Antisymmetric subspace

The antisymmetric subspace $\mathcal{A}_p^d$ is the subspace of $(\mathbb{C}^d)^{\otimes p}$ of all vectors that are negated by odd permutations:

$\displaystyle \mathcal{A}_p^d \triangleq \big\{ \mathbf{v} \in (\mathbb{C}^d)^{\otimes p} : \mathbf{v} = (-1)^{{\rm sgn}(\sigma)}P_\sigma \mathbf{v} \ \ \forall \sigma \in S_p \big\},$

where $S_p$ is the symmetric group, ${\rm sgn}(\sigma)$ is the parity of the permutation $\sigma$, and $P_\sigma$ is the unitary operator that permutes the $p$ subsystems according to the permutation $\sigma$:

$\displaystyle P_\sigma(\mathbf{v}_1 \otimes \cdots \otimes \mathbf{v}_p) \triangleq \mathbf{v}_{\sigma(1)} \otimes \cdots \otimes \mathbf{v}_{\sigma(p)}$.

The antisymmetric subspace plays a role quite complementary to that of the symmetric subspace (and indeed, if $\mathcal{S}_p^d$ is the symmetric subspace then $\mathcal{A}_p^d \perp \mathcal{S}_p^d$).

Construction

The projection $P_{\mathcal{A}}$ onto the antisymmetric subspace can be constructed by averaging the signed permutation operators:

$\displaystyle P_{\mathcal{A}} = \frac{1}{p!}\sum_{\sigma \in S_p} (-1)^{{\rm sgn}(\sigma)}P_\sigma$.

In order to explicitly construct an orthonormal basis of the antisymmetric subspace, first fix an orthonormal basis $\{|i\rangle\}_{i=1}^d$ of $\mathbb{C}^d$. Now let $q$ be an increasing vector with $p$ entries containing distinct elements of $\{1, 2, \ldots, d\}$ as its entries. Then define

$\displaystyle \mathbf{v}_q \triangleq \frac{1}{\sqrt{p!}}\sum_{\sigma \in S_p} (-1)^{{\rm sgn}(\sigma)} P_\sigma (| q_1 \rangle \otimes \cdots \otimes | q_p \rangle)$.

It is then the case that $\{\mathbf{v}_q\}_q$ is an orthonormal basis of $\mathcal{A}_p^d$ if $q$ ranges over all $\binom{d}{p}$ possible increasing vectors with $p$ distinct entries chosen from $\{1, 2, \ldots, d\}$.

Facts

• The dimension of the antisymmetric subspace is $\binom{d}{p}$. It follows that the antisymmetric subspace only has nonzero dimension when d ≥ p. When p = 2, the dimension of the antisymmetric subspace is d(d-1)/2, from which it follows that the symmetric and antisymmetric subspaces span the whole space in this case (and this case only): $\mathcal{A}_2^d \oplus \mathcal{S}_2^d \cong \mathbb{C}^d \otimes \mathbb{C}^d$.

Related QETLAB functions

• AntisymmetricProjection: Produces the projection onto the antisymmetric subspace $P_{\mathcal{A}}$
• PermutationOperator: Produces a permutation operator $P_\sigma$

See also

• Symmetric subspace