1 Introduction
In physics textbooks, we often come across the terms “pseudo-vector” and “pseudo-scalar.”
In fact, on a 3-dimensional manifold, a “pseudo-vector” is the exterior product of two tangent vectors, denoted as $v\in T_pM\wedge T_pM=\bigwedge^2(T_pM)$, while a “pseudo-scalar” is the exterior product of three tangent vectors, denoted as $s\in T_pM\wedge T_pM\wedge T_pM=\bigwedge^3(T_pM)$.
When equipped with an inner product (or non-degenerate bilinear form), there exists a Hodge duality between $\bigwedge^2(T_pM)$ and $\bigwedge^1(T_pM)$, which leads us to mistakenly consider the pseudo-vector as a vector. Similarly, due to the Hodge duality between $\bigwedge^3(T_pM)$ and $\bigwedge^0(T_pM)$ (scalar fields), we mistakenly treat the pseudo-scalar as a scalar.