In mathematics, E6 is the name of some closely related Lie groups, linear algebraic groups or their Lie algebras
ak{e}6
The fundamental group of the complex form, compact real form, or any algebraic version of E6 is the cyclic group Z/3Z, and its outer automorphism group is the cyclic group Z/2Z. Its fundamental representation is 27-dimensional (complex), and a basis is given by the 27 lines on a cubic surface. The dual representation, which is inequivalent, is also 27-dimensional.
In particle physics, E6 plays a role in some grand unified theories.
There is a unique complex Lie algebra of type E6, corresponding to a complex group of complex dimension 78. The complex adjoint Lie group E6 of complex dimension 78 can be considered as a simple real Lie group of real dimension 156. This has fundamental group Z/3Z, has maximal compact subgroup the compact form (see below) of E6, and has an outer automorphism group non-cyclic of order 4 generated by complex conjugation and by the outer automorphism which already exists as a complex automorphism.
As well as the complex Lie group of type E6, there are five real forms of the Lie algebra, and correspondingly five real forms of the group with trivial center (all of which have an algebraic double cover, and three of which have further non-algebraic covers, giving further real forms), all of real dimension 78, as follows:
The EIV form of E6 is the group of collineations (line-preserving transformations) of the octonionic projective plane OP2.[1] It is also the group of determinant-preserving linear transformations of the exceptional Jordan 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 the isometry group of a 32-dimensional Riemannian manifold known as the 'bioctonionic projective plane'; similar constructions for E7 and E8 are known as the Rosenfeld projective planes, and are part of the Freudenthal magic square.
By means of a Chevalley basis for the Lie algebra, one can define E6 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") adjoint form of E6. Over an algebraically closed field, this and its triple cover are the only forms; however, over other fields, there are often many other forms, or "twists" of E6, which are classified in the general framework of Galois cohomology (over a perfect field k) by the set H1(k, Aut(E6)) which, because the Dynkin diagram of E6 (see below) has automorphism group Z/2Z, maps to H1(k, Z/2Z) = Hom (Gal(k), Z/2Z) with kernel H1(k, E6,ad).[2]
Over the field of real numbers, the real component of the identity of these algebraically twisted forms of E6 coincide with the three real Lie groups mentioned above, but with a subtlety concerning the fundamental group: all adjoint forms of E6 have fundamental group Z/3Z in the sense of algebraic geometry, with Galois action as on the third roots of unity; this means that they admit exactly one triple cover (which may be trivial on the real points); the further non-compact real Lie group forms of E6 are therefore not algebraic and admit no faithful finite-dimensional representations. The compact real form of E6 as well as the noncompact forms EI=E6(6) and EIV=E6(-26) are said to be inner or of type 1E6 meaning that their class lies in H1(k, E6,ad) or that complex conjugation induces the trivial automorphism on the Dynkin diagram, whereas the other two real forms are said to be outer or of type 2E6.
Over finite fields, the Lang–Steinberg theorem implies that H1(k, E6) = 0, meaning that E6 has exactly one twisted form, known as 2E6: see below.
Similar to how the algebraic group G2 is the automorphism group of the octonions and the algebraic group F4 is the automorphism group of an Albert algebra, an exceptional Jordan algebra, the algebraic group E6 is the group of linear automorphisms of an Albert algebra that preserve a certain cubic form, called the "determinant".[3]
The Dynkin diagram for E6 is given by, which may also be drawn as .
Although they span a six-dimensional space, it is much more symmetrical to consider them as vectors in a six-dimensional subspace of a nine-dimensional space. Then one can take the roots to be
(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),plus all 27 combinations of
(3;3;3)
3
| \left( | 2 |
| 3 |
,-
| 1 | |
| 3 |
,-
| 1 | |
| 3 |
\right), \left(-
| 1 | |
| 3 |
,
| 2 | |
| 3 |
,-
| 1 | |
| 3 |
\right), \left(-
| 1 | |
| 3 |
,-
| 1 | |
| 3 |
,
| 2 | |
| 3 |
\right),
(\bar{3
\bar{3
| \left(- | 2 | , |
| 3 |
| 1 | , | |
| 3 |
| 1 | \right), \left( | |
| 3 |
| 1 | |
| 3 |
,-
| 2 | |
| 3 |
,
| 1 | |
| 3 |
\right), \left(
| 1 | |
| 3 |
,
| 1 | |
| 3 |
,-
| 2 | |
| 3 |
\right).
Simple roots
One possible selection for the simple roots of E6 is:
(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)
| \left( | 1 | ,- |
| 3 |
| 2 | , | |
| 3 |
| 1 | ;- | |
| 3 |
| 2 | , | |
| 3 |
| 1 | , | |
| 3 |
| 1 | ;- | |
| 3 |
| 2 | , | |
| 3 |
| 1 | , | |
| 3 |
| 1 | |
| 3 |
\right)
E6 is the subset of E8 where a consistent set of three coordinates are equal (e.g. first or last). This facilitates explicit definitions of E7 and E6 as:
E7 =,
E6 =
The following 72 E6 roots are derived in this manner from the split real even E8 roots. Notice the last 3 dimensions being the same as required:
An alternative (6-dimensional) description of the root system, which is useful in considering E6 × SU(3) as a subgroup of E8, is the following:
All
4 x \begin{pmatrix}5\\2\end{pmatrix}
(\pm1,\pm1,0,0,0,0)
and all of the following roots with an odd number of plus signs
\left(\pm{1\over2},\pm{1\over2},\pm{1\over2},\pm{1\over2},\pm{1\over2},\pm{\sqrt{3}\over2}\right).
Thus the 78 generators consist of the following subalgebras:
A 45-dimensional SO(10) subalgebra, including the above
4 x \begin{pmatrix}5\\2\end{pmatrix}
Two 16-dimensional subalgebras that transform as a Weyl spinor of
\operatorname{spin}(10)
1 generator which is their chirality generator, and is the sixth Cartan generator.
One choice of simple roots for E6 is given by the rows of the following matrix, indexed in the order :
\left[\begin{smallmatrix} 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 | &- | |
| 2 |
| 1 | &- | |
| 2 |
| 1 | &- | |
| 2 |
| 1 | &- | |
| 2 |
| 1 | & | |
| 2 |
| \sqrt{3 | |
The Weyl group of E6 is of order 51840: it is the automorphism group of the unique simple group of order 25920 (which can be described as any of: PSU4(2), PSΩ6−(2), PSp4(3) or PSΩ5(3)).[4]
\left[\begin{smallmatrix} 2&-1&0&0&0&0\\ -1&2&-1&0&0&0\\ 0&-1&2&-1&0&-1\\ 0&0&-1&2&-1&0\\ 0&0&0&-1&2&0\\ 0&0&-1&0&0&2 \end{smallmatrix}\right]
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.
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 :
1, 27 (twice), 78, 351 (four times), 650, 1728 (twice), 2430, 2925, 3003 (twice), 5824 (twice), 7371 (twice), 7722 (twice), 17550 (twice), 19305 (four times), 34398 (twice), 34749, 43758, 46332 (twice), 51975 (twice), 54054 (twice), 61425 (twice), 70070, 78975 (twice), 85293, 100386 (twice), 105600, 112320 (twice), 146432 (twice), 252252 (twice), 314496 (twice), 359424 (four times), 371800 (twice), 386100 (twice), 393822 (twice), 412776 (twice), 442442 (twice)...
The underlined terms in the sequence above are the dimensions of those irreducible representations possessed by the adjoint form of E6 (equivalently, those whose weights belong to the root lattice of E6), whereas the full sequence gives the dimensions of the irreducible representations of the simply connected form of E6.
The symmetry of the Dynkin diagram of E6 explains why many dimensions occur twice, the corresponding representations being related by the non-trivial outer automorphism; however, there are sometimes even more representations than this, such as four of dimension 351, two of which are fundamental and two of which are not.
The fundamental representations have dimensions 27, 351, 2925, 351, 27 and 78 (corresponding to the six nodes in the Dynkin diagram in the order chosen for the Cartan matrix above, i.e., the nodes are read in the five-node chain first, with the last node being connected to the middle one).
The embeddings of the maximal subgroups of E6 up to dimension 78 are shown to the right.
The E6 polytope is the convex hull of the roots of E6. It therefore exists in 6 dimensions; its symmetry group contains the Coxeter group for E6 as an index 2 subgroup.
See main article: <sup>2</sup>E<sub>6</sub>.
The groups of type E6 over arbitrary fields (in particular finite fields) were introduced by .
The points over a finite field with q elements of the (split) algebraic group E6 (see above), whether of the adjoint (centerless) or simply connected form (its algebraic universal cover), give a finite Chevalley group. This is closely connected to the group written E6(q), however there is ambiguity in this notation, which can stand for several things:
\tildeE6(q)
From the finite group perspective, the relation between these three groups, which is quite analogous to that between SL(n,q), PGL(n,q) and PSL(n,q), can be summarized as follows: E6(q) is simple for any q, E6,sc(q) is its Schur cover, and E6,ad(q) lies in its automorphism group; furthermore, when q−1 is not divisible by 3, all three coincide, and otherwise (when q is congruent to 1 mod 3), the Schur multiplier of E6(q) is 3 and E6(q) is of index 3 in E6,ad(q), which explains why E6,sc(q) and E6,ad(q) are often written as 3·E6(q) and E6(q)·3. From the algebraic group perspective, it is less common for E6(q) to refer to the finite simple group, because the latter is not in a natural way the set of points of an algebraic group over Fq unlike E6,sc(q) and E6,ad(q).
Beyond this "split" (or "untwisted") form of E6, there is also one other form of E6 over the finite field Fq, known as 2E6, which is obtained by twisting by the non-trivial automorphism of the Dynkin diagram of E6. Concretely, 2E6(q), which is known as a Steinberg group, can be seen as the subgroup of E6(q2) fixed by the composition of the non-trivial diagram automorphism and the non-trivial field automorphism of Fq2. Twisting does not change the fact that the algebraic fundamental group of 2E6,ad is Z/3Z, but it does change those q for which the covering of 2E6,ad by 2E6,sc is non-trivial on the Fq-points. Precisely: 2E6,sc(q) is a covering of 2E6(q), and 2E6,ad(q) lies in its automorphism group; when q+1 is not divisible by 3, all three coincide, and otherwise (when q is congruent to 2 mod 3), the degree of 2E6,sc(q) over 2E6(q) is 3 and 2E6(q) is of index 3 in 2E6,ad(q), which explains why 2E6,sc(q) and 2E6,ad(q) are often written as 3·2E6(q) and 2E6(q)·3.
Two notational issues should be raised concerning the groups 2E6(q). One is that this is sometimes written 2E6(q2), a notation which has the advantage of transposing more easily to the Suzuki and Ree groups, but the disadvantage of deviating from the notation for the Fq-points of an algebraic group. Another is that whereas 2E6,sc(q) and 2E6,ad(q) are the Fq-points of an algebraic group, the group in question also depends on q (e.g., the points over Fq2 of the same group are the untwisted E6,sc(q2) and E6,ad(q2)).
The groups E6(q) and 2E6(q) are simple for any q,[5] [6] and constitute two of the infinite families in the classification of finite simple groups. Their order is given by the following formula :
|E6(q)|=
| 1 | |
| gcd(3,q-1) |
q36(q12-1)(q9-1)(q8-1)(q6-1)(q5-1)(q2-1)
| 2E | |
| |{} | |
| 6 |
(q)|=
| 1 | |
| gcd(3,q+1) |
q36(q12-1)(q9+1)(q8-1)(q6-1)(q5+1)(q2-1)
. The order of E6,sc(q) or E6,ad(q) (both are equal) can be obtained by removing the dividing factor gcd(3,q−1) from the first formula, and the order of 2E6,sc(q) or 2E6,ad(q) (both are equal) can be obtained by removing the dividing factor gcd(3,q+1) from the second .
The Schur multiplier of E6(q) is always gcd(3,q−1) (i.e., E6,sc(q) is its Schur cover). The Schur multiplier of 2E6(q) is gcd(3,q+1) (i.e., 2E6,sc(q) is its Schur cover) outside of the exceptional case q=2 where it is 22·3 (i.e., there is an additional 22-fold cover). The outer automorphism group of E6(q) is the product of the diagonal automorphism group Z/gcd(3,q−1)Z (given by the action of E6,ad(q)), the group Z/2Z of diagram automorphisms, and the group of field automorphisms (i.e., cyclic of order f if q=pf where p is prime). The outer automorphism group of 2E6(q) is the product of the diagonal automorphism group Z/gcd(3,q+1)Z (given by the action of 2E6,ad(q)) and the group of field automorphisms (i.e., cyclic of order f if q=pf where p is prime).
supergravity in five dimensions, which is a dimensional reduction from eleven-dimensional supergravity, admits an bosonic global symmetry and an bosonic local symmetry. The fermions are in representations of, the gauge fields are in a representation of, and the scalars are in a representation of both (Gravitons are singlets with respect to both). Physical states are in representations of the coset .
In grand unification theories, appears as a possible gauge group which, after its breaking, gives rise to gauge group of the standard model. One way of achieving this is through breaking to . The adjoint representation breaks, as explained above, into an adjoint, spinor and as well as a singlet of the subalgebra. Including the charge we have
78 → 450 ⊕ 16-3 ⊕ \overline{16}3+10.
Where the subscript denotes the charge.
Likewise, the fundamental representation and its conjugate break into a scalar, a vector and a spinor, either or :
27 → 14 ⊕ 10-2 ⊕ 161,
\bar{27} → 1-4 ⊕ 102 ⊕ \overline{16}-1.
Thus, one can get the Standard Model's elementary fermions and Higgs boson.
Maximal Subgroups and Ordinary Characters for Simple Groups
. 1985 . Oxford University Press . 0-19-853199-0 . 26 .