A bivector is an element of the second exterior power . A simple bivector is one exterior product ; in real Euclidean space, it records the oriented area generated by those two vectors. A general bivector is a sum of such elements and need not describe just one plane. Covariant counterparts are differential two-forms, which take two vectors as inputs rather than belonging to .
In , choose
Expanding by bilinearity gives
The three coefficients are signed areas of the projections onto the , , and coordinate planes. They are three components of one bivector, not the three coordinates of either input vector.
Figure 1.
One bivector has three coordinate-plane area components in three dimensions
. Original parallelogram generated by and . The three planar panels show its projected signed areas , , and in the coordinate orders , , and . With the usual dot product, the full area is ; projected areas are components, so they are not added to obtain that area. Details.
With the usual dot product and a fixed orientation of a vector space, the cross product represents this area element by the normal vector . The order of the components matters: corresponds to , while corresponds to . The Gram determinant checks the full area:
Here the norm on bivectors is the one induced by the Euclidean inner product. The exterior product exists without that metric and in arbitrary dimension; the familiar cross product description relies on the additional three-dimensional geometry.
A simple bivector can be expressed as one exterior product of two vectors. Changing the pair need not change its area element: for every scalar , by bilinearity and . This operation shears the represented parallelogram while preserving its oriented area.
Every bivector in a real vector space of dimension at most three is simple, but this fails in dimension four. For an ordered basis , consider
The two components describe independent coordinate planes. Their square is
whereas because the factors repeat. Thus this cannot be one simple bivector. Over the real numbers in dimension four, the converse also holds: a nonzero bivector with is simple. The nonzero factor two is important; that criterion cannot be applied unchanged in characteristic two.

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A bivector is a geometric object that arises in the context of multivector algebra, particularly within the framework of geometric algebra. It represents an oriented area element and can be thought of as being associated with the plane spanned by two vectors in a vector space. In more formal terms, a bivector is defined as the exterior (or wedge) product of two vectors.