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In mathematics, **E _{8}** is any of several closely related exceptional simple Lie groups, linear algebraic groups or Lie algebras of dimension 248; the same notation is used for the corresponding root lattice, which has rank 8. The designation E

- Basic description
- Real and complex forms
- E8 as an algebraic group
- Constructions
- Geometry
- E8 root system
- Construction
- Dynkin diagram
- Cartan matrix
- Simple roots
- Weyl group
- E8 root lattice
- Simple subalgebras of E8
- Chevalley groups of type E8
- Subgroups, subalgebras, and extensions
- Applications
- History
- See also
- Footnotes
- References
- External links
- Lusztig–Vogan polynomial calculation
- Other links

The Lie group E_{8} has dimension 248. Its rank, which is the dimension of its maximal torus, is eight.

Therefore, the vectors of the root system are in eight-dimensional Euclidean space: they are described explicitly later in this article. The Weyl group of E_{8}, which is the group of symmetries of the maximal torus which are induced by conjugations in the whole group, has order 2^{14} 3^{5} 5^{2} 7 = 696729600.

The compact group E_{8} is unique among simple compact Lie groups in that its non-trivial representation of smallest dimension is the adjoint representation (of dimension 248) acting on the Lie algebra E_{8} itself; it is also the unique one which has the following four properties: trivial center, compact, simply connected, and simply laced (all roots have the same length).

There is a Lie algebra E_{k} for every integer *k* ≥ 3. The largest value of *k* for which E_{k} is finite-dimensional is *k* = 8, that is, E_{k} is infinite-dimensional for any *k* > 8.

There is a unique complex Lie algebra of type E_{8}, corresponding to a complex group of complex dimension 248. The complex Lie group E_{8} of complex dimension 248 can be considered as a simple real Lie group of real dimension 496. This is simply connected, has maximal compact subgroup the compact form (see below) of E_{8}, and has an outer automorphism group of order 2 generated by complex conjugation.

As well as the complex Lie group of type E_{8}, there are three real forms of the Lie algebra, three real forms of the group with trivial center (two of which have non-algebraic double covers, giving two further real forms), all of real dimension 248, as follows:

- The compact form (which is usually the one meant if no other information is given), which is simply connected and has trivial outer automorphism group.
- The split form, EVIII (or E
_{8(8)}), which has maximal compact subgroup Spin(16)/(**Z**/2**Z**), fundamental group of order 2 (implying that it has a double cover, which is a simply connected Lie real group but is not algebraic, see below) and has trivial outer automorphism group. - EIX (or E
_{8(−24)}), which has maximal compact subgroup E_{7}×SU(2)/(−1,−1), fundamental group of order 2 (again implying a double cover, which is not algebraic) and has trivial outer automorphism group.

For a complete list of real forms of simple Lie algebras, see the list of simple Lie groups.

By means of a Chevalley basis for the Lie algebra, one can define E_{8} as a linear algebraic group over the integers and, consequently, over any commutative ring and in particular over any field: this defines the so-called split (sometimes also known as “untwisted”) form of E_{8}. Over an algebraically closed field, this is the only form; however, over other fields, there are often many other forms, or “twists” of E_{8}, which are classified in the general framework of Galois cohomology (over a perfect field *k*) by the set H^{1}(*k*,Aut(E_{8})) which, because the Dynkin diagram of E_{8} (see below) has no automorphisms, coincides with H^{1}(*k*,E_{8}).^{ [1] }

Over **R**, the real connected component of the identity of these algebraically twisted forms of E_{8} coincide with the three real Lie groups mentioned above, but with a subtlety concerning the fundamental group: all forms of E_{8} are simply connected in the sense of algebraic geometry, meaning that they admit no non-trivial algebraic coverings; the non-compact and simply connected real Lie group forms of E_{8} are therefore not algebraic and admit no faithful finite-dimensional representations.

Over finite fields, the Lang–Steinberg theorem implies that H^{1}(*k*,E_{8})=0, meaning that E_{8} has no twisted forms: see below.

The characters of finite dimensional representations of the real and complex Lie algebras and Lie groups are all given by the Weyl character formula. The dimensions of the smallest irreducible representations are (sequence A121732 in the OEIS ):

- 1, 248, 3875, 27000, 30380, 147250, 779247, 1763125, 2450240, 4096000, 4881384, 6696000, 26411008, 70680000, 76271625, 79143000, 146325270, 203205000, 281545875, 301694976, 344452500, 820260000, 1094951000, 2172667860, 2275896000, 2642777280, 2903770000, 3929713760, 4076399250, 4825673125, 6899079264, 8634368000 (twice), 12692520960…

The 248-dimensional representation is the adjoint representation. There are two non-isomorphic irreducible representations of dimension 8634368000 (it is not unique; however, the next integer with this property is 175898504162692612600853299200000 (sequence A181746 in the OEIS )). The fundamental representations are those with dimensions 3875, 6696000, 6899079264, 146325270, 2450240, 30380, 248 and 147250 (corresponding to the eight nodes in the Dynkin diagram in the order chosen for the Cartan matrix below, i.e., the nodes are read in the seven-node chain first, with the last node being connected to the third).

The coefficients of the character formulas for infinite dimensional irreducible representations of E_{8} depend on some large square matrices consisting of polynomials, the Lusztig–Vogan polynomials, an analogue of Kazhdan–Lusztig polynomials introduced for reductive groups in general by George Lusztig and David Kazhdan (1983). The values at 1 of the Lusztig–Vogan polynomials give the coefficients of the matrices relating the standard representations (whose characters are easy to describe) with the irreducible representations.

These matrices were computed after four years of collaboration by a group of 18 mathematicians and computer scientists, led by Jeffrey Adams, with much of the programming done by Fokko du Cloux. The most difficult case (for exceptional groups) is the split real form of E_{8} (see above), where the largest matrix is of size 453060×453060. The Lusztig–Vogan polynomials for all other exceptional simple groups have been known for some time; the calculation for the split form of *E*_{8} is far longer than any other case. The announcement of the result in March 2007 received extraordinary attention from the media (see the external links), to the surprise of the mathematicians working on it.

The representations of the E_{8} groups over finite fields are given by Deligne–Lusztig theory.

One can construct the (compact form of the) E_{8} group as the automorphism group of the corresponding **e**_{8} Lie algebra. This algebra has a 120-dimensional subalgebra **so**(16) generated by *J*_{ij} as well as 128 new generators *Q*_{a} that transform as a Weyl–Majorana spinor of **spin**(16). These statements determine the commutators

as well as

while the remaining commutators (not anticommutators!) between the spinor generators are defined as

It is then possible to check that the Jacobi identity is satisfied.

The compact real form of E_{8} is the isometry group of the 128-dimensional exceptional compact Riemannian symmetric space EVIII (in Cartan's classification). It is known informally as the "octooctonionic projective plane" because it can be built using an algebra that is the tensor product of the octonions with themselves, and is also known as a Rosenfeld projective plane, though it does not obey the usual axioms of a projective plane. This can be seen systematically using a construction known as the *magic square*, due to Hans Freudenthal and Jacques Tits ( Landsberg & Manivel 2001 ).

A root system of rank *r* is a particular finite configuration of vectors, called *roots*, which span an *r*-dimensional Euclidean space and satisfy certain geometrical properties. In particular, the root system must be invariant under reflection through the hyperplane perpendicular to any root.

The **E _{8} root system** is a rank 8 root system containing 240 root vectors spanning

In the so-called *even coordinate system*, E_{8} is given as the set of all vectors in **R**^{8} with length squared equal to 2 such that coordinates are either all integers or all half-integers and the sum of the coordinates is even.

Explicitly, there are 112 roots with integer entries obtained from

by taking an arbitrary combination of signs and an arbitrary permutation of coordinates, and 128 roots with half-integer entries obtained from

by taking an even number of minus signs (or, equivalently, requiring that the sum of all the eight coordinates be even). There are 240 roots in all.

The 112 roots with integer entries form a D_{8} root system. The E_{8} root system also contains a copy of A_{8} (which has 72 roots) as well as E_{6} and E_{7} (in fact, the latter two are usually *defined* as subsets of E_{8}).

In the *odd coordinate system*, E_{8} is given by taking the roots in the even coordinate system and changing the sign of any one coordinate. The roots with integer entries are the same while those with half-integer entries have an odd number of minus signs rather than an even number.

The Dynkin diagram for E_{8} is given by .

This diagram gives a concise visual summary of the root structure. Each node of this diagram represents a simple root. A line joining two simple roots indicates that they are at an angle of 120° to each other. Two simple roots which are not joined by a line are orthogonal.

The Cartan matrix of a rank *r* root system is an *r × r* matrix whose entries are derived from the simple roots. Specifically, the entries of the Cartan matrix are given by

where ( , ) is the Euclidean inner product and *α _{i}* are the simple roots. The entries are independent of the choice of simple roots (up to ordering).

The Cartan matrix for E_{8} is given by

The determinant of this matrix is equal to 1.

A set of simple roots for a root system Φ is a set of roots that form a basis for the Euclidean space spanned by Φ with the special property that each root has components with respect to this basis that are either all nonnegative or all nonpositive.

Given the E_{8} Cartan matrix (above) and a Dynkin diagram node ordering of:

One choice of simple roots is given by the rows of the following matrix:

With this numbering of nodes in the Dynkin diagram, the highest root in the root system has Coxeter labels (2, 3, 4, 5, 6, 4, 2, 3). Using this representation of the simple roots, the lowest root is given by

The only simple root that can be added to the lowest root to obtain another root is the one corresponding to node 1 in this labeling of the Dynkin diagram — as is to be expected from the affine Dynkin diagram for . The Hasse diagram to the right enumerates the 120 roots of positive height relative to any particular choice of simple roots consistent with this node numbering.

Note that the Hasse diagram does not represent the full Lie algebra, or even the full root system. The 120 roots of negative height relative to the same set of simple roots can be adequately represented by a second copy of the Hasse diagram with the arrows reversed; but it is less straightforward to connect these two diagrams via a basis for the eight-dimensional Cartan subalgebra. In the notation of the exposition of Chevalley generators and Serre relations: Insofar as an arrow represents the Lie bracket by the generator associated with a simple root, each root in the height -1 layer of the reversed Hasse diagram must correspond to some and can have only one upward arrow, connected to a node in the height 0 layer representing the element of the Cartan subalgebra given by . But the upward arrows from the height 0 layer must then represent , where is (the transpose of) the Cartan matrix. One could draw multiple upward arrows from each associated with all for which is nonzero; but this neither captures the numerical entries in the Cartan matrix nor reflects the fact that each only has nonzero Lie bracket with one degree of freedom in the Cartan subalgebra (just not the same degree of freedom as ).

More fundamentally, this organization implies that the *span* of the generators designated as "the" Cartan subalgebra is somehow inherently special, when in most applications, any mutually commuting set of eight of the 248 Lie algebra generators (of which there are many!) — or any eight linearly independent, mutually commuting Lie derivations on any manifold with E_{8} structure — would have served just as well. Once a Cartan subalgebra has been selected (or defined *a priori*, as in the case of a lattice), a basis of "Cartan generators" (the among the Chevalley generators) and a root system are a useful way to describe structure *relative to this subalgebra*. But the root system map is not the Lie algebra (let alone group!) territory. Given a set of Chevalley generators, most degrees of freedom in a Lie algebra and their sparse Lie brackets with can be represented schematically as circles and arrows, but this simply breaks down on the chosen Cartan subalgebra. Such are the hazards of schematic visual representations of mathematical structures.

The Weyl group of E_{8} is of order 696729600, and can be described as O^{+}_{8}(2): it is of the form 2.*G*.2 (that is, a stem extension by the cyclic group of order 2 of an extension of the cyclic group of order 2 by a group *G*) where *G* is the unique simple group of order 174182400 (which can be described as PSΩ_{8}^{+}(2)).^{ [3] }

The integral span of the E_{8} root system forms a lattice in **R**^{8} naturally called the ** E _{8} root lattice **. This lattice is rather remarkable in that it is the only (nontrivial) even, unimodular lattice with rank less than 16.

The Lie algebra E_{8} contains as subalgebras all the exceptional Lie algebras as well as many other important Lie algebras in mathematics and physics. The height of the Lie algebra on the diagram approximately corresponds to the rank of the algebra. A line from an algebra down to a lower algebra indicates that the lower algebra is a subalgebra of the higher algebra.

Chevalley (1955) showed that the points of the (split) algebraic group E_{8} (see above) over a finite field with *q* elements form a finite Chevalley group, generally written E_{8}(*q*), which is simple for any *q*,^{ [4] }^{ [5] } and constitutes one of the infinite families addressed by the classification of finite simple groups. Its number of elements is given by the formula (sequence A008868 in the OEIS ):

The first term in this sequence, the order of E_{8}(2), namely 337804753143634806261388190614085595079991692242467651576160959909068800000 ≈ 3.38×10^{74}, is already larger than the size of the Monster group. This group E_{8}(2) is the last one described (but without its character table) in the ATLAS of Finite Groups.^{ [6] }

The Schur multiplier of E_{8}(*q*) is trivial, and its outer automorphism group is that of field automorphisms (i.e., cyclic of order *f* if *q*=*p ^{f}* where

Lusztig (1979) described the unipotent representations of finite groups of type *E*_{8}.

The smaller exceptional groups E_{7} and E_{6} sit inside E_{8}. In the compact group, both E_{6}×SU(3)/(**Z**/3**Z**) and E_{7}×SU(2)/(+1,−1) are maximal subgroups of E_{8}.

The 248-dimensional adjoint representation of E_{8} may be considered in terms of its restricted representation to the first of these subgroups. It transforms under E_{6}×SU(3) as a sum of tensor product representations, which may be labelled as a pair of dimensions as (78,1) + (1,8) + (__27__,3) + (27,__3__). (Since the maximal subgroup is actually the quotient of this group product by a finite group, these notations may strictly be taken as indicating the infinitesimal (Lie algebra) representations.) Since the adjoint representation can be described by the roots together with the generators in the Cartan subalgebra, we may choose a particular E_{6} root system within E_{8} and decompose the sum representation relative to this E_{6}. In this description,

- (78,1), a copy of , consists of the 72 roots with (−1⁄2,−1⁄2,−1⁄2), (0,0,0), or (1⁄2,1⁄2,1⁄2) in the last three dimensions, together with five Cartan generators corresponding to the first five dimensions and one Cartan generator corresponding to an equally weighted sum of the last three Cartan generators of the E
_{8}system; - (1,8), a copy of , consists of the six roots with permutations of (0,1,−1) in the last three dimensions, together with two Cartan generators corresponding to the two trace-free combinations of the last three Cartan generators of the E
_{8}system; - (
__27__,3) consists of all roots with permutations of (-1,0,0), (−1⁄2,1⁄2,1⁄2), or (0,1,1) in the last three dimensions; and - (27,
__3__) consists of all roots with permutations of (1,0,0), (1⁄2,−1⁄2,−1⁄2), or (0,-1,-1) in the last three dimensions.

The 248-dimensional adjoint representation of E_{8}, when similarly restricted to the second maximal subgroup, transforms under E_{7}×SU(2) as: (133,1) + (1,3) + (56,2). We may again see the decomposition by looking at the roots together with the generators in the Cartan subalgebra. In this description,

- (133,1), a copy of , consists of the 126 roots with (−1,−1), (−1⁄2,−1⁄2), (0,0), (1⁄2,1⁄2), or (1,1) in the last two dimensions, together with six Cartan generators corresponding to the first six dimensions and one Cartan generator corresponding to an equally weighted sum of the last two Cartan generators of the E
_{8}system; - (1,3), a copy of , consists of the two roots (0,0,0,0,0,0,1,−1), (0,0,0,0,0,0,−1,1), together with one Cartan generator corresponding to the trace-free combination of the last two Cartan generators of the E
_{8}system; and - (56,2) consists of all roots with permutations of (0,-1), (1⁄2,−1⁄2), or (1,0) in the last two dimensions.

The connection between these two descriptions is given by the graded exceptional Lie algebra constructions of J. Tits and B. N. Allison. Any 27-dimensional representation of E_{6} can be equipped with a non-associative (but strictly power-associative) Jordan product operation to form an Albert algebra (an important exceptional case in algebraic constructions). The Kantor–Koecher–Tits construction applied to this Albert algebra recovers the 78-dimensional as the reduced structure algebra of the Albert algebra. This , together with the 27 and __27__ representations and the grade operator (the element of the Cartan subalgebra with weight -1 on the 27, +1 on the __27__, and 0 on the 78), forms an 3-graded Lie algebra. A complete exposition of this construction may be found in standard texts on Jordan algebras such as Jacobson 1968 or McCrimmon 2004.

Starting this 3-graded Lie algebra construction with any particular 27-dimensional representation, embedded within , of any particular E_{6} subgroup of E_{8} produces the corresponding subalgebra. The particular in the E_{7}×SU(2) decomposition given above corresponds to choosing the 27 consisting of all roots with (1,0,0), (1⁄2,-1⁄2,-1⁄2), or (0,-1,-1) in the last three dimensions (in order), with the grade operator having weight (-1,1⁄2,1⁄2) in these dimensions; or equivalently to choosing the "__27__" consisting of all roots with (-1,0,0), (−1⁄2,1⁄2,1⁄2), or (0,1,1) in the last three dimensions (in order), with the grade operator having weight (1,-1⁄2,-1⁄2) in these dimensions. Note that there is nothing special about this choice of dimensions — the within which the root system is embedded is not the set of eight independent but non-orthogonal axes corresponding to the simple roots, and any three dimensions will do — and there are also constructions using other equivalent groupings of roots. What matters is that the kernel of the Lie bracket with the generator chosen as the "grade operator" be an subalgebra (plus a central associated with the grade operator itself and the remaining generator of the Cartan subalgebra), not , , , *etc.*

(In the simple Lie algebra case, the sign of the grade of the 27 versus the __27__ representation is a matter of convention, as is the scale of the grading. However, choosing -1 as the grade of the 27-dimensional "vector" representation is consistent with an extension of the 3-graded algebra to higher positive grades via the exterior algebra over the __27__ "covector" representation. The "vector" representation then lies, not in this nonnegative-graded exterior algebra, but in the graded algebra of derivations over the exterior algebra; the 78-dimensional is the grade 0 subalgebra (a subalgebra of the inner derivations by "vector-valued 1-forms") of this graded algebra of derivations. For details on how this asymmetric structure works starting from a general 3-graded algebra, see references at Frölicher–Nijenhuis bracket. The relevance of this observation to E_{8} is simply that E_{7} and E_{8} are their own clusters of structures, distinguished as exceptional simple Lie groups/algebras, and that any particular reconstruction of them using representations of their subgroups/subalgebras will have extensions beyond the motivating case. Varying conventions of sign, scale, and conjugate relationship in the literature are due not just to inaccuracies but also to the directions in which the authors seek to extend their constructions.)

The distinguished in the E_{7}×SU(2) decomposition above is then given by the subalgebra of that commutes with the grade operator (which lies in the Cartan subalgebra of this ). Of the four remaining roots in the , two are of grade 1⁄2 and two are of grade -1⁄2. In the convention where the 27 of E_{6} used to construct the has grade -1 and the __27__ has grade +1, the other two 27's have grade +1⁄2 and the other two __27__'s have grade -1⁄2, as is apparent from permuting the values of the last three roots in the description above. Grouping these 4×(1+27)=112 generators to form the grade +1⁄2 and -1⁄2 subspaces of (relative to the original choice of grade operator within ), each subspace may be given a quite particular non-associative (nor even power-associative) product operation, resulting in two copies of Brown's 56-dimensional structurable algebra. Allison's 5-graded Lie algebra construction based on this structurable algebra recovers the original . (Allison's 5-grading differs from the above by a factor -2.) Grouping these generators differently, based on their weights relative to the Cartan generator of the *orthogonal* to , gives two 56-dimensional subspaces which each carry the lowest-dimensional non-trivial irreducible representation of E_{7}. Either of these may be combined with the Cartan generator to form a 57-dimensional Heisenberg algebra, and adjoining this to produces the (non-simple) Lie algebra E7½ described by Landsberg and Manivel.

From the perspective in which the 27-dimensional grade -1 subspace of (relative to a choice of grade operator) plays the role of "vector" representation of E_{6} and the __27__ with roots opposite it plays the role of "covector" representation, it is natural to look for "spinor" representations in the grade +1⁄2 and -1⁄2 subspaces, or in some other combination of the (__27__,3) and (27,__3__) representations of E_{6}×SU(3), and to attempt to relate these to geometrical spinors in the Clifford algebra sense as employed in quantum field theory. Variations on this idea are common in the physics literature. See Distler and Garibaldi 2009 for discussion of the mathematical obstacles to constructing a *chiral* gauge theory based on E_{8}. The structure of relative to its subalgebra, together with the conventional scaling of elements of the Cartan subalgebra, invites extensions by geometric analogy but does not necessarily imply a relationship to low-dimensional geometry or low-energy physics. The same may be said of connections to Jordan and Heisenberg algebras, whose historical origins are intertwined with the development of quantum mechanics. Not every visual representation evocative of a tobacco pipe will hold tobacco.

The finite quasisimple groups that can embed in (the compact form of) E_{8} were found by Griess & Ryba (1999).

The Dempwolff group is a subgroup of (the compact form of) E_{8}. It is contained in the Thompson sporadic group, which acts on the underlying vector space of the Lie group E_{8} but does not preserve the Lie bracket. The Thompson group fixes a lattice and does preserve the Lie bracket of this lattice mod 3, giving an embedding of the Thompson group into E_{8}(**F**_{3}).

The embeddings of the maximal subgroups of E_{8} up to dimension 248 are shown to the right.

The E_{8} Lie group has applications in theoretical physics and especially in string theory and supergravity. E_{8}×E_{8} is the gauge group of one of the two types of heterotic string and is one of two anomaly-free gauge groups that can be coupled to the *N* = 1 supergravity in ten dimensions. E_{8} is the U-duality group of supergravity on an eight-torus (in its split form).

One way to incorporate the standard model of particle physics into heterotic string theory is the symmetry breaking of E_{8} to its maximal subalgebra SU(3)×E_{6}.

In 1982, Michael Freedman used the E_{8} lattice to construct an example of a topological 4-manifold, the E_{8} manifold, which has no smooth structure.

Antony Garrett Lisi's incomplete "An Exceptionally Simple Theory of Everything" attempts to describe all known fundamental interactions in physics as part of the E_{8} Lie algebra.^{ [7] }^{ [8] }

R.Coldea,D. A. Tennant,andE. M. Wheeleret al. ( 2010 ) reported an experiment where the electron spins of a cobalt-niobium crystal exhibited, under certain conditions, two of the eight peaks related to E_{8} that were predicted by Zamolodchikov (1989).^{ [9] }^{ [10] }

WilhelmKilling ( 1888a , 1888b , 1889 , 1890 ) discovered the complex Lie algebra E_{8} during his classification of simple compact Lie algebras, though he did not prove its existence, which was first shown by Élie Cartan. Cartan determined that a complex simple Lie algebra of type E_{8} admits three real forms. Each of them gives rise to a simple Lie group of dimension 248, exactly one of which (as for any complex simple Lie algebra) is compact. Chevalley (1955) introduced algebraic groups and Lie algebras of type E_{8} over other fields: for example, in the case of finite fields they lead to an infinite family of finite simple groups of Lie type. E_{8} continues to be an area of active basic research by Atlas of Lie Groups and Representations, which aims to determine the unitary representations of all the Lie groups.^{ [11] }

- ↑ Платонов, Владимир П.; Рапинчук, Андрей С. (1991),
*Алгебраические группы и теория чисел*, Наука, ISBN 5-02-014191-7 (English translation: Platonov, Vladimir P.; Rapinchuk, Andrei S. (1994),*Algebraic groups and number theory*, Academic Press, ISBN 0-12-558180-7 ), §2.2.4 - ↑ "The 600-Cell (Part 1)". December 16, 2017.
- ↑ Conway, John Horton; Curtis, Robert Turner; Norton, Simon Phillips; Parker, Richard A; Wilson, Robert Arnott (1985),
*Atlas of Finite Groups: Maximal Subgroups and Ordinary Characters for Simple Groups*, Oxford University Press, p. 85, ISBN 0-19-853199-0 - ↑ Carter, Roger W. (1989),
*Simple Groups of Lie Type*, Wiley Classics Library, John Wiley & Sons, ISBN 0-471-50683-4 - ↑ Wilson, Robert A. (2009),
*The Finite Simple Groups*, Graduate Texts in Mathematics, vol. 251, Springer-Verlag, ISBN 978-1-84800-987-5 - ↑ Conway &al,
*op. cit.*, p. 235. - ↑ A. G. Lisi; J. O. Weatherall (2010). "A Geometric Theory of Everything".
*Scientific American*.**303**(6): 54–61. Bibcode:2010SciAm.303f..54L. doi:10.1038/scientificamerican1210-54. PMID 21141358. - ↑ Greg Boustead (2008-11-17). "Garrett Lisi's Exceptional Approach to Everything".
*SEED Magazine*. Archived from the original on 2009-02-02.`{{cite news}}`

: CS1 maint: unfit URL (link) - ↑ Shiga, David (2010-01-07). "'Most beautiful' math structure appears in lab for first time".
*New Scientist*. Retrieved 2023-02-01. - ↑ Did a 1-dimensional magnet detect a 248-dimensional Lie algebra?,
*Notices of the American Mathematical Society*, September 2011. - ↑ "AIM math: Representations of E8".
*aimath.org*.

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In mathematics, a Lie algebra is **semisimple** if it is a direct sum of simple Lie algebras..

In mathematics, an **affine Lie algebra** is an infinite-dimensional Lie algebra that is constructed in a canonical fashion out of a finite-dimensional simple Lie algebra. Given an affine Lie algebra, one can also form the associated affine Kac-Moody algebra, as described below. From a purely mathematical point of view, affine Lie algebras are interesting because their representation theory, like representation theory of finite-dimensional semisimple Lie algebras, is much better understood than that of general Kac–Moody algebras. As observed by Victor Kac, the character formula for representations of affine Lie algebras implies certain combinatorial identities, the Macdonald identities.

In mathematics, a **generalized Kac–Moody algebra** is a Lie algebra that is similar to a Kac–Moody algebra, except that it is allowed to have imaginary simple roots. Generalized Kac–Moody algebras are also sometimes called **GKM algebras**, **Borcherds–Kac–Moody algebras**, **BKM algebras**, or **Borcherds algebras**. The best known example is the monster Lie algebra.

In conformal field theory and representation theory, a **W-algebra** is an associative algebra that generalizes the Virasoro algebra. W-algebras were introduced by Alexander Zamolodchikov, and the name "W-algebra" comes from the fact that Zamolodchikov used the letter W for one of the elements of one of his examples.

In mathematics, the **Littelmann path model** is a combinatorial device due to Peter Littelmann for computing multiplicities *without overcounting* in the representation theory of symmetrisable Kac–Moody algebras. Its most important application is to complex semisimple Lie algebras or equivalently compact semisimple Lie groups, the case described in this article. Multiplicities in irreducible representations, tensor products and branching rules can be calculated using a coloured directed graph, with labels given by the simple roots of the Lie algebra.

In algebra, the **Nichols algebra** of a braided vector space is a braided Hopf algebra which is denoted by and named after the mathematician Warren Nichols. It takes the role of quantum Borel part of a pointed Hopf algebra such as a quantum groups and their well known finite-dimensional truncations. Nichols algebras can immediately be used to write down new such quantum groups by using the Radford biproduct.

In representation theory, a branch of mathematics, the **theorem of the highest weight** classifies the irreducible representations of a complex semisimple Lie algebra . There is a closely related theorem classifying the irreducible representations of a connected compact Lie group . The theorem states that there is a bijection

This is a glossary for the terminology applied in the mathematical theories of Lie groups and Lie algebras. For the topics in the representation theory of Lie groups and Lie algebras, see Glossary of representation theory. Because of the lack of other options, the glossary also includes some generalizations such as quantum group.

In abstract algebra, specifically the theory of Lie algebras, **Serre's theorem** states: given a root system , there exists a finite-dimensional semisimple Lie algebra whose root system is the given .

In mathematics, the **representation theory of semisimple Lie algebras** is one of the crowning achievements of the theory of Lie groups and Lie algebras. The theory was worked out mainly by E. Cartan and H. Weyl and because of that, the theory is also known as the **Cartan–Weyl theory**. The theory gives the structural description and classification of a finite-dimensional representation of a semisimple Lie algebra ; in particular, it gives a way to parametrize irreducible finite-dimensional representations of a semisimple Lie algebra, the result known as the theorem of the highest weight.

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