- E₆
In
mathematics , E6 is the name of someLie group s and also theirLie algebra s . It is one of the five exceptional compactsimple Lie group s as well as one of thesimply laced group s. E6 has rank 6 and dimension 78. The fundamental group of the compact form is thecyclic group Z3 and itsouter automorphism group is thecyclic group Z2. Itsfundamental representation is 27-dimensional (complex). Thedual representation , which is inequivalent, is also 27-dimensional.A certain noncompact real form of E6 is the group of collineations (line-preserving transformations) of the
octonion icprojective plane OP2. It is also the group of determinant-preserving linear transformations of the exceptionalJordan algebra . The exceptional Jordan algebra is 27-dimensional, which explains why the compact real form of E6 has a 27-dimensional complex representation. The compact real form of E6 is theisometry group of a 32-dimensionalRiemannian manifold known as the 'bioctonionic projective plane'. Altogether there are 5 real forms and one complex form.In
particle physics , E6 plays a role in some grand unified theories.Algebra
Dynkin diagram Roots of E6
Although they span a six-dimensional space, it's much more symmetrical to consider them as vectors in a six-dimensional subspace of a nine-dimensional space.
:(1,−1,0;0,0,0;0,0,0), (−1,1,0;0,0,0;0,0,0),
:(−1,0,1;0,0,0;0,0,0), (1,0,−1;0,0,0;0,0,0),
:(0,1,−1;0,0,0;0,0,0), (0,−1,1;0,0,0;0,0,0),
:(0,0,0;1,−1,0;0,0,0), (0,0,0;−1,1,0;0,0,0),
:(0,0,0;−1,0,1;0,0,0), (0,0,0;1,0,−1;0,0,0),
:(0,0,0;0,1,−1;0,0,0), (0,0,0;0,−1,1;0,0,0),
:(0,0,0;0,0,0;1,−1,0), (0,0,0;0,0,0;−1,1,0),
:(0,0,0;0,0,0;−1,0,1), (0,0,0;0,0,0;1,0,−1),
:(0,0,0;0,0,0;0,1,−1), (0,0,0;0,0,0;0,−1,1),
All 27 combinations of where is one of
All 27 combinations of where is one of
Simple roots
:(0,0,0;0,0,0;0,1,−1)
:(0,0,0;0,0,0;1,−1,0)
:(0,0,0;0,1,−1;0,0,0)
:(0,0,0;1,−1,0;0,0,0)
:(0,1,−1;0,0,0;0,0,0)
:
An alternative description
An alternative (6-dimensional) description of the root system, which is useful in considering as a subgroup of , is the following:
All permutations of: preserving the zero at the last entry,
and all of the following roots with an even number of plus signs
:.
Thus the 78 generators comprise of the following subalgebras:: A 45-dimensional subalgebra, including the above generators plus the five Cartan generators corresponding to the first five entries.: Two 16-dimensional subalgebras that transform as a
Weyl spinor of and its complex conjugate. These have a non-zero last entry.: 1 generator which is their chirality generator, and is the sixth Cartan generator.The
simple root s in this description are(−1/2,−1/2,−1/2,−1/2,−1/2,−√3 / 2})
(1,1,0,0,0,0)
(0,−1,1,0,0,0)
(0,0,−1,1,0,0)
(0,0,0,−1,1,0)
(−1,1,0,0,0,0)
we have ordered them so that their corresponding nodes in the
Dynkin diagram are ordered from left to right (in the diagram depicted above) with the side node last.Cartan matrix :
=Important subalgebras and representations=The Lie algebra E6 has an F4 subalgebra, which is the fixed subalgebra of an outer automorphism, and an SU(3) × SU(3) × SU(3) subalgebra.
Other maximal subalgebras which have an importance in physics (see below) and can be read off the Dynkin diagram, are the algebras of SO(10) × U(1) and SU(6) × SU(2).
In addition to the 78-dimensional adjoint representation, there are two dual 27-dimensional "vector" representations.
E6 polytope
The E6 polytope is the
convex hull of the roots of E6. It therefore exists in 6 dimensions; itssymmetry group contains theCoxeter group for E6 as an index 2 subgroup.Importance in physics
N=8
supergravity in five dimensions, which is adimensional reduction from 11 dimensional supergravity, admits an E6 bosonic global symmetry and an bosonic local symmetry. The fermions are in representations of , the gauge fields are in a representation of E6, and the scalars are in a representation of both (Gravitons aresinglet s with respect to both). Physical states are in representations of the coset .In grand unification theories, E6 appears as a possible gauge group which, after its breaking, gives rise to the
gauge group of thestandard model (also see Importance in physics of E8).One way of achieving this is through breaking to . The adjoint 78 representation breaks, as explained above, into an adjoint , spinor and as well as a singlet of the subalgebra. Including the charge we have:
Where the subscript denotes the charge.
References
*. Online HTML version at [http://math.ucr.edu/home/baez/octonions/node17.html] .
*. Online scanned version at [http://ccdb4fs.kek.jp/cgi-bin/img_index?7904075] .ee also
*
En (Lie algebra)
*ADE classification
*Freudenthal magic square
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