The matrix of a cube-zero root subgroup #
The matrix of a Kostant root subgroup at parameter t is the divided-power exponential
∑ₖ tᵏ e⁽ᵏ⁾ of the root operator, read in the chosen lattice basis. When the operator squares to
zero this is 1 + t X for the integral matrix X of the operator, which is
TauCeti.UniversalEnvelopingAlgebra.kostantRootSubgroupMatrix_eq_one_add_smul. This file treats the
next case, an operator that cubes to zero, where one more term survives:
xᵢ(t) = 1 + t X + t² Y,
Y being the integral matrix of the divided square e⁽²⁾ = e² / 2 on the lattice. This is the
shape of a simple root subgroup acting through a three-term weight string, such as a short root
subgroup of type G₂ on the seven-dimensional module. The equation is proved on every
algebra-valued point and then read on the coordinate morphism, where it lets a consumer check a
matrix equation on all points of the root subgroup at once.
Main results #
Both live in the namespace TauCeti.UniversalEnvelopingAlgebra.
kostantRootSubgroupMatrix_eq_one_add_smul_add_smul: the matrix of a cube-zero root subgroup at a point is1 + t X + t² Y.map_genericMatrix_kostantRootSubgroupCoordinateMap_eq_one_add_smul_add_smul: the same equation on the generic matrix, along the root-subgroup coordinate morphism.
The matrix of a cube-zero root subgroup is 1 + t X + t² X₂. When the root operator
cubes to zero its divided-power exponential stops after the quadratic term.
The generic matrix of a cube-zero root subgroup is 1 + t X + t² Y. This is
TauCeti.UniversalEnvelopingAlgebra.kostantRootSubgroupMatrix_eq_one_add_smul_add_smul read on
the coordinate morphism rather than on a point: the entries of the generic matrix of GL N are
carried to those of 1 + t X + t² Y for the parameter t of the universal point of 𝔾ₐ.