Given a free associative algebra $K \langle \mathtt{1}, \dots, \mathtt{d} \rangle$ over a field $K$, the signed volume tensor is $$\frac{1}{d!}\sum_{\sigma} (-1)^{\operatorname{sign}(\sigma)} \mathtt{\sigma(1)}\dots \mathtt{\sigma(d)}$$ where the sum is taken over all permutations of ${1, \dots, d}$. Under the isomorphism $\mathbb R \langle \mathtt{1}, \dots, \mathtt{d} \rangle \to T(\mathbb{R}^d), \ \mathtt{i} \mapsto e_i^*$ it corresponds to the determinant $e_1^* \wedge \dots \wedge e_d^*$.
This method computes the signed volume tensor of the given NCPolynomialRing. The output is in the same ring.
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The paper [1] explores under what conditions the value of the signature at the signed volume tensor computes the volume of the convex hull of a path. One instance where this is true is the case of canonical axis paths (see CAxisTensor). For example, for $\mathtt{d}=3$ the convex hull of the canonical axis path in $\mathbb{R}^{\mathtt{d}}$ is a tetrahedron, whose volume is $\frac{1}{6}$. We verify this.
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The object sgnVolTensor is a method function.
The source of this document is in PathSignatures/documentation.m2:918:0.