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A hyperbolic plane is a two-dimensional vector space with a quadratic form and a basis $e,f$ satisfying $q(e)=q(f)=0$ and $B(e,f)=1$, where $B$ is the polar bilinear form of a quadratic form. Equivalently, $q(xe+yf)=xy$. This definition also applies in characteristic two. Over the real numbers, the identity $xy=((x+y)/2{)}^2-((x-y)/2{)}^2$ gives one positive and one negative square, hence signature zero. The signature statement is specific to real quadratic forms.

A quadratic form on a vector space over a field $F$ is a function $Q:V\to F$ satisfying $Q(av)=a^{2}Q(v)$ whose polar bilinear form of a quadratic form $B_Q(v,w)=Q(v+w)-Q(v)-Q(w)$ is a bilinear form. In finite dimension, it is represented in coordinates by a homogeneous degree-two polynomial, or by $Q(v)=v^{T}Av$ with a suitable matrix $A$.

When the characteristic is not two, one may choose $A$ to be a symmetric matrix and recover it from $B_Q/2$. In characteristic two, the symmetric-matrix restriction would lose examples: $Q(x,y)=xy$ has an upper-triangular representing matrix $\left(\begin{array}{cc}0& 1\\ 0& 0\end{array}\right)$, while $v^{T}Av$ for a symmetric matrix has no $xy$ cross term. Its polar form is $B_Q((x,y),(u,v))=xv+yu$, an alternating bilinear form. The distinction matters when studying quadratic forms over finite fields.^[ref]