Sym(V ⊕ ∧² V) isomorphic to direct sum of all Schur functors of V Let $V$ be a finite-dimensional $K$-vector space. Then, the symmetric power $\mathrm{Sym}\left(V\oplus \wedge^2 V\right)$ is isomorphic to the direct sum of all Schur functors applied to $V$ (each one time only) as a Schur functor.
This follows by comparison of characters using the so-called Schur identity
$\sum\limits_{\lambda\text{ is a partition}} s_{\lambda} = \prod\limits_i \left(1-\xi_i\right)^{-1} \cdot \prod\limits_{i < j} \left(1-\xi_i\xi_j\right)^{-1}$,
where $s_{\lambda}$ denote the Schur "polynomials" and $\xi_i$ are countably many indeterminates (see, for instance, chapter 5.4 in "M. Lothaire", Algebraic Combinatorics on Words). While it is easy to like the Schur identity, it is hard not to dislike the proof of the "strong" isomorphism $\mathrm{Sym}\left(V\oplus \wedge^2 V\right)\cong \bigoplus\limits_{\lambda\text{ is a partition}} \mathrm{Schur}_{\lambda}\left(V\right)$ using the "weak" identity for Schur polynomials. Is there any better argument known? Maybe even one yielding a canonical isomorphism?
 A: Here is how I think it should go. First
$\mathrm{Sym}\left(V\oplus \wedge^2 V\right)\cong \mathrm{Sym}\left(V\right)\otimes \mathrm{Sym}\left(\wedge^2 V\right)$
Then we have
$\mathrm{Sym}\left(\wedge^2 V\right)\cong \sum\limits_{\lambda} \mathrm{Schur}_{\lambda}\left(V\right)$
where the sum is over partitions such that all parts of the conjugate partition are even. This came up in 
Symmetric tensor products of irreducible representations
The tensor product $\mathrm{Sym}\left(V\right)\otimes \mathrm{Schur}_{\lambda}\left(V\right)$ is known by Pieri's rule.
Now given a partition we take a maximal subdiagram such that every column has an even number of boxes. The complement is skew shape with at most one box in each column.
Further comment In response to the request for representation theoretic proofs of the results used see 
MR1606831 (99b:20073)  Goodman, Roe ;  Wallach, Nolan R.  Representations and invariants of the classical groups.
Encyclopedia of Mathematics and its Applications, 68. Cambridge University Press, Cambridge,  1998. xvi+685 pp. ISBN: 0-521-58273-3; 0-521-66348-2 
In particular see 9.2.2 Reciprocity rules for Pieri's rule and see 5.2.6 to see the decomposition of $\mathrm{Sym}\left(\wedge^2 V\right)$. The highest weight vectors are constructed using Pfaffians.
A: Another way to think about it. It's equivalent to show that each dominant character of the Borel 
occurs with multiplicity one in the polynomial algebra on wedge-2(V) + V.
Now  multiplicity <= 1 because there is a Zariski dense orbit.
To see every one occurs:  write down explicit  polynomials
that correspond to fundamental weights (fun).
