The integral seven-dimensional representation of type G2 #
This file realizes the Chevalley generators of type G₂ on the seven-element weight diagram of
the fundamental module V(ϖ₁), whose weights are the six short roots together with zero. In the
fundamental-weight coordinates of TauCeti.DynkinType.g2Root, and with Bourbaki's numbering in
which the first simple root α₁ is short and the second α₂ is long, the weights are listed as
2α₁ + α₂, α₁ + α₂, α₁, 0, -α₁, -(α₁ + α₂), -(2α₁ + α₂),
the first being the highest weight ϖ₁. On the coordinate vector belonging to a weight, the
Cartan generator H_i acts by the i-th coordinate of that weight; the lowering generator F_i
moves each weight down by α_i along the diagram; and the raising generator E_i moves it up.
The three-term string α₁, 0, -α₁ through the zero weight forces a coefficient 2 on one step of
F₁ and one of E₁; it is placed on the step out of the zero weight in both cases, which is what
makes the divided squares E₁² / 2 and F₁² / 2 integral matrices.
The resulting integer matrices satisfy the Chevalley--Serre relations for the Cartan matrix
CartanMatrix.G₂, whose entry (i, j) is the value of the j-th simple root on the i-th simple
coroot. The universal property of the Serre presentation then gives an explicit integral
seven-dimensional representation of the type-G₂ Serre Lie algebra. The generators of the short
simple root cube to zero and square to twice an integral matrix; those of the long simple root
square to zero.
No identification with the abstract irreducible highest-weight module is asserted, and nothing
here concerns the group scheme the representation will carry: the carrier built from these
matrices is not identified with the pinned simply connected group scheme of type G₂, and
constructions on it transfer to that scheme only along such an identification.
Main definitions #
TauCeti.G2ShortRoot.weight: the seven weights in fundamental-weight coordinates.TauCeti.G2ShortRoot.cartanMatrix,raisingMatrix, andloweringMatrix: the integral Cartan, raising, and lowering matrices, withTauCeti.G2ShortRoot.cartanMatrix_apply,TauCeti.G2ShortRoot.raisingMatrix_applyandTauCeti.G2ShortRoot.loweringMatrix_applygiving their entries from the weights and from the step coefficientsTauCeti.G2ShortRoot.raisingCoefficientandTauCeti.G2ShortRoot.loweringCoefficient.TauCeti.G2ShortRoot.isSerreSystem: the Chevalley--Serre relations between them overℤ, withTauCeti.G2ShortRoot.isSl2Triplethesl₂triple at each node.TauCeti.G2ShortRoot.serreRepresentation: the induced representation of the type-G₂Serre Lie algebra.
Main results #
TauCeti.G2ShortRoot.range_weight: the weights are exactly the short roots and zero, withTauCeti.G2ShortRoot.weight_revandTauCeti.G2ShortRoot.sum_weightrecording the symmetry of the diagram about the origin.TauCeti.G2ShortRoot.span_range_weight_eq_top: the weights span the character lattice.TauCeti.G2ShortRoot.raisingMatrix_pow_threeandloweringMatrix_pow_three: every generator cubes to zero, withraisingMatrix_one_mul_selfandloweringMatrix_one_mul_selfrecording that the long-root generators already square to zero.
References #
The numbering and coordinates follow N. Bourbaki, Lie Groups and Lie Algebras, Chapters 4--6,
Plate IX. The seven-dimensional representation and its weight diagram follow J. E. Humphreys,
Introduction to Lie Algebras and Representation Theory, §19.3 and §21.3, and J. C. Jantzen,
Representations of Algebraic Groups, II.2. The generator API and declaration order use
TauCeti.Algebra.Lie.E7.Minuscule.Basic as a formal template.
The integral generator matrices #
The Cartan generator H_i, acting on each weight vector by the i-th coordinate of its
weight.
Equations
- TauCeti.G2ShortRoot.cartanMatrix i = Matrix.diagonal fun (a : Fin 7) => TauCeti.G2ShortRoot.weight a i
Instances For
The nonzero entries of the raising generators, indexed by their row: the i-th raising
generator carries the (a+1)-st weight vector to raisingCoefficient i a times the a-th.
Instances For
The nonzero entries of the lowering generators, indexed by their row: the i-th lowering
generator carries the (a-1)-st weight vector to loweringCoefficient i a times the a-th.
Equations
Instances For
The entries of the raising generators. They are supported on the superdiagonal: the weights are listed in decreasing order, so a raising generator either moves a weight vector one step up the list or kills it.
The entries of the lowering generators. They are supported on the subdiagonal: the weights are listed in decreasing order, so a lowering generator either moves a weight vector one step down the list or kills it.
Chevalley--Serre relations #
The integral generator matrices satisfy the Chevalley--Serre relations of type G₂, for the
Cartan matrix whose entry (i, j) is the value of the j-th simple root on the i-th simple
coroot.
At each simple node, the integral Cartan, raising and lowering matrices form an sl₂
triple. Only the nonvanishing of the Cartan generator is a computation; the three relations are
the diagonal instances of the Chevalley--Serre relations, the diagonal Cartan number being 2.
The explicit integral seven-dimensional representation of the type-G₂ Serre Lie algebra.
Equations
Instances For
The integral Serre representation sends H_i to the Cartan generator matrix.
The integral Serre representation sends E_i to the raising generator matrix.
The integral Serre representation sends F_i to the lowering generator matrix.
Nilpotency of the generators #
Every raising generator cubes to zero.
Every lowering generator cubes to zero.
The long-root raising generator squares to zero.
The long-root lowering generator squares to zero.
The short-root raising generator squares to twice a single unit matrix.
The short-root lowering generator squares to twice a single unit matrix.