E₆ (mathematics)

In mathematics, E₆ is the name of some closely related Lie groups, linear algebraic groups or their Lie algebras ${\mathfrak {e}}_{6}$ , all of which have dimension 78; the same notation E₆ is used for the corresponding root lattice, which has rank 6. The designation E₆ comes from the Cartan–Killing classification of the complex simple Lie algebras (see Élie Cartan § Work). This classifies Lie algebras into four infinite series labeled A_n, B_n, C_n, D_n, and five exceptional cases labeled E₆, E₇, E₈, F₄, and G₂. The E₆ algebra is thus one of the five exceptional cases.

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.

Real and complex forms

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 compact form (which is usually the one meant if no other information is given), which has fundamental group Z/3Z and outer automorphism group Z/2Z.
The split form, EI (or E₆₍₆₎), which has maximal compact subgroup Sp(4)/(±1), fundamental group of order 2 and outer automorphism group of order 2.
The quasi-split form EII (or E₆₍₂₎), which has maximal compact subgroup SU(2) × SU(6)/(center), fundamental group cyclic of order 6 and outer automorphism group of order 2.
EIII (or E_6(-14)), which has maximal compact subgroup SO(2) × Spin(10)/(center), fundamental group Z and trivial outer automorphism group.
EIV (or E_6(-26)), which has maximal compact subgroup F₄, trivial fundamental group cyclic and outer automorphism group of order 2.

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.

E₆ as an algebraic group

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, E_6,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=E_6(-26) are said to be inner or of type ¹E₆ meaning that their class lies in H¹(k, E_6,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.

Automorphisms of an Albert Algebra

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]

Algebra

Dynkin diagram

The Dynkin diagram for E₆ is given by , which may also be drawn as .

Roots of E₆

The 72 vertices of the 1₂₂ polytope represent the root vectors of the E₆, as shown in this Coxeter plane projection. Orange vertices are doubled in this projection.
Coxeter–Dynkin diagram:

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 $(\mathbf {3$ where $\mathbf {3}$ is one of $\left({\frac {2}{3}},-{\frac {1}{3}},-{\frac {1}{3}}\right),\ \left(-{\frac {1}{3}},{\frac {2}{3}},-{\frac {1}{3}}\right),\ \left(-{\frac {1}{3}},-{\frac {1}{3}},{\frac {2}{3}}\right),$ plus all 27 combinations of $({\bar {\mathbf {3} }};{\bar {\mathbf {3} }};{\bar {\mathbf {3} }})$ where ${\bar {\mathbf {3} }}$ is one of $\left(-{\frac {2}{3}},{\frac {1}{3}},{\frac {1}{3}}\right),\ \left({\frac {1}{3}},-{\frac {2}{3}},{\frac {1}{3}}\right),\ \left({\frac {1}{3}},{\frac {1}{3}},-{\frac {2}{3}}\right).$

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({\frac {1}{3}},-{\frac {2}{3}},{\frac {1}{3}};-{\frac {2}{3}},{\frac {1}{3}},{\frac {1}{3}};-{\frac {2}{3}},{\frac {1}{3}},{\frac {1}{3}}\right)

Graph of E₆ as a subgroup of E₈ projected into the Coxeter plane

Hasse diagram of E₆ root poset with edge labels identifying added simple root position

E₆ roots derived from the roots of E₈

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 = {α ∈ Z⁷ ∪ (Z+12)⁷ : Σα_i² + α₁² = 2, Σα_i + α₁ ∈ 2Z},

E₆ = {α ∈ Z⁶ ∪ (Z+12)⁶ : Σα_i² + 2α₁² = 2, Σα_i + 2α₁ ∈ 2Z}

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 description

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 $4\times {\begin{pmatrix}5\\2\end{pmatrix}}$ permutations of

(\pm 1,\pm 1,0,0,0,0)

preserving the zero at the last entry,

and all of the following roots with an odd number of plus signs

\left(\pm {1 \over 2},\pm {1 \over 2},\pm {1 \over 2},\pm {1 \over 2},\pm {1 \over 2},\pm {{\sqrt {3}} \over 2}\right).

Thus the 78 generators consist of the following subalgebras:

A 45-dimensional SO(10) subalgebra, including the above

4\times {\begin{pmatrix}5\\2\end{pmatrix}}

generators plus the five Cartan generators corresponding to the first five entries.

Two 16-dimensional subalgebras that transform as a Weyl spinor of

\operatorname {spin} (10)

and its complex conjugate. These have a non-zero last entry.

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\\-{\frac {1}{2}}&-{\frac {1}{2}}&-{\frac {1}{2}}&-{\frac {1}{2}}&-{\frac {1}{2}}&{\frac {\sqrt {3}}{2}}\\0&0&0&1&-1&0\\\end{smallmatrix}}\right]

Weyl group

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]

Cartan matrix

\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]

Important subalgebras and representations

Embeddings of the maximal subgroups of E₆ up to dimension 78 with associated projection matrix.

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 (sequence A121737 in the OEIS):

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.

E6 polytope

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.

Chevalley and Steinberg groups of type E₆ and ²E₆

The groups of type E₆ over arbitrary fields (in particular finite fields) were introduced by Dickson (1901, 1908).

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:

the finite group consisting of the points over F_q of the simply connected form of E₆ (for clarity, this can be written E_6,sc(q) or more rarely ${\tilde {E}}_{6}(q)$ and is known as the "universal" Chevalley group of type E₆ over F_q),
(rarely) the finite group consisting of the points over F_q of the adjoint form of E₆ (for clarity, this can be written E_6,ad(q), and is known as the "adjoint" Chevalley group of type E₆ over F_q), or
the finite group which is the image of the natural map from the former to the latter: this is what will be denoted by E₆(q) in the following, as is most common in texts dealing with finite groups.

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, E_6,sc(q) is its Schur cover, and E_6,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 E_6,ad(q), which explains why E_6,sc(q) and E_6,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 F_q unlike E_6,sc(q) and E_6,ad(q).

Beyond this "split" (or "untwisted") form of E₆, there is also one other form of E₆ over the finite field F_q, 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 F_q². Twisting does not change the fact that the algebraic fundamental group of ²E_6,ad is Z/3Z, but it does change those q for which the covering of ²E_6,ad by ²E_6,sc is non-trivial on the F_q-points. Precisely: ²E_6,sc(q) is a covering of ²E₆(q), and ²E_6,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 ²E_6,sc(q) over ²E₆(q) is 3 and ²E₆(q) is of index 3 in ²E_6,ad(q), which explains why ²E_6,sc(q) and ²E_6,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 F_q-points of an algebraic group. Another is that whereas ²E_6,sc(q) and ²E_6,ad(q) are the F_q-points of an algebraic group, the group in question also depends on q (e.g., the points over F_q² of the same group are the untwisted E_6,sc(q²) and E_6,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 (sequence A008872 in the OEIS):

|E_{6}(q)|={\frac {1}{\mathrm {gcd} (3,q-1)}}q^{36}(q^{12}-1)(q^{9}-1)(q^{8}-1)(q^{6}-1)(q^{5}-1)(q^{2}-1)

|{}^{2}\!E_{6}(q)|={\frac {1}{\mathrm {gcd} (3,q+1)}}q^{36}(q^{12}-1)(q^{9}+1)(q^{8}-1)(q^{6}-1)(q^{5}+1)(q^{2}-1)

(sequence A008916 in the OEIS). The order of E_6,sc(q) or E_6,ad(q) (both are equal) can be obtained by removing the dividing factor gcd(3,q−1) from the first formula (sequence A008871 in the OEIS), and the order of ²E_6,sc(q) or ²E_6,ad(q) (both are equal) can be obtained by removing the dividing factor gcd(3,q+1) from the second (sequence A008915 in the OEIS).

The Schur multiplier of E₆(q) is always gcd(3,q−1) (i.e., E_6,sc(q) is its Schur cover). The Schur multiplier of ²E₆(q) is gcd(3,q+1) (i.e., ²E_6,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 E_6,ad(q)), the group Z/2Z of diagram automorphisms, and the group of field automorphisms (i.e., cyclic of order f if q=p^f 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 ²E_6,ad(q)) and the group of field automorphisms (i.e., cyclic of order f if q=p^f where p is prime).

Importance in physics

The pattern of weak isospin,

W

, weaker isospin,

W'

, strong

g 3

and

g 8

, and baryon minus lepton,

B

, charges for particles in the SO(10) Grand Unified Theory, rotated to show the embedding in

E 6

.

$N = 8$ supergravity in five dimensions, which is a dimensional reduction from $11$ dimensional supergravity, admits an $E 6$ bosonic global symmetry and an $Sp(8)$ bosonic local symmetry. The fermions are in representations of $Sp(8)$ , the gauge fields are in a representation of $E 6$ , and the scalars are in a representation of both (Gravitons are singlets with respect to both). Physical states are in representations of the coset $E 6 /Sp(8)$ .

In grand unification theories, $E 6$ appears as a possible gauge group which, after its breaking, gives rise to $the SU(3) \times SU(2) \times U(1)$ gauge group of the standard model. One way of achieving this is through breaking to $SO(10) \times U(1)$ . The adjoint $78$ representation breaks, as explained above, into an adjoint $45$ , spinor $16$ and $16$ as well as a singlet of the $SO(10)$ subalgebra. Including the $U(1)$ charge we have

78\rightarrow 45_{0}\oplus 16_{-3}\oplus {\overline {16}}_{3}+1_{0}.

Where the subscript denotes the $U(1)$ charge.

Likewise, the fundamental representation $27$ and its conjugate $27$ break into a scalar $1$ , a vector $10$ and a spinor, either $16$ or $16$ :

27\rightarrow 1_{4}\oplus 10_{-2}\oplus 16_{1},

{\bar {27}}\rightarrow 1_{-4}\oplus 10_{2}\oplus {\overline {16}}_{-1}.

Thus, one can get the Standard Model's elementary fermions and Higgs boson.

References

Adams, J. Frank (1996), Lectures on exceptional Lie groups, Chicago Lectures in Mathematics, University of Chicago Press, ISBN 978-0-226-00526-3, MR 1428422.
Baez, John (2002). "The Octonions, Section 4.4: E₆". Bull. Amer. Math. Soc. 39 (2): 145–205. arXiv:math/0105155. doi:10.1090/S0273-0979-01-00934-X. ISSN 0273-0979. S2CID 586512. Online HTML version at .
Cremmer, E.; J. Scherk; J. H. Schwarz (1979). "Spontaneously Broken N=8 Supergravity". Phys. Lett. B. 84 (1): 83–86. Bibcode:1979PhLB...84...83C. doi:10.1016/0370-2693(79)90654-3. Online scanned version at .
Dickson, Leonard Eugene (1901), "A class of groups in an arbitrary realm connected with the configuration of the 27 lines on a cubic surface", The Quarterly Journal of Pure and Applied Mathematics, 33: 145–173, reprinted in volume V of his collected works
Dickson, Leonard Eugene (1908), "A class of groups in an arbitrary realm connected with the configuration of the 27 lines on a cubic surface (second paper)", The Quarterly Journal of Pure and Applied Mathematics, 39: 205–209, ISBN 9780828403061, reprinted in volume VI of his collected works
Ichiro, Yokota (2009). "Exceptional Lie groups". arXiv:0902.0431 [math.DG].

Rosenfeld, Boris (1997), Geometry of Lie Groups (theorem 7.4 on page 335, and following paragraph).
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
Springer, Tonny A.; Veldkamp, Ferdinand D. (2000). Octonions, Jordan Algebras, and Exceptional Groups. Springer. doi:10.1007/978-3-662-12622-6. ISBN 978-3-642-08563-5. MR 1763974., §7.3
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. 26. 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.

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[1] Rosenfeld, Boris (1997), Geometry of Lie Groups (theorem 7.4 on page 335, and following paragraph).

[2] 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

[3] Springer, Tonny A.; Veldkamp, Ferdinand D. (2000). Octonions, Jordan Algebras, and Exceptional Groups. Springer. doi:10.1007/978-3-662-12622-6. ISBN 978-3-642-08563-5. MR 1763974., §7.3

[4] 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. 26. ISBN 0-19-853199-0.

[5] Carter, Roger W. (1989). Simple Groups of Lie Type. Wiley Classics Library. John Wiley & Sons. ISBN 0-471-50683-4.

[6] Wilson, Robert A. (2009). The Finite Simple Groups. Graduate Texts in Mathematics. Vol. 251. Springer-Verlag. ISBN 978-1-84800-987-5.

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