Symmetric, Skew-symmetric and Alternating Forms
We define a form to be
- symmetric if B(v, w) = B(w, v) for all v, w in V;
- alternating if B(v, v) = 0 for all v in V;
- skew-symmetric if B(v, w) = −B(w, v) for all v, w in V;
Proposition: Every alternating form is skew-symmetric. Proof: this can be seen by expanding B(v+w, v+w).
If the characteristic of F is not 2 then the converse is also true: every skew-symmetric form is alternating. If, however, char(F) = 2 then a skew-symmetric form is the same as a symmetric form and there exist symmetric/skew-symmetric forms which are not alternating.
A bilinear form is symmetric (resp. skew-symmetric) if and only if its coordinate matrix (relative to any basis) is symmetric (resp. skew-symmetric). A bilinear form is alternating if and only if its coordinate matrix is skew-symmetric and the diagonal entries are all zero (which follows from skew-symmetry when char(F) ≠ 2).
A bilinear form is symmetric if and only if the maps B1, B2: V → V* are equal, and skew-symmetric if and only if they are negatives of one another. If char(F) ≠ 2 then one can decompose a bilinear form into a symmetric and a skew-symmetric part as follows
where B* is the transpose of B (defined above).
Also if char(F) ≠ 2 then one can define a quadratic form in terms of its associated symmetric form. One can likewise define quadratic forms corresponding to skew-symmetric forms, Hermitian forms, and skew-Hermitian forms; the general concept is ε-quadratic form.
Read more about this topic: Bilinear Form
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“When we speak the word life, it must be understood we are not referring to life as we know it from its surface of fact, but to that fragile, fluctuating center which forms never reach.”
—Antonin Artaud (18961948)