A Schauder basis of a real Banach space is a sequence for which every has a unique norm-convergent expansion . Its basis projection is
and its basis constant is .
For the sequence space in the question, define
Convergence in the definition of makes well defined, and uniqueness of basis coefficients makes it a linear bijection. Moreover,
whereas
Thus is an isomorphism and, in particular, the displayed supremum really is a complete norm on .
The coordinate functional of a Schauder basis is
It is bounded because . On finite linear combinations of the , the nth partial-sum operator is the restriction of , since
The operators have norms at most , so the standard basis criterion shows that the dual sequence of a Schauder basis is a basic sequence in . For every and ,
which is precisely in the weak-star topology.
Suppose now that is a reflexive Banach space. If did not tend to zero, approximation by finite basis blocks would give a bounded block sequence and an such that . Reflexivity gives a weakly convergent subsequence. Every fixed coordinate functional is eventually zero on a block sequence, so its weak limit has every basis coordinate zero and is therefore zero. This contradicts . Hence in norm for every , so the basis is shrinking and is a basis of .
The converse fails. The standard basis of is shrinking because its dual sequence is the standard basis of , but is not reflexive.
Finally assume is a basis of . Map to
For ,
so . Conversely, if and , define
The limit exists: for ,
because is a basis. Also , so and . These two constructions are inverse and satisfy
Thus and are isomorphic.
Use the B2 root system convention
Thus is the five-dimensional vector representation of the Special orthogonal Lie algebra . Label its weight vertices
The crystal basis is the colored chain
because each Kashiwara operator subtracts .
For the tensor product of crystals, write for . The complete colored-arrow graph is compactly specified by
Its three connected highest-weight components start at , , and . Their vertex sets are
Their highest weights and dimensions identify the ten-vertex component with the exterior square and the other two with the symmetric square. Therefore
of dimensions and , respectively.
The module is the four-dimensional spin representation. Its weights are , and its crystal is
Every weight of lies in the root lattice, so every weight of every tensor power also lies in that lattice. But represents the nonzero coset in the quotient of the weight lattice by the root lattice. Consequently no irreducible constituent of can have highest weight , and never occurs.

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