Tensor product of quadratic forms: Difference between revisions

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Template:Notability Template:One source In mathematics, the tensor product of quadratic forms is most easily understood when one views the quadratic forms as quadratic spaces.[1] If R is a commutative ring where 2 is invertible, and if (V1,q1) and (V2,q2) are two quadratic spaces over R, then their tensor product (V1V2,q1q2) is the quadratic space whose underlying R-module is the tensor product V1V2 of R-modules and whose quadratic form is the quadratic form associated to the tensor product of the bilinear forms associated to q1 and q2.

In particular, the form q1q2 satisfies

(q1q2)(v1v2)=q1(v1)q2(v2)v1V1, v2V2

(which does uniquely characterize it however). It follows from this that if the quadratic forms are diagonalizable (which is always possible if 2 is invertible in R), i.e.,

q1a1,...,an
q2b1,...,bm

then the tensor product has diagonalization

q1q2a1b1,a1b2,...a1bm,a2b1,...,a2bm,...,anb1,...anbm.

References

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