Let be the standard Cartan element of the sl2 Lie algebra, with and . For a finite-dimensional representation, its formal character records its weight multiplicities:The classification of finite-dimensional sl2 representations and the Weyl complete reducibility theorem give , with finitely many nonzero . Each has weights , each of multiplicity one. ThereforeIn particular , and for one has . This proves parity unimodality of an sl2 character: within each parity, the coefficients increase towards zero and decrease away from zero. For a representation whose weights have a single parity, deleting the intervening zero coefficients gives a symmetric unimodal sequence.
The parity convention is necessary for the printed assertion. If unimodality means the full coefficient sequence at every consecutive integer exponent, it is false: the standard two-dimensional representation has character , whose coefficients at exponents are . The statement established above is unimodality on cosets of the root lattice for , and is the version needed in part ii. Infinite-dimensional representations need not even have Laurent-polynomial characters.
Assume with integers, as required for the quantum binomial expression. Let be the -dimensional irreducible sl2 Lie algebra representation, with one-dimensional weight spaces of weights , . The exterior-power Lie algebra representation on has characterThis is already a Laurent polynomial with nonnegative integer coefficients.
To identify it with the requested quotient, introduce and the Gaussian binomial coefficientSplitting the subsets according to whether is included provesThe product satisfies the same recurrence: after factoring common numerator and denominator terms, the needed identity is . Induction on therefore proves the product identity, including its polynomiality.
Since the quantum integer is , taking the quotient of the products givesThus this is the symmetric quantum binomial coefficient. All its weights have parity , because the exponent in the exterior-power sum differs from by an even integer. Applying part i to this finite-dimensional representation proves symmetric unimodality in steps of two. Equivalently, the ordinary polynomial has a unimodal coefficient sequence at consecutive powers of .
Again, the full integer-exponent coefficient sequence in , including the absent parity, need not be unimodal: for the answer is . This counterexample makes precise the convention under which the claimed quantum unimodality holds. The cases or give the constant one.
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