The integral short-root representation of type F4 #
This file realizes the Chevalley generators of type F₄ on the twenty-six-element weight
diagram TauCeti.DynkinType.f4ShortRootWeight, whose weights are the twenty-four short roots
and the zero weight taken twice. On the coordinate vector belonging to the bth weight, the
Cartan generator H_i acts by the simple-coroot coordinate of that weight, and each raising
generator E_i and lowering generator F_i carries the coordinate vector to an integer
multiple of a single coordinate vector, read from explicit target and coefficient tables. Every
generator is therefore a step matrix, a matrix each of whose columns has at most one nonzero
entry, and products of step matrices are again step matrices.
The resulting integer matrices satisfy the Chevalley--Serre relations for the transpose of the
Bourbaki Cartan matrix of type F₄, which is the convention under which ⁅H_i, E_j⁆ is the
pairing of the jth simple root with the ith simple coroot times E_j. The universal
property of the Serre presentation gives the explicit integral twenty-six-dimensional
representation. The two long simple raising and lowering generators square to zero. The two
short ones do not: their squares are twice an integral matrix, the divided square, and their
cubes vanish. Those divided squares are what an admissible lattice built on this weight basis
must be stable under.
The two zero-weight coordinate vectors are the images of the two short simple lowering generators applied to the coordinate vectors of the corresponding simple roots, and the tables record how each short simple raising generator returns them: the one from its own root with coefficient two, the other with coefficient one.
No identification with the abstract irreducible highest-weight module is asserted here, and the zero-weight basis is the explicitly tabulated one rather than one characterized by a generation property. The construction is explicit: every matrix entry is read from the weight, target and coefficient tables.
Main definitions #
TauCeti.F4ShortRoot.cartanMatrix,raisingMatrix, andloweringMatrix: the integral Cartan, raising, and lowering matrices.TauCeti.F4ShortRoot.raisingDividedSquareMatrixandloweringDividedSquareMatrix: the divided squares of the raising and lowering matrices.TauCeti.F4ShortRoot.isSerreSystem: the Chevalley--Serre relations between them overℤ, withTauCeti.F4ShortRoot.isSl2Triplethesl₂triple at each node.TauCeti.F4ShortRoot.serreRepresentation: the induced representation of the type-F₄Serre Lie algebra.
Main results #
TauCeti.F4ShortRoot.raisingMatrix_mul_selfandloweringMatrix_mul_self: each square is twice the divided square.TauCeti.F4ShortRoot.raisingMatrix_mul_raisingDividedSquareMatrixand its three siblings: each generator annihilates its own divided square on either side, so each generator cubes to zero.TauCeti.F4ShortRoot.raisingMatrix_mul_self_of_lt_twoandloweringMatrix_mul_self_of_lt_two: the two long simple generators square to zero.
References #
The numbering follows Bourbaki, Lie Groups and Lie Algebras, Chapters 4--6, Plate VIII. The
admissible lattice generated from a highest weight vector by divided-power lowering operators is
the one of B. Kostant, Groups over ℤ, and R. Steinberg, Lectures on Chevalley Groups,
§12. The construction of the twenty-six-dimensional module from its weight diagram and the
Serre presentation follows J. E. Humphreys, Introduction to Lie Algebras and Representation
Theory, §§18 and 27.
Step matrices #
The tables #
The target index of each coordinate vector under the ith raising generator; a column with
coefficient zero has itself as its target.
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The coefficient of each coordinate vector under the ith raising generator.
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The target index of each coordinate vector under the ith lowering generator; a column
with coefficient zero has itself as its target.
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The coefficient of each coordinate vector under the ith lowering generator.
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The target index of each coordinate vector under the divided square of the ith raising
generator. Only the two short simple roots contribute, each moving the coordinate vector of the
negative of its root to that of the root itself.
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The coefficient of each coordinate vector under the divided square of the ith raising
generator.
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The target index of each coordinate vector under the divided square of the ith lowering
generator.
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The coefficient of each coordinate vector under the divided square of the ith lowering
generator.
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The integral generator matrices #
The Cartan generator H_i in the short-root weight basis.
Equations
- TauCeti.F4ShortRoot.cartanMatrix i = Matrix.diagonal fun (a : Fin 26) => TauCeti.DynkinType.f4ShortRootWeight a i
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The raising generator E_i in the short-root weight basis.
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The lowering generator F_i in the short-root weight basis.
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The divided square E_i^(2) = E_i² / 2 of the raising generator, an integral matrix.
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The divided square F_i^(2) = F_i² / 2 of the lowering generator, an integral matrix.
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The entrywise formula for the diagonal Cartan generator matrix.
The entrywise formula for the raising generator matrix.
The entrywise formula for the lowering generator matrix.
The entrywise formula for the divided square of the raising generator.
The entrywise formula for the divided square of the lowering generator.
Chevalley--Serre relations #
The integral short-root generator matrices satisfy the Chevalley--Serre relations of type
F₄, for the transpose of the Bourbaki Cartan matrix, in Bourbaki numbering.
At each simple node, the integral Cartan, raising and lowering matrices form an sl₂
triple: the raising and lowering matrices bracket to the nonzero Cartan matrix, which brackets
with them to 2 and -2 times themselves. So each node spans a copy of sl₂ inside the matrix
Lie algebra of the integral short-root module.
The explicit integral twenty-six-dimensional representation of the type-F₄ Serre Lie
algebra.
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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.
Squares and cubes of the generators #
The square of a raising generator is twice its divided square.
The square of a lowering generator is twice its divided square.
A raising generator annihilates its divided square on the left.
A raising generator annihilates its divided square on the right.
A lowering generator annihilates its divided square on the left.
A lowering generator annihilates its divided square on the right.
Every raising generator cubes to zero.
Every lowering generator cubes to zero.
The divided square of a long simple raising generator vanishes.
The divided square of a long simple lowering generator vanishes.
The long simple raising generators square to zero.
The long simple lowering generators square to zero.