Weights and highest vectors for U_q(sl₂) #
The weight spaces of a native UqSl2 q-module are the eigenspaces of the action of K, and
its generalized weight spaces are the maximal generalized eigenspaces of K. The generators
E and F shift both kinds of weight by q² and q⁻², respectively. A finite-dimensional
module is the direct sum of its generalized weight spaces, whether or not K is
diagonalizable. At a generic parameter, raising or lowering any vector of a finite-dimensional
module therefore eventually kills it: otherwise the finite spectrum of K would contain an
infinite geometric progression. Consequently every nonzero finite-dimensional module has a
highest-weight vector. More precisely, every nonzero generalized weight vector is moved by some
element of UqSl2 q to a nonzero highest-weight vector, and by another to a nonzero
lowest-weight vector. This is the starting point for classifying finite-dimensional simple
modules, and the generalized weight decomposition is the setting of the finite-dimensional
complete-reducibility argument. Taking generalized weight spaces of finite-dimensional modules is
exact: a surjective module map carries generalized weight spaces onto those of its target.
The action conventions are those of A. Virelizier, Quantum groups, Sections 2.3--2.4.
The μ-weight space of a module is the native eigenspace of the action of K.
Instances For
The weight space agrees with the native eigenspace of the action of K.
Membership in a weight space means that K acts by its weight.
The zero-weight space vanishes because K is invertible.
Every nonzero weight vector has nonzero weight.
On a vector of weight μ, the generator K⁻¹ acts by μ⁻¹.
Raising a weight vector multiplies its weight by q².
Lowering a weight vector multiplies its weight by q⁻².
The weight after n raising operations.
The weight after n lowering operations.
On a vector of weight μ, the integer power K ^ b acts by μ ^ b.
A module map carries each weight space into the weight space of the same weight.
A finite-dimensional module has only finitely many weights.
Generalized weight spaces #
The generalized μ-weight space of a module is the native maximal generalized eigenspace of
the action of K: the vectors killed by some power of K - μ.
Instances For
The generalized weight space agrees with the native maximal generalized eigenspace of the
action of K.
Membership in a generalized weight space means that some power of K - μ kills the
vector.
Every weight space lies in the generalized weight space of the same weight.
The generalized zero-weight space vanishes because K is invertible.
An element a that q-commutes with K in the form K a = c (a K) maps the generalized
μ-weight space into the generalized c μ-weight space.
Raising a generalized weight vector multiplies its generalized weight by q².
Lowering a generalized weight vector multiplies its generalized weight by q⁻².
The generalized weight after n raising operations.
The generalized weight after n lowering operations.
Generalized weight spaces for distinct weights are independent.
K preserves every generalized weight space.
K⁻¹ preserves every generalized weight space.
A vector of weight α in the generalized weight space of a different weight vanishes.
If K² v = ρ² v for a generalized weight vector v of weight ν ≠ -ρ, then K v = ρ v.
Some power of K - μ sends a nonzero generalized weight vector of weight μ to a nonzero
weight vector of weight μ.
A finite-dimensional module is the sum of its generalized weight spaces.
A surjective module map carries the generalized weight spaces of a finite-dimensional module onto the generalized weight spaces of its target. In particular, taking generalized weight spaces is exact on quotient modules.
At a generic parameter p, a sequence of vectors whose n-th term has generalized weight
(p²)ⁿ μ eventually vanishes: otherwise the finite spectrum of K would contain an infinite
geometric progression.
At a generic parameter, the raising string through any vector of a finite-dimensional module
terminates: E acts locally nilpotently.
At a generic parameter, the lowering string through any vector of a finite-dimensional
module terminates: F acts locally nilpotently.
At a generic parameter, the raising string through a nonzero vector of a finite-dimensional
module ends in a nonzero vector Eⁿ v killed by E. When v has weight μ, this is a
highest-weight vector of weight (q²)ⁿ μ.
Every nonzero finite-dimensional module at a generic parameter has a highest-weight
vector. No diagonalizability of K is assumed.
At a generic parameter, every nonzero generalized weight space of weight ν yields a nonzero
vector of weight (q²)ⁿ ν, for some n, killed by E.
At a generic parameter, every nonzero generalized weight vector w of weight μ in a
finite-dimensional module can be moved by an element of UqSl2 q to a nonzero highest-weight
vector, of weight q^(2n) μ for some n.
At a generic parameter, every nonzero generalized weight vector w of weight μ in a
finite-dimensional module can be moved by an element of UqSl2 q to a nonzero lowest-weight
vector, of weight q^(-2n) μ for some n.