models have as much potential as some simple non-Abelian models.”
Wade Bloomquist, Zhenghan Wang, On Topological Quantum Computing With Mapping Class Group Representations, J. Phys. A: Math. Theor. 52 (2019) 015301 (arXiv:1805.04622, doi:10.1088/1751-8121/aaeea1)
Seth Lloyd, Quantum computation with abelian anyons, Quantum Information Processing 1 1/2 (2002) (arXiv:quant-ph/0004010, doi:10.1023/A:1019649101654)
Realization in experiment:
Daniel Nigg, Markus Mueller, Esteban A. Martinez, Philipp Schindler, Markus Hennrich, Thomas Monz, Miguel A. Martin-Delgado, Rainer Blatt,
Experimental Quantum Computations on a Topologically Encoded Qubit, Science 18 Jul 2014: Vol. 345, Issue 6194, pp. 302-305 (arXiv:1403.5426, doi:10.1126/science.1253742)
(for quantum error correction)
On linear representations of braid groups (see also at braid group statistics and interpretation as quantum gates in topological quantum computation):
Review:
Camilo Arias Abad, Introduction to representations of braid groups, Rev. colomb. mat. vol.49 no.1 (2015) (arXiv:1404.0724, doi:10.15446/recolma.v49n1.54160)
Toshitake Kohno, Introduction to representation theory of braid groups, Peking 2018 (pdf, pdf)
in relation to modular tensor categories:
Braid representations from the monodromy of the Knizhnik-Zamolodchikov connection on bundles of conformal blocks over configuration spaces of points:
Ivan Todorov, Ludmil Hadjiivanov, Monodromy Representations of the Braid Group, Phys. Atom. Nucl. 64 (2001) 2059-2068; Yad.Fiz. 64 (2001) 2149-2158 [arXiv:hep-th/0012099, doi:10.1134/1.1432899]
Ivan Marin, Sur les représentations de Krammer génériques, Annales de l’Institut Fourier, 57 6 (2007) 1883-1925 [numdam:AIF_2007__57_6_1883_0]
and understood in terms of anyon statistics:
Braid representations seen inside the topological K-theory of the braid group‘s classifying space:
Alejandro Adem, Daniel C. Cohen, Frederick R. Cohen, On representations and K-theory of the braid groups, Math. Ann. 326 (2003) 515-542 (arXiv:math/0110138, doi:10.1007/s00208-003-0435-8)
Frederick R. Cohen, Section 3 of: On braid groups, homotopy groups, and modular forms, in: J.M. Bryden (ed.), Advances in Topological Quantum Field Theory, Kluwer 2004, 275–288 (pdf)
See also:
As quantum gates for topological quantum computation with anyons:
Louis H. Kauffman, Samuel J. Lomonaco, Braiding Operators are Universal Quantum Gates, New Journal of Physics, Volume 6, January 2004 (arXiv:quant-ph/0401090, doi:10.1088/1367-2630/6/1/134)
Samuel J. Lomonaco, Louis Kauffman, Topological Quantum Computing and the Jones Polynomial, Proc. SPIE 6244, Quantum Information and Computation IV, 62440Z (2006) (arXiv:quant-ph/0605004)
(braid group representation serving as a topological quantum gate to compute the Jones polynomial)
Louis H. Kauffman, Samuel J. Lomonaco, Topological quantum computing and $SU(2)$ braid group representations, Proceedings Volume 6976, Quantum Information and Computation VI; 69760M (2008) (doi:10.1117/12.778068, rg:228451452)
C.-L. Ho, A.I. Solomon, C.-H.Oh, Quantum entanglement, unitary braid representation and Temperley-Lieb algebra, EPL 92 (2010) 30002 (arXiv:1011.6229)
Louis H. Kauffman, Majorana Fermions and Representations of the Braid Group, International Journal of Modern Physics AVol. 33, No. 23, 1830023 (2018) (arXiv:1710.04650, doi:10.1142/S0217751X18300235)
Introduction and review:
Colleen Delaney, Eric C. Rowell, Zhenghan Wang, Local unitary representations of the braid group and their applications to quantum computing, Revista Colombiana de Matemáticas(2017), 50 (2):211 (arXiv:1604.06429, doi:10.15446/recolma.v50n2.62211)
Eric C. Rowell, Braids, Motions and Topological Quantum Computing [arXiv:2208.11762]
Realization of Fibonacci anyons on quasicrystal-states:
Realization on supersymmetric spin chains:
On approximating given quantum gates by (i.e. compiling them to) cicuits of anyon braid gates (generally considered for su(2)-anyons and here mostly for universal Fibonacci anyons, to some extent also for non-universal Majorana anyons):
Nicholas E. Bonesteel, Layla Hormozi, Georgios Zikos, Steven H. Simon, Braid Topologies for Quantum Computation, Phys. Rev. Lett. 95 140503 (2005) $[$arXiv:quant-ph/0505065, doi:10.1103/PhysRevLett.95.140503$]$
Layla Hormozi, Georgios Zikos, Nicholas E. Bonesteel, Steven H. Simon, Topological Quantum Compiling, Phys. Rev. B 75 165310 (2007) $[$arXiv:quant-ph/0610111, doi:10.1103/PhysRevB.75.165310$]$
Layla Hormozi, Nicholas E. Bonesteel, Steven H. Simon, Topological Quantum Computing with Read-Rezayi States, Phys. Rev. Lett. 103 160501 (2009) $[$doi:10.1103/PhysRevLett.103.160501, arXiv:0903.2239$]$
M. Baraban, Nicholas E. Bonesteel, Steven H. Simon, Resources required for topological quantum factoring, Phys. Rev. A 81 062317 (2010) $[$doi:10.1103/PhysRevA.81.062317, arXiv:1002.0537$]$
(focus on compiling Shor's algorithm)
Vadym Kliuchnikov, Alex Bocharov, Krysta M. Svore, Asymptotically Optimal Topological Quantum Compiling, Phys. Rev. Lett. 112 140504 (2014) $[$arXiv:1310.4150, journal: doi:10.1103/PhysRevLett.112.140504, talk recording: doi:10.48660/13100129$]$
J. W. Brunekreef, Topological Quantum Computation and Quantum Compilation (2014) $[$studenttheses.uu.nl:20.500.12932/17738
Yuan-Hang Zhang, Pei-Lin Zheng, Yi Zhang, Dong-Ling Deng, Topological Quantum Compiling with Reinforcement Learning, Phys. Rev. Lett. 125 170501 (2020) $[$doi:2004.04743, doi:10.1103/PhysRevLett.125.170501$]$
Emil Génetay Johansen and Tapio Simula, Fibonacci Anyons Versus Majorana Fermions: A Monte Carlo Approach to the Compilation of Braid Circuits in $SU(2)_k$ Anyon Models, PRX Quantum 2 010334 (2021) $[$doi:10.1103/PRXQuantum.2.010334$]$
Cheng-Qian Xu, D. L. Zhou, Quantum teleportation using Ising anyons, Phys. Rev. A 106 012413 (2022) $[$arXiv:2201.11923, doi:10.1103/PhysRevA.106.012413$]$
(focus on implemening the quantum teleportation-protocol with Ising anyons)
Approximating all topological quantum gates by just the weaves among all braids:
Steven H. Simon, Nick E. Bonesteel, Michael H. Freedman, N. Petrovic, Layla Hormozi, Topological Quantum Computing with Only One Mobile Quasiparticle, Phys. Rev. Lett. 96 (2006) 070503 (arXiv:quant-ph/0509175, doi:10.1103/PhysRevLett.96.070503)
Layla Hormozi, Georgios Zikos, Nick E. Bonesteel, Steven H. Simon, Topological quantum compiling, Phys. Rev. B 75, 165310 (doi:10.1103/PhysRevB.75.165310, arXiv:quant-ph/0610111)
Mohamed Taha Rouabah, Compiling single-qubit braiding gate for Fibonacci anyons topological quantum computation (arXiv:2008.03542)
Last revised on September 2, 2022 at 04:55:17. See the history of this page for a list of all contributions to it.